Sample records for additional negative charge

  1. Nanotribological Properties of Positively and Negatively charged nanodiamonds as additives to solutions

    NASA Astrophysics Data System (ADS)

    Liu, Zijian; Corley, Steven; Shenderova, Olga; Brenner, Donald; Krim, Jacqueline

    2013-03-01

    Nano-diamond (ND) particles are known to be beneficial for wear and friction reduction when used as additives in liquids, but the fundamental origins of the improvement in tribological properties has not been established. In order to explore this issue, we have investigated the nanotribological properties of ND coated with self-assembled monolayers (SAM) as additives to solutions, employing gold/chrome coated quartz crystal microbalances (QCM). Measurements were performed with the QCM initially immersed in deionized water. ND particles with positively and negatively charged SAM end groups were then added to the water, while the frequency and amplitude of the QCM were monitored. Negative shifts in both the QCM frequency and amplitude were observed when ND with positively charged SAM end groups were added, while positive shifts in both the QCM frequency and amplitude were observed when ND with negatively charged ND end groups were added. The results are consistent with a lubricating effect for the negatively charged ND, but were only observed for sufficiently small negative ND particle size. Experiments on QCM surfaces with differing textures and roughness are in progress, to determine the separate contributing effects of surface roughness charge-water interactions. Funding provided by NSF DMR.

  2. Thunderstorm Charge Structures Producing Negative Gigantic Jets

    NASA Astrophysics Data System (ADS)

    Boggs, L.; Liu, N.; Riousset, J. A.; Shi, F.; Rassoul, H.

    2016-12-01

    Here we present observational and modeling results that provide insight into thunderstorm charge structures that produce gigantic jet discharges. The observational results include data from four different thunderstorms producing 9 negative gigantic jets from 2010 to 2014. We used radar, very high frequency (VHF) and low frequency (LF) lightning data to analyze the storm characteristics, charge structures, and lightning activity when the gigantic jets emerged from the parent thunderstorms. A detailed investigation of the evolution of one of the charge structures by analyzing the VHF data is also presented. The newly found charge structure obtained from the observations was analyzed with fractal modeling and compared with previous fractal modeling studies [Krehbiel et al., Nat. Geosci., 1, 233-237, 2008; Riousset et al., JGR, 115, A00E10, 2010] of gigantic jet discharges. Our work finds that for normal polarity thunderstorms, gigantic jet charge structures feature a narrow upper positive charge region over a wide middle negative charge region. There also likely exists a `ring' of negative screening charge located around the perimeter of the upper positive charge. This is different from previously thought charge structures of the storms producing gigantic jets, which had a very wide upper positive charge region over a wide middle negative charge region, with a very small negative screening layer covering the cloud top. The newly found charge structure results in leader discharge trees in the fractal simulations that closely match the parent flashes of gigantic jets inside and outside the thundercloud. The previously used charge structures, while vital to the understanding of gigantic jet initiation and the role of charge imbalances inside the cloud, do not produce leader discharge trees that agree with observed gigantic jet discharges.Finally, the newly discovered gigantic jet charge structures are formed near the end of a convective pulse [Meyer et al., JGR, 118

  3. Is the negative glow plasma of a direct current glow discharge negatively charged?

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Bogdanov, E. A.; Saifutdinov, A. I.; Demidov, V. I., E-mail: Vladimir.Demidov@mail.wvu.edu

    A classic problem in gas discharge physics is discussed: what is the sign of charge density in the negative glow region of a glow discharge? It is shown that traditional interpretations in text-books on gas discharge physics that states a negative charge of the negative glow plasma are based on analogies with a simple one-dimensional model of discharge. Because the real glow discharges with a positive column are always two-dimensional, the transversal (radial) term in divergence with the electric field can provide a non-monotonic axial profile of charge density in the plasma, while maintaining a positive sign. The numerical calculationmore » of glow discharge is presented, showing a positive space charge in the negative glow under conditions, where a one-dimensional model of the discharge would predict a negative space charge.« less

  4. Recovery curves of the surface electric field after lightning discharges occurring between the positive charge pocket and negative charge centre in a thundercloud

    NASA Astrophysics Data System (ADS)

    Pawar, S. D.; Kamra, A. K.

    2002-12-01

    Surface observations of the electric field recovery curves of the lightning discharges occurring between the positive charge pocket and negative main charge centre in an overhead thundercloud are reported. Such recovery curves are observed to have an additional step of very slow field-change observed at an after-discharge value of electric field equal to 5-6 kV m-1. The behavior of recovery curves is explained in terms of the coronae charge and the relative efficiencies of the charge generating processes responsible for growth of positive charge pocket and main negative charge centre in the thundercloud. The charging currents responsible for the growth of charge in positive charge pockets is computed to be 2-4 times larger than that for the growth of the main negative charge. However, the charge destroyed in such a discharge is found to be comparable to that in a discharge between the main charge centres of the thundercloud.

  5. Enhancing biocompatibility of D-oligopeptide hydrogels by negative charges.

    PubMed

    Hyland, Laura L; Twomey, Julianne D; Vogel, Savannah; Hsieh, Adam H; Yu, Y Bruce

    2013-02-11

    Oligopeptide hydrogels are emerging as useful matrices for cell culture with commercial products on the market, but L-oligopeptides are labile to proteases. An obvious solution is to create D-oligopeptide hydrogels, which lack enzymatic recognition. However, D-oligopeptide matrices do not support cell growth as well as L-oligopeptide matrices. In addition to chiral interactions, many cellular activities are strongly governed by charge-charge interactions. In this work, the effects of chirality and charge on human mesenchymal stem cell (hMSC) behavior were studied using hydrogels assembled from oppositely charged oligopeptides. It was found that negative charges significantly improved hMSC viability and proliferation in D-oligopeptide gels but had little effect on their interactions with L-oligopeptide gels. This result points to the possibility of using charge and other factors to engineer biomaterials whose chirality is distinct from that of natural biomaterials, but whose performance is close to that of natural biomaterials.

  6. Devices that can identify positive vs. negative charge

    NASA Astrophysics Data System (ADS)

    Lincoln, James

    2017-10-01

    When your clothes come out of the dryer, covered with static, do you know whether they are positively or negatively charged? In this article, I discuss a variety of devices that can determine sign of the charge on an insulator or conductor. Purposefully, none of these methods utilize comparison with a known charge. Some of these ideas have been previously published, and I am extending them, but many are original. These demonstrations provide students and teachers with an opportunity to contrast the actual flow of charge with conventional current and to compare the behavior of positive and negative charges with what we expect from protons and electrons.

  7. Negative space charge effects in photon-enhanced thermionic emission solar converters

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Segev, G.; Weisman, D.; Rosenwaks, Y.

    2015-07-06

    In thermionic energy converters, electrons in the gap between electrodes form a negative space charge and inhibit the emission of additional electrons, causing a significant reduction in conversion efficiency. However, in Photon Enhanced Thermionic Emission (PETE) solar energy converters, electrons that are reflected by the electric field in the gap return to the cathode with energy above the conduction band minimum. These electrons first occupy the conduction band from which they can be reemitted. This form of electron recycling makes PETE converters less susceptible to negative space charge loss. While the negative space charge effect was studied extensively in thermionicmore » converters, modeling its effect in PETE converters does not account for important issues such as this form of electron recycling, nor the cathode thermal energy balance. Here, we investigate the space charge effect in PETE solar converters accounting for electron recycling, with full coupling of the cathode and gap models, and addressing conservation of both electric and thermal energy. The analysis shows that the negative space charge loss is lower than previously reported, allowing somewhat larger gaps compared to previous predictions. For a converter with a specific gap, there is an optimal solar flux concentration. The optimal solar flux concentration, the cathode temperature, and the efficiency all increase with smaller gaps. For example, for a gap of 3 μm the maximum efficiency is 38% and the optimal flux concentration is 628, while for a gap of 5 μm the maximum efficiency is 31% and optimal flux concentration is 163.« less

  8. Penetration and release studies of positively and negatively charged nanoemulsions--is there a benefit of the positive charge?

    PubMed

    Baspinar, Yücel; Borchert, Hans-Hubert

    2012-07-01

    The surface of all tissues, including the stratum corneum, carries a negative charge. Following that fact it is assumed that a positively charged topical formulation could lead to an enhanced penetration because of an increased interaction with the negative charge of the membrane. The intention of this study is to prove an enhanced penetration of a positively charged nanoemulsion compared to a negatively charged nanoemulsion, both containing prednicarbate. The release and penetration of these nanoemulsions, produced with the high pressure homogenization method, were investigated. Regarding these results reveals that the release of the negatively charged formulation is higher compared to the positively charged nanoemulsion, while the penetration of the positively charged nanoemulsion is enhanced compared to the negatively charged formulation. The results of the investigated positively charged nanoemulsion containing prednicarbate show that its topical use could be advantageous for the therapy of atopic dermatitis, especially regarding phytosphingosine, which was responsible for the positive charge. Copyright © 2012 Elsevier B.V. All rights reserved.

  9. Optimization of microelectrophoresis to select highly negatively charged sperm.

    PubMed

    Simon, Luke; Murphy, Kristin; Aston, Kenneth I; Emery, Benjamin R; Hotaling, James M; Carrell, Douglas T

    2016-06-01

    The sperm membrane undergoes extensive surface remodeling as it matures in the epididymis. During this process, the sperm is encapsulated in an extensive glycocalyx layer, which provides the membrane with its characteristic negative electrostatic charge. In this study, we develop a method of microelectrophoresis and standardize the protocol to isolate sperm with high negative membrane charge. Under an electric field, the percentage of positively charged sperm (PCS), negatively charged sperm (NCS), and neutrally charged sperm was determined for each ejaculate prior to and following density gradient centrifugation (DGC), and evaluated for sperm DNA damage, and histone retention. Subsequently, PCS, NCS, and neutrally charged sperm were selected using an ICSI needle and directly analyzed for DNA damage. When raw semen was analyzed using microelectrophoresis, 94 % were NCS. In contrast, DGC completely or partially stripped the negative membrane charge from sperm resulting PCS and neutrally charged sperm, while the charged sperm populations are increased with an increase in electrophoretic current. Following DGC, high sperm DNA damage and abnormal histone retention were inversely correlated with percentage NCS and directly correlated with percentage PCS. NCS exhibited significantly lower DNA damage when compared with control (P < 0.05) and PCS (P < 0.05). When the charged sperm population was corrected for neutrally charged sperm, sperm DNA damage was strongly associated with NCS at a lower electrophoretic current. The results suggest that selection of NCS at lower current may be an important biomarker to select healthy sperm for assisted reproductive treatment.

  10. Membrane Permeabilization Induced by Sphingosine: Effect of Negatively Charged Lipids

    PubMed Central

    Jiménez-Rojo, Noemi; Sot, Jesús; Viguera, Ana R.; Collado, M. Isabel; Torrecillas, Alejandro; Gómez-Fernández, J.C.; Goñi, Félix M.; Alonso, Alicia

    2014-01-01

    Sphingosine [(2S, 3R, 4E)-2-amino-4-octadecen-1, 3-diol] is the most common sphingoid long chain base in sphingolipids. It is the precursor of important cell signaling molecules, such as ceramides. In the last decade it has been shown to act itself as a potent metabolic signaling molecule, by activating a number of protein kinases. Moreover, sphingosine has been found to permeabilize phospholipid bilayers, giving rise to vesicle leakage. The present contribution intends to analyze the mechanism by which this bioactive lipid induces vesicle contents release, and the effect of negatively charged bilayers in the release process. Fluorescence lifetime measurements and confocal fluorescence microscopy have been applied to observe the mechanism of sphingosine efflux from large and giant unilamellar vesicles; a graded-release efflux has been detected. Additionally, stopped-flow measurements have shown that the rate of vesicle permeabilization increases with sphingosine concentration. Because at the physiological pH sphingosine has a net positive charge, its interaction with negatively charged phospholipids (e.g., bilayers containing phosphatidic acid together with sphingomyelins, phosphatidylethanolamine, and cholesterol) gives rise to a release of vesicular contents, faster than with electrically neutral bilayers. Furthermore, phosphorous 31-NMR and x-ray data show the capacity of sphingosine to facilitate the formation of nonbilayer (cubic phase) intermediates in negatively charged membranes. The data might explain the pathogenesis of Niemann-Pick type C1 disease. PMID:24940775

  11. Negative Ion CID Fragmentation of O-linked Oligosaccharide Aldoses—Charge Induced and Charge Remote Fragmentation

    NASA Astrophysics Data System (ADS)

    Doohan, Roisin A.; Hayes, Catherine A.; Harhen, Brendan; Karlsson, Niclas Göran

    2011-06-01

    Collision induced dissociation (CID) fragmentation was compared between reducing and reduced sulfated, sialylated, and neutral O-linked oligosaccharides. It was found that fragmentation of the [M - H]- ions of aldoses with acidic residues gave unique Z-fragmentation of the reducing end GalNAc containing the acidic C-6 branch, where the entire C-3 branch was lost. This fragmentation pathway, which is not seen in the alditols, showed that the process involved charge remote fragmentation catalyzed by a reducing end acidic anomeric proton. With structures containing sialic acid on both the C-3 and C-6 branch, the [M - H]- ions were dominated by the loss of sialic acid. This fragmentation pathway was also pronounced in the [M - 2H]2- ions revealing both the C-6 Z-fragment plus its complementary C-3 C-fragment in addition to glycosidic and cross ring fragmentation. This generation of the Z/C-fragment pairs from GalNAc showed that the charges were not participating in their generation. Fragmentation of neutral aldoses showed pronounced Z-fragmentation believed to be generated by proton migration from the C-6 branch to the negatively charged GalNAc residue followed by charge remote fragmentation similar to the acidic oligosaccharides. In addition, A-type fragments generated by charge induced fragmentation of neutral oligosaccharides were observed when the charge migrated from C-1 of the GalNAc to the GlcNAc residue followed by rearrangement to accommodate the 0,2A-fragmentation. LC-MS also showed that O-linked aldoses existed as interchangeable α/β pyranose anomers, in addition to a third isomer (25% of the total free aldose) believed to be the furanose form.

  12. Charging of dust grains in a plasma with negative ions

    NASA Astrophysics Data System (ADS)

    Kim, Su-Hyun; Merlino, Robert L.

    2006-05-01

    The effect of negative ions on the charging of dust particles in a plasma is investigated experimentally. A plasma containing a very low percentage of electrons is formed in a single-ended SF6 is admitted into the vacuum system. The relatively cold (Te≈0.2eV ) readily attach to SF6 molecules to form SF6- negative ions. Calculations of the dust charge indicate that for electrons, negative ions, and positive ions of comparable temperatures, the charge (or surface potential) of the dust can be positive if the positive ion mass is smaller than the negative ion mass and if ɛ, the ratio of the electron to positive ion density, is sufficiently small. The K+ positive ions (mass 39amu) and SF6- negative ions (mass 146amu), and also utilizes a rotating cylinder to dispense dust into the plasma column. Analysis of the current-voltage characteristics of a Langmuir probe in the dusty plasma shows evidence for the reduction in the (magnitude) of the negative dust charge and the transition to positively charged dust as the relative concentration of the residual electrons is reduced. Some remarks are offered concerning experiments that could become possible in a dusty plasma with positive grains.

  13. Electrostatic Power Generation from Negatively Charged, Simulated Lunar Regolith

    NASA Technical Reports Server (NTRS)

    Choi, Sang H.; King, Glen C.; Kim, Hyun-Jung; Park, Yeonjoon

    2010-01-01

    Research was conducted to develop an electrostatic power generator for future lunar missions that facilitate the utilization of lunar resources. The lunar surface is known to be negatively charged from the constant bombardment of electrons and protons from the solar wind. The resulting negative electrostatic charge on the dust particles, in the lunar vacuum, causes them to repel each other minimizing the potential. The result is a layer of suspended dust about one meter above the lunar surface. This phenomenon was observed by both Clementine and Surveyor spacecrafts. During the Apollo 17 lunar landing, the charged dust was a major hindrance, as it was attracted to the astronauts' spacesuits, equipment, and the lunar buggies. The dust accumulated on the spacesuits caused reduced visibility for the astronauts, and was unavoidably transported inside the spacecraft where it caused breathing irritation [1]. In the lunar vacuum, the maximum charge on the particles can be extremely high. An article in the journal "Nature", titled "Moon too static for astronauts?" (Feb 2, 2007) estimates that the lunar surface is charged with up to several thousand volts [2]. The electrostatic power generator was devised to alleviate the hazardous effects of negatively charged lunar soil by neutralizing the charged particles through capacitive coupling and thereby simultaneously harnessing power through electric charging [3]. The amount of power generated or collected is dependent on the areal coverage of the device and hovering speed over the lunar soil surface. A thin-film array of capacitors can be continuously charged and sequentially discharged using a time-differentiated trigger discharge process to produce a pulse train of discharge for DC mode output. By controlling the pulse interval, the DC mode power can be modulated for powering devices and equipment. In conjunction with a power storage system, the electrostatic power generator can be a power source for a lunar rover or other

  14. An in situ generated carbon as integrated conductive additive for hierarchical negative plate of lead-acid battery

    NASA Astrophysics Data System (ADS)

    Saravanan, M.; Ganesan, M.; Ambalavanan, S.

    2014-04-01

    In this work, we report an in situ generated carbon from sugar as additive in the Negative Active Mass (NAM) which enhances the charge-discharge characteristics of the lead-acid cells. In situ formed sugar derived carbon (SDC) with leady oxide (LO) provides a conductive network and excellent protection against NAM irreversible lead sulfation. The effect of SDC and carbon black (CB) added negative plates are characterized by X-ray diffraction (XRD), Raman spectroscopy, scanning electron microscopy (SEM), galvanostatic charge-discharge, cyclic voltammetry (CV) and electrochemical impedance spectroscopy (EIS), respectively. The results show that subtle changes in the addition of carbon to NAM led to subsequent changes on the performance during partial-state-of-charge (PSoC) operations in lead-acid cells. Furthermore, SDC added cells exhibit remarkable improvement in the rate capability, active material utilization, cycle performance and charge acceptance compared to that of the conventional CB added cells. The impact of SDC with LO at various synthesis conditions on the electrochemical performance of the negative plate is studied systematically.

  15. Electrostatic plasma lens for focusing negatively charged particle beams.

    PubMed

    Goncharov, A A; Dobrovolskiy, A M; Dunets, S M; Litovko, I V; Gushenets, V I; Oks, E M

    2012-02-01

    We describe the current status of ongoing research and development of the electrostatic plasma lens for focusing and manipulating intense negatively charged particle beams, electrons, and negative ions. The physical principle of this kind of plasma lens is based on magnetic isolation electrons providing creation of a dynamical positive space charge cloud in shortly restricted volume propagating beam. Here, the new results of experimental investigations and computer simulations of wide-aperture, intense electron beam focusing by plasma lens with positive space charge cloud produced due to the cylindrical anode layer accelerator creating a positive ion stream towards an axis system is presented.

  16. Coarse-grained modeling of proline rich protein 1 (PRP-1) in bulk solution and adsorbed to a negatively charged surface.

    PubMed

    Skepö, Marie; Linse, Per; Arnebrant, Thomas

    2006-06-22

    Structural properties of the acidic proline rich protein PRP-1 of salivary origin in bulk solution and adsorbed onto a negatively charged surface have been studied by Monte Carlo simulations. A simple model system with focus on electrostatic interactions and short-ranged attractions among the uncharged amino acids has been used. In addition to PRP-1, some mutants were considered to assess the role of the interactions in the systems. Contrary to polyelectrolytes, the protein has a compact structure in salt-free bulk solutions, whereas at high salt concentration the protein becomes more extended. The protein adsorbs to a negatively charged surface, although its net charge is negative. The adsorbed protein displays an extended structure, which becomes more compact upon addition of salt. Hence, the conformational response upon salt addition in the adsorbed state is the opposite as compared to that in bulk solution. The conformational behavior of PRP-1 in bulk solution and at charged surfaces as well as its propensity to adsorb to surfaces with the same net charge are rationalized by the block polyampholytic character of the protein. The presence of a triad of positively charged amino acids in the C-terminal was found to be important for the adsorption of the protein.

  17. Charge mobility retrieval approach from apparent charge packet movements based on the negative differential resistance theory.

    PubMed

    Meng, Jia; Zhang, Yewen; Holé, Stéphane; Zheng, Feihu; An, Zhenlian

    2018-04-12

    Space charge migration characteristics play an important role in the evaluation of polymer insulation performance. However, an accurate description of charge carrier mobility in several typical insulating polymers such as polyethylene, polypropylene is currently not available. Recently, with the observation of a series of negative charge packet movements associated with the negative differential resistance characteristic of charge mobility in LDPE films, the extraction of charge mobility from the apparent charge packet movement has been attempted using appropriate methods. Based on the previous report of the successful derivation of charge mobility from experimental results using numerical methods, the present research improves the derivation accuracy and describes the details of the charge mobility derivation procedure. Back simulation results under several typical polarizing fields using the derived charge mobility are exhibited. The results indicate that both the NDR theory and the simulation models for the polyethylene materials are reasonable. A significant migration velocity difference between the charge carrier and the charge packet is observed. Back simulations of the charge packet under several typical polarizing fields using the obtained E-v curve show good agreement with the experimental results. The charge packet shapes during the migrations were also found to vary with the polarizing field.

  18. Negative differential mobility for negative carriers as revealed by space charge measurements on crosslinked polyethylene insulated model cables

    NASA Astrophysics Data System (ADS)

    Teyssedre, G.; Vu, T. T. N.; Laurent, C.

    2015-12-01

    Among features observed in polyethylene materials under relatively high field, space charge packets, consisting in a pulse of net charge that remains in the form of a pulse as it crosses the insulation, are repeatedly observed but without complete theory explaining their formation and propagation. Positive charge packets are more often reported, and the models based on negative differential mobility(NDM) for the transport of holes could account for some charge packets phenomenology. Conversely, NDM for electrons transport has never been reported so far. The present contribution reports space charge measurements by pulsed electroacoustic method on miniature cables that are model of HVDC cables. The measurements were realized at room temperature or with a temperature gradient of 10 °C through the insulation under DC fields on the order 30-60 kV/mm. Space charge results reveal systematic occurrence of a negative front of charges generated at the inner electrode that moves toward the outer electrode at the beginning of the polarization step. It is observed that the transit time of the front of negative charge increases, and therefore the mobility decreases, with the applied voltage. Further, the estimated mobility, in the range 10-14-10-13 m2 V-1 s-1 for the present results, increases when the temperature increases for the same condition of applied voltage. The features substantiate the hypothesis of negative differential mobility used for modelling space charge packets.

  19. An analysis of five negative sprite-parent discharges and their associated thunderstorm charge structures

    NASA Astrophysics Data System (ADS)

    Boggs, Levi D.; Liu, Ningyu; Splitt, Michael; Lazarus, Steven; Glenn, Chad; Rassoul, Hamid; Cummer, Steven A.

    2016-01-01

    In this study we analyze the discharge morphologies of five confirmed negative sprite-parent discharges and the associated charge structures of the thunderstorms that produced them. The negative sprite-parent lightning took place in two thunderstorms that were associated with a tropical disturbance in east central and south Florida. The first thunderstorm, which moved onshore in east central Florida, produced four of the five negative sprite-parent discharges within a period of 17 min, as it made landfall from the Atlantic Ocean. These negative sprite-parents were composed of bolt-from-the-blue (BFB), hybrid intracloud-negative cloud-to-ground (IC-NCG), and multicell IC-NCGs discharges. The second thunderstorm, which occurred inland over south Florida, produced a negative sprite-parent that was a probable hybrid IC-NCG discharge and two negative gigantic jets (GJs). Weakened upper positive charge with very large midlevel negative charge was inferred for both convective cells that initiated the negative-sprite-parent discharges. Our study suggests tall, intense convective systems with high wind shear at the middle to upper regions of the cloud accompanied by low cloud-to-ground (CG) flash rates promote these charge structures. The excess amount of midlevel negative charge results in these CG discharges transferring much more charge to ground than typical negative CG discharges. We find that BFB discharges prefer an asymmetrical charge structure that brings the negative leader exiting the upper positive charge region closer to the lateral positive screening charge layer. This may be the main factor in determining whether a negative leader exiting the upper positive region of the thundercloud forms a BFB or GJ.

  20. Bactericidal action mechanism of negatively charged food grade clove oil nanoemulsions.

    PubMed

    Majeed, Hamid; Liu, Fei; Hategekimana, Joseph; Sharif, Hafiz Rizwan; Qi, Jing; Ali, Barkat; Bian, Yuan-Yuan; Ma, Jianguo; Yokoyama, Wallace; Zhong, Fang

    2016-04-15

    Clove oil (CO) anionic nanoemulsions were prepared with varying ratios of CO to canola oil (CA), emulsified and stabilized with purity gum ultra (PGU), a newly developed succinylated waxy maize starch. Interfacial tension measurements showed that CO acted as a co-surfactant and there was a gradual decrease in interfacial tension which favored the formation of small droplet sizes on homogenization until a critical limit (5:5% v/v CO:CA) was reached. Antimicrobial activity of the negatively charged CO nanoemulsion was determined against Gram positive GPB (Listeria monocytogenes and Staphylococcus aureus) and Gram negative GNB (Escherichia coli) bacterial strains using minimum inhibitory concentration (MIC) and a time kill dynamic method. Negatively charged PGU emulsified CO nanoemulsion showed prolonged antibacterial activities against Gram positive bacterial strains. We concluded that negatively charged CO nanoemulsion droplets self-assemble with GPB cell membrane, and facilitated interaction with cellular components of bacteria. Moreover, no electrostatic interaction existed between negatively charged droplets and the GPB membrane. Copyright © 2015 Elsevier Ltd. All rights reserved.

  1. Negative differential mobility for negative carriers as revealed by space charge measurements on crosslinked polyethylene insulated model cables

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Teyssedre, G., E-mail: gilbert.teyssedre@laplace.univ-tlse.fr; Laurent, C.; CNRS, LAPLACE, F-31062 Toulouse

    Among features observed in polyethylene materials under relatively high field, space charge packets, consisting in a pulse of net charge that remains in the form of a pulse as it crosses the insulation, are repeatedly observed but without complete theory explaining their formation and propagation. Positive charge packets are more often reported, and the models based on negative differential mobility(NDM) for the transport of holes could account for some charge packets phenomenology. Conversely, NDM for electrons transport has never been reported so far. The present contribution reports space charge measurements by pulsed electroacoustic method on miniature cables that are modelmore » of HVDC cables. The measurements were realized at room temperature or with a temperature gradient of 10 °C through the insulation under DC fields on the order 30–60 kV/mm. Space charge results reveal systematic occurrence of a negative front of charges generated at the inner electrode that moves toward the outer electrode at the beginning of the polarization step. It is observed that the transit time of the front of negative charge increases, and therefore the mobility decreases, with the applied voltage. Further, the estimated mobility, in the range 10{sup −14}–10{sup −13} m{sup 2} V{sup −1} s{sup −1} for the present results, increases when the temperature increases for the same condition of applied voltage. The features substantiate the hypothesis of negative differential mobility used for modelling space charge packets.« less

  2. Aberration of a negative ion beam caused by space charge effect.

    PubMed

    Miyamoto, K; Wada, S; Hatayama, A

    2010-02-01

    Aberrations are inevitable when the charged particle beams are extracted, accelerated, transmitted, and focused with electrostatic and magnetic fields. In this study, we investigate the aberration of a negative ion accelerator for a neutral beam injector theoretically, especially the spherical aberration caused by the negative ion beam expansion due to the space charge effect. The negative ion current density profiles with the spherical aberration are compared with those without the spherical aberration. It is found that the negative ion current density profiles in a log scale are tailed due to the spherical aberration.

  3. Positive zeta potential of a negatively charged semi-permeable plasma membrane

    NASA Astrophysics Data System (ADS)

    Sinha, Shayandev; Jing, Haoyuan; Das, Siddhartha

    2017-08-01

    The negative charge of the plasma membrane (PM) severely affects the nature of moieties that may enter or leave the cells and controls a large number of ion-interaction-mediated intracellular and extracellular events. In this letter, we report our discovery of a most fascinating scenario, where one interface (e.g., membrane-cytosol interface) of the negatively charged PM shows a positive surface (or ζ) potential, while the other interface (e.g., membrane-electrolyte interface) still shows a negative ζ potential. Therefore, we encounter a completely unexpected situation where an interface (e.g., membrane-cytosol interface) that has a negative surface charge density demonstrates a positive ζ potential. We establish that the attainment of such a property by the membrane can be ascribed to an interplay of the nature of the membrane semi-permeability and the electrostatics of the electric double layer established on either side of the charged membrane. We anticipate that such a membrane property can lead to such capabilities of the cell (in terms of accepting or releasing certain kinds of moieties as well regulating cellular signaling) that was hitherto inconceivable.

  4. Production of negatively charged radioactive ion beams

    DOE PAGES

    Liu, Y.; Stracener, D. W.; Stora, T.

    2017-02-15

    Beams of short-lived radioactive nuclei are needed for frontier experimental research in nuclear structure, reactions, and astrophysics. Negatively charged radioactive ion beams have unique advantages and allow for the use of a tandem accelerator for post-acceleration, which can provide the highest beam quality and continuously variable energies. Negative ion beams can be obtained with high intensity and some unique beam purification techniques based on differences in electronegativity and chemical reactivity can be used to provide beams with high purity. This article describes the production of negative radioactive ion beams at the former holifield radioactive ion beam facility at Oak Ridgemore » National Laboratory and at the CERN ISOLDE facility with emphasis on the development of the negative ion sources employed at these two facilities.« less

  5. Positively versus negatively charged moral emotion expectancies in adolescence: the role of situational context and the developing moral self.

    PubMed

    Krettenauer, Tobias; Johnston, Megan

    2011-09-01

    The study analyses adolescents' positively charged versus negatively charged moral emotion expectancies. Two hundred and five students (M= 14.83 years, SD= 2.21) participated in an interview depicting various situations in which a moral norm was either regarded or transgressed. Emotion expectancies were assessed for specific emotions (pride, guilt) as well as for overall strength and valence. In addition, self-importance of moral values was measured by a questionnaire. Results revealed that positively charged emotion expectancies were more pronounced in contexts of prosocial action than in the context of moral transgressions, whereas the opposite was true for negatively charged emotions. At the same time, expectations of guilt and pride were substantially related to the self-importance of moral values. ©2010 The British Psychological Society.

  6. The Role of Hydrophobicity in the Cellular Uptake of Negatively Charged Macromolecules.

    PubMed

    Abou Matar, Tamara; Karam, Pierre

    2018-02-01

    It is generally accepted that positively charged molecules are the gold standard to by-pass the negatively charged cell membrane. Here, it is shown that cellular uptake is also possible for polymers with negatively charged side chains and hydrophobic backbones. Specifically, poly[5-methoxy-2-(3-sulfopropoxy)-1,4-phenylenevinylene], a conjugated polyelectrolyte with sulfonate, as water-soluble functional groups, is shown to accumulate in the intracellular region. When the polymer hydrophobic backbone is dissolved using polyvinylpyrrolidone, an amphiphilic macromolecule, the cellular uptake is dramatically reduced. The report sheds light on the fine balance between negatively charged side groups and the hydrophobicity of polymers to either enhance or reduce cellular uptake. As a result, these findings will have important ramifications on the future design of targeted cellular delivery nanocarriers for imaging and therapeutic applications. © 2017 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim.

  7. Polymerization on the rocks: negatively-charged alpha-amino acids

    NASA Technical Reports Server (NTRS)

    Hill, A. R. Jr; Bohler, C.; Orgel, L. E.; Bada, J. L. (Principal Investigator)

    1998-01-01

    Oligomers of the negatively-charged amino acids, glutamic acid, aspartic acid, and O-phospho-L-serine are adsorbed by hydroxylapatite and illite with affinities that increase with oligomer length. In the case of oligo-glutamic acids adsorbed on hydroxylapatite, addition of an extra residue results in an approximately four-fold increase in the strength of adsorption. Oligomers much longer than the 7-mer are retained tenaciously by the mineral. Repeated incubation of short oligo-glutamic acids adsorbed on hydroxylapatite or illite with activated monomer leads to the accumulation of oligomers at least 45 units long. The corresponding reactions of aspartic acid and O-phospho-L-serine on hydroxylapatite are less effective in generating long oligomers, while illite fails to accumulate substantial amounts of long oligomers of aspartic acid or of O-phospho-L-serine.

  8. Cationic cell-penetrating peptide binds to planar lipid bilayers containing negatively charged lipids but does not induce conductive pores.

    PubMed

    Gurnev, Philip A; Yang, Sung-Tae; Melikov, Kamran C; Chernomordik, Leonid V; Bezrukov, Sergey M

    2013-05-07

    Using a cation-selective gramicidin A channel as a sensor of the membrane surface charge, we studied interactions of oligoarginine peptide R9C, a prototype cationic cell-penetrating peptide (CPP), with planar lipid membranes. We have found that R9C sorption to the membrane depends strongly on its lipid composition from virtually nonexistent for membranes made of uncharged lipids to very pronounced for membranes containing negatively charged lipids, with charge overcompensation at R9C concentrations exceeding 1 μM. The sorption was reversible as it was removed by addition of polyanionic dextran sulfate to the membrane bathing solution. No membrane poration activity of R9C (as would be manifested by increased bilayer conductance) was detected in the charged or neutral membranes, including those with asymmetric negative/neutral and negative/positive lipid leaflets. We conclude that interaction of R9C with planar lipid bilayers does not involve pore formation in all studied lipid combinations up to 20 μM peptide concentration. However, R9C induces leakage of negatively charged but not neutral liposomes in a process that involves lipid mixing between liposomes. Our findings suggest that direct traversing of CPPs through the uncharged outer leaflet of the plasma membrane bilayer is unlikely and that permeabilization necessarily involves both anionic lipids and CPP-dependent fusion between opposing membranes. Copyright © 2013 Biophysical Society. Published by Elsevier Inc. All rights reserved.

  9. Comparing Positively and Negatively Charged Distonic Radical Ions in Phenylperoxyl Forming Reactions.

    PubMed

    Williams, Peggy E; Marshall, David L; Poad, Berwyck L J; Narreddula, Venkateswara R; Kirk, Benjamin B; Trevitt, Adam J; Blanksby, Stephen J

    2018-06-04

    In the gas phase, arylperoxyl forming reactions play a significant role in low-temperature combustion and atmospheric processing of volatile organic compounds. We have previously demonstrated the application of charge-tagged phenyl radicals to explore the outcomes of these reactions using ion trap mass spectrometry. Here, we present a side-by-side comparison of rates and product distributions from the reaction of positively and negatively charge tagged phenyl radicals with dioxygen. The negatively charged distonic radical ions are found to react with significantly greater efficiency than their positively charged analogues. The product distributions of the anion reactions favor products of phenylperoxyl radical decomposition (e.g., phenoxyl radicals and cyclopentadienone), while the comparable fixed-charge cations yield the stabilized phenylperoxyl radical. Electronic structure calculations rationalize these differences as arising from the influence of the charged moiety on the energetics of rate-determining transition states and reaction intermediates within the phenylperoxyl reaction manifold and predict that this influence could extend to intra-molecular charge-radical separations of up to 14.5 Å. Experimental observations of reactions of the novel 4-(1-carboxylatoadamantyl)phenyl radical anion confirm that the influence of the charge on both rate and product distribution can be modulated by increasing the rigidly imposed separation between charge and radical sites. These findings provide a generalizable framework for predicting the influence of charged groups on polarizable radicals in gas phase distonic radical ions. Graphical Abstract.

  10. Comparing Positively and Negatively Charged Distonic Radical Ions in Phenylperoxyl Forming Reactions

    NASA Astrophysics Data System (ADS)

    Williams, Peggy E.; Marshall, David L.; Poad, Berwyck L. J.; Narreddula, Venkateswara R.; Kirk, Benjamin B.; Trevitt, Adam J.; Blanksby, Stephen J.

    2018-06-01

    In the gas phase, arylperoxyl forming reactions play a significant role in low-temperature combustion and atmospheric processing of volatile organic compounds. We have previously demonstrated the application of charge-tagged phenyl radicals to explore the outcomes of these reactions using ion trap mass spectrometry. Here, we present a side-by-side comparison of rates and product distributions from the reaction of positively and negatively charge tagged phenyl radicals with dioxygen. The negatively charged distonic radical ions are found to react with significantly greater efficiency than their positively charged analogues. The product distributions of the anion reactions favor products of phenylperoxyl radical decomposition (e.g., phenoxyl radicals and cyclopentadienone), while the comparable fixed-charge cations yield the stabilized phenylperoxyl radical. Electronic structure calculations rationalize these differences as arising from the influence of the charged moiety on the energetics of rate-determining transition states and reaction intermediates within the phenylperoxyl reaction manifold and predict that this influence could extend to intra-molecular charge-radical separations of up to 14.5 Å. Experimental observations of reactions of the novel 4-(1-carboxylatoadamantyl)phenyl radical anion confirm that the influence of the charge on both rate and product distribution can be modulated by increasing the rigidly imposed separation between charge and radical sites. These findings provide a generalizable framework for predicting the influence of charged groups on polarizable radicals in gas phase distonic radical ions.

  11. Recombination energy for negatively charged excitons inside type-II core/shell spherical quantum dots

    NASA Astrophysics Data System (ADS)

    Chafai, A.; Essaoudi, I.; Ainane, A.; Dujardin, F.; Ahuja, R.

    2018-07-01

    The recombination energy of isolated neutral exciton and that of isolated negatively charged exciton inside a type-II core/shell spherical quantum dot are studied. Our investigation considers the charge-carriers effective mass discontinuity at the surface contact between the core and shell materials. Although our model omits the effect of the surface polarization, the dielectric-constant mismatch at the nanodot boundaries was taken into account. In order to achieve the exciton and negative trion energies, we proceed by a variational calculation in the framework of the envelope approximation. Our results reveal a strong correlation between the nanodot morphology and the energy spectrum of the neutral and negatively charged exciton.

  12. Presence of negative charge on the basal planes of New York talc.

    PubMed

    Burdukova, E; Becker, M; Bradshaw, D J; Laskowski, J S

    2007-11-01

    Potentiometric titration measurements as well as rheological measurements of talc aqueous suspensions indicate that the behavior of the New York talc particles is consistent with the presence of a negative charge on their basal planes. The possibility of the presence of a negative electrical charge on the basal planes of talc particles is analyzed in this paper. Samples of New York talc were studied using electron microprobe analysis and dehydration techniques and the exact chemical formula of New York talc was determined. It was found that there exists a deficiency of protons in the tetrahedral layers of talc, resulting from substitution of Si(4+) ions with Al(3+) and Ti(3+) ions. The comparison of the level of substitution of Si(4+) ions with ions of a lower valency was found to be of a similar order of magnitude as that found in other talc deposits. This strongly points to the presence of a negative charge on the talc basal planes.

  13. Negative charge emission due to excimer laser bombardment of sodium trisilicate glass

    NASA Astrophysics Data System (ADS)

    Langford, S. C.; Jensen, L. C.; Dickinson, J. T.; Pederson, L. R.

    1990-10-01

    We describe measurements of negative charge emission accompanying irradiation of sodium trisilicate glass (Na2Oṡ3SiO2) with 248-nm excimer laser light at fluences on the order of 2 J/cm2 per pulse, i.e., at the threshold for ablative etching of the glass surface. The negative charge emission consists of a very prompt photoelectron burst coincident with the laser pulse, followed by a much slower plume of electrons and negative ions traveling with a high density cloud of positive ions, previously identified as primarily Na+. Using combinations of E and B fields in conjunction with time-of-flight methods, the negative ions were successfully separated from the plume and tentatively identified as O-, Si-, NaO-, and perhaps NaSi-. These negative species are probably formed by gas phase collisions in the near-surface region which result in electron attachment.

  14. Negative charge emission due to excimer laser bombardment of sodium trisilicate glass

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Langford, S.C.; Jensen, L.C.; Dickinson, J.T.

    We describe measurements of negative charge emission accompanying irradiation of sodium trisilicate glass (Na{sub 2}O{center dot}3SiO{sub 2}) with 248-nm excimer laser light at fluences on the order of 2 J/cm{sup 2} per pulse, i.e., at the threshold for ablative etching of the glass surface. The negative charge emission consists of a very prompt photoelectron burst coincident with the laser pulse, followed by a much slower plume of electrons and negative ions traveling with a high density cloud of positive ions, previously identified as primarily Na{sup +}. Using combinations of {bold E} and {bold B} fields in conjunction with time-of-flight methods,more » the negative ions were successfully separated from the plume and tentatively identified as O{sup {minus}}, Si{sup {minus}}, NaO{sup {minus}}, and perhaps NaSi{sup {minus}}. These negative species are probably formed by gas phase collisions in the near-surface region which result in electron attachment.« less

  15. Frequency-Dependent Capacitance of Hydrophobic Membranes Containing Fixed Negative Charges

    PubMed Central

    Ilani, Asher

    1968-01-01

    Filters containing fixed negative charges were saturated with hydrophobic solvent and interposed between aqueous solutions. The capacitance of such membranes was measured in the frequency range of 0.05-30 kc. The capacitance increased with decrease in frequency. The frequency dependence of the capacitance was sensitive to nature of the cation present and to salt concentration in the aqueous solution. It is suggested that variation of membrane resistivity in the space charge region of the membrane is responsible for this phenomenon. Possible effects of the potential and counterion concentration profiles at the membrane-water interface are discussed. PMID:5699796

  16. Differential effects of DEAE negative mode chromatography and gel-filtration chromatography on the charge status of Helicobacter pylori neutrophil-activating protein

    PubMed Central

    Pan, Timothy; Tzeng, Huey-Fen

    2017-01-01

    Helicobacter pylori neutrophil-activating protein (HP-NAP) is involved in H. pylori-associated gastric inflammation. HP-NAP is also a vaccine candidate, a possible drug target, and a potential diagnostic marker for H. pylori-associated diseases. Previously, we purified recombinant HP-NAP by one-step diethylaminoethyl (DEAE) negative mode chromatography by collecting the unbound fraction at pH 8.0 at 4°C. It remains unclear why HP-NAP does not bind to DEAE resins at the pH above its isoelectric point during the purification. To investigate how pH affects the surface net charge of HP-NAP and its binding to DEAE resins during the purification, recombinant HP-NAP expressed in Escherichia coli was subjected to DEAE negative mode chromatography at pH ranging from 7.0 to 9.0 at 25°C and the surface charge of purified HP-NAP was determined by capillary electrophoresis. A minimal amount of HP-NAP was detected in the elution fraction of DEAE Sepharose resin at pH 8.5, whereas recombinant HP-NAP was detected in the elution fraction of DEAE Sephadex resin only at pH 7.0 and 8.0. The purified recombinant HP-NAP obtained from the unbound fractions was not able to bind to DEAE resins at pH 7.0 to 9.0. In addition, the surface charge of the purified HP-NAP was neutral at pH 7.0 to 8.0 and was either neutral or slightly negative at pH 8.5 and 9.0. However, recombinant HP-NAP purified from gel-filtration chromatography was able to bind to DEAE Sepharose resin at pH 7.0 to 9.0 and DEAE Sephadex resin at pH 7.0. At pH 8.5 and 9.0, only the negatively charged species of HP-NAP were found. Thus, recombinant HP-NAP with different charge status can be differentially purified by DEAE negative mode chromatography and gel-filtration chromatography. Furthermore, the charge distribution on the surface of HP-NAP, the presence of impure proteins, and the overall net charge of the resins all affect the binding of HP-NAP to DEAE resins during the negative purification. PMID:28328957

  17. Differential effects of DEAE negative mode chromatography and gel-filtration chromatography on the charge status of Helicobacter pylori neutrophil-activating protein.

    PubMed

    Hong, Zhi-Wei; Yang, Yu-Chi; Pan, Timothy; Tzeng, Huey-Fen; Fu, Hua-Wen

    2017-01-01

    Helicobacter pylori neutrophil-activating protein (HP-NAP) is involved in H. pylori-associated gastric inflammation. HP-NAP is also a vaccine candidate, a possible drug target, and a potential diagnostic marker for H. pylori-associated diseases. Previously, we purified recombinant HP-NAP by one-step diethylaminoethyl (DEAE) negative mode chromatography by collecting the unbound fraction at pH 8.0 at 4°C. It remains unclear why HP-NAP does not bind to DEAE resins at the pH above its isoelectric point during the purification. To investigate how pH affects the surface net charge of HP-NAP and its binding to DEAE resins during the purification, recombinant HP-NAP expressed in Escherichia coli was subjected to DEAE negative mode chromatography at pH ranging from 7.0 to 9.0 at 25°C and the surface charge of purified HP-NAP was determined by capillary electrophoresis. A minimal amount of HP-NAP was detected in the elution fraction of DEAE Sepharose resin at pH 8.5, whereas recombinant HP-NAP was detected in the elution fraction of DEAE Sephadex resin only at pH 7.0 and 8.0. The purified recombinant HP-NAP obtained from the unbound fractions was not able to bind to DEAE resins at pH 7.0 to 9.0. In addition, the surface charge of the purified HP-NAP was neutral at pH 7.0 to 8.0 and was either neutral or slightly negative at pH 8.5 and 9.0. However, recombinant HP-NAP purified from gel-filtration chromatography was able to bind to DEAE Sepharose resin at pH 7.0 to 9.0 and DEAE Sephadex resin at pH 7.0. At pH 8.5 and 9.0, only the negatively charged species of HP-NAP were found. Thus, recombinant HP-NAP with different charge status can be differentially purified by DEAE negative mode chromatography and gel-filtration chromatography. Furthermore, the charge distribution on the surface of HP-NAP, the presence of impure proteins, and the overall net charge of the resins all affect the binding of HP-NAP to DEAE resins during the negative purification.

  18. Negatively Charged Lipid Membranes Promote a Disorder-Order Transition in the Yersinia YscU Protein

    PubMed Central

    Weise, Christoph F.; Login, Frédéric H.; Ho, Oanh; Gröbner, Gerhard; Wolf-Watz, Hans; Wolf-Watz, Magnus

    2014-01-01

    The inner membrane of Gram-negative bacteria is negatively charged, rendering positively charged cytoplasmic proteins in close proximity likely candidates for protein-membrane interactions. YscU is a Yersinia pseudotuberculosis type III secretion system protein crucial for bacterial pathogenesis. The protein contains a highly conserved positively charged linker sequence that separates membrane-spanning and cytoplasmic (YscUC) domains. Although disordered in solution, inspection of the primary sequence of the linker reveals that positively charged residues are separated with a typical helical periodicity. Here, we demonstrate that the linker sequence of YscU undergoes a largely electrostatically driven coil-to-helix transition upon binding to negatively charged membrane interfaces. Using membrane-mimicking sodium dodecyl sulfate micelles, an NMR derived structural model reveals the induction of three helical segments in the linker. The overall linker placement in sodium dodecyl sulfate micelles was identified by NMR experiments including paramagnetic relaxation enhancements. Partitioning of individual residues agrees with their hydrophobicity and supports an interfacial positioning of the helices. Replacement of positively charged linker residues with alanine resulted in YscUC variants displaying attenuated membrane-binding affinities, suggesting that the membrane interaction depends on positive charges within the linker. In vivo experiments with bacteria expressing these YscU replacements resulted in phenotypes displaying significantly reduced effector protein secretion levels. Taken together, our data identify a previously unknown membrane-interacting surface of YscUC that, when perturbed by mutations, disrupts the function of the pathogenic machinery in Yersinia. PMID:25418176

  19. Negatively charged lipid membranes promote a disorder-order transition in the Yersinia YscU protein.

    PubMed

    Weise, Christoph F; Login, Frédéric H; Ho, Oanh; Gröbner, Gerhard; Wolf-Watz, Hans; Wolf-Watz, Magnus

    2014-10-21

    The inner membrane of Gram-negative bacteria is negatively charged, rendering positively charged cytoplasmic proteins in close proximity likely candidates for protein-membrane interactions. YscU is a Yersinia pseudotuberculosis type III secretion system protein crucial for bacterial pathogenesis. The protein contains a highly conserved positively charged linker sequence that separates membrane-spanning and cytoplasmic (YscUC) domains. Although disordered in solution, inspection of the primary sequence of the linker reveals that positively charged residues are separated with a typical helical periodicity. Here, we demonstrate that the linker sequence of YscU undergoes a largely electrostatically driven coil-to-helix transition upon binding to negatively charged membrane interfaces. Using membrane-mimicking sodium dodecyl sulfate micelles, an NMR derived structural model reveals the induction of three helical segments in the linker. The overall linker placement in sodium dodecyl sulfate micelles was identified by NMR experiments including paramagnetic relaxation enhancements. Partitioning of individual residues agrees with their hydrophobicity and supports an interfacial positioning of the helices. Replacement of positively charged linker residues with alanine resulted in YscUC variants displaying attenuated membrane-binding affinities, suggesting that the membrane interaction depends on positive charges within the linker. In vivo experiments with bacteria expressing these YscU replacements resulted in phenotypes displaying significantly reduced effector protein secretion levels. Taken together, our data identify a previously unknown membrane-interacting surface of YscUC that, when perturbed by mutations, disrupts the function of the pathogenic machinery in Yersinia.

  20. High flux and antifouling properties of negatively charged membrane for dyeing wastewater treatment by membrane distillation.

    PubMed

    An, Alicia Kyoungjin; Guo, Jiaxin; Jeong, Sanghyun; Lee, Eui-Jong; Tabatabai, S Assiyeh Alizadeh; Leiknes, TorOve

    2016-10-15

    This study investigated the applicability of membrane distillation (MD) to treat dyeing wastewater discharged by the textile industry. Four different dyes containing methylene blue (MB), crystal violet (CV), acid red 18 (AR18), and acid yellow 36 (AY36) were tested. Two types of hydrophobic membranes made of polytetrafluoroethylene (PTFE) and polyvinylidene fluoride (PVDF) were used. The membranes were characterized by testing against each dye (foulant-foulant) and the membrane-dye (membrane-foulant) interfacial interactions and their mechanisms were identified. The MD membranes possessed negative charges, which facilitated the treatment of acid and azo dyes of the same charge and showed higher fluxes. In addition, PTFE membrane reduced the wettability with higher hydrophobicity of the membrane surface. The PTFE membrane evidenced especially its resistant to dye absorption, as its strong negative charge and chemical structure caused a flake-like (loose) dye-dye structure to form on the membrane surface rather than in the membrane pores. This also enabled the recovery of flux and membrane properties by water flushing (WF), thereby direct-contact MD with PTFE membrane treating 100 mg/L of dye mixtures showed stable flux and superior color removal during five days operation. Thus, MD shows a potential for stable long-term operation in conjunction with a simple membrane cleaning process, and its suitability in dyeing wastewater treatment. Copyright © 2016 Elsevier Ltd. All rights reserved.

  1. Complex shaped boron carbides from negative additive manufacturing

    DOE PAGES

    Lu, Ryan; Chandrasekaran, Swetha; Du Frane, Wyatt L.; ...

    2018-03-13

    In this paper, complex shaped boron carbide with carbon (B 4C/C) at near-full densities were achieved for the first time using negative additive manufacturing techniques via gelcasting. Negative additive manufacturing involves 3D printing of sacrificial molds used for casting negative copies. B 4C powder distributions and rheology of suspensions were optimized to successfully cast complex shapes. In addition to demonstrating scalability of these complex geometries, hierarchically meso-porous structures were also shown to be possible from this technique. Resorcinol-Formaldehyde (RF) polymer was selected as the gelling agent and can also pyrolyze into a carbon aerogel network to act as the sinteringmore » aid for B 4C. Finally, due to the highly effective distribution of in situ carbon for the B 4C matrix, near-full sintered density of 97–98% of theoretical maximum density was achieved.« less

  2. Complex shaped boron carbides from negative additive manufacturing

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Lu, Ryan; Chandrasekaran, Swetha; Du Frane, Wyatt L.

    In this paper, complex shaped boron carbide with carbon (B 4C/C) at near-full densities were achieved for the first time using negative additive manufacturing techniques via gelcasting. Negative additive manufacturing involves 3D printing of sacrificial molds used for casting negative copies. B 4C powder distributions and rheology of suspensions were optimized to successfully cast complex shapes. In addition to demonstrating scalability of these complex geometries, hierarchically meso-porous structures were also shown to be possible from this technique. Resorcinol-Formaldehyde (RF) polymer was selected as the gelling agent and can also pyrolyze into a carbon aerogel network to act as the sinteringmore » aid for B 4C. Finally, due to the highly effective distribution of in situ carbon for the B 4C matrix, near-full sintered density of 97–98% of theoretical maximum density was achieved.« less

  3. Numerical modelling of needle-grid electrodes for negative surface corona charging system

    NASA Astrophysics Data System (ADS)

    Zhuang, Y.; Chen, G.; Rotaru, M.

    2011-08-01

    Surface potential decay measurement is a simple and low cost tool to examine electrical properties of insulation materials. During the corona charging stage, a needle-grid electrodes system is often used to achieve uniform charge distribution on the surface of the sample. In this paper, a model using COMSOL Multiphysics has been developed to simulate the gas discharge. A well-known hydrodynamic drift-diffusion model was used. The model consists of a set of continuity equations accounting for the movement, generation and loss of charge carriers (electrons, positive and negative ions) coupled with Poisson's equation to take into account the effect of space and surface charges on the electric field. Four models with the grid electrode in different positions and several mesh sizes are compared with a model that only has the needle electrode. The results for impulse current and surface charge density on the sample clearly show the effect of the extra grid electrode with various positions.

  4. The effect of surface charge, negative and bipolar ionization on the deposition of airborne bacteria.

    PubMed

    Meschke, S; Smith, B D; Yost, M; Miksch, R R; Gefter, P; Gehlke, S; Halpin, H A

    2009-04-01

    A series of experiments were conducted to evaluate the effect of surface charge and air ionization on the deposition of airborne bacteria. The interaction between surface electrostatic potential and the deposition of airborne bacteria in an indoor environment was investigated using settle plates charged with electric potentials of 0, +/-2.5kV and +/-5kV. Results showed that bacterial deposition on the plates increased proportionally with increased potential to over twice the gravitational sedimentation rate at +5kV. Experiments were repeated under similar conditions in the presence of either negative or bipolar air ionization. Bipolar air ionization resulted in reduction of bacterial deposition onto the charged surfaces to levels nearly equal to gravitational sedimentation. In contrast, diffusion charging appears to have occurred during negative air ionization, resulting in an even greater deposition onto the oppositely charged surface than observed without ionization. Static charges on fomitic surfaces may attract bacteria resulting in deposition in excess of that expected by gravitational sedimentation or simple diffusion. Implementation of bipolar ionization may result in reduction of bacterial deposition. Fomitic surfaces are important vehicles for the transmission of infectious organisms. This study has demonstrated a simple strategy for minimizing charge related deposition of bacteria on surfaces.

  5. Lactoferricin B causes depolarization of the cytoplasmic membrane of Escherichia coli ATCC 25922 and fusion of negatively charged liposomes.

    PubMed

    Ulvatne, H; Haukland, H H; Olsvik, O; Vorland, L H

    2001-03-09

    Antimicrobial peptides have been extensively studied in order to elucidate their mode of action. Most of these peptides have been shown to exert a bactericidal effect on the cytoplasmic membrane of bacteria. Lactoferricin is an antimicrobial peptide with a net positive charge and an amphipatic structure. In this study we examine the effect of bovine lactoferricin (lactoferricin B; Lfcin B) on bacterial membranes. We show that Lfcin B neither lyses bacteria, nor causes a major leakage from liposomes. Lfcin B depolarizes the membrane of susceptible bacteria, and induces fusion of negatively charged liposomes. Hence, Lfcin B may have additional targets responsible for the antibacterial effect.

  6. Gas-Phase Stability of Negatively Charged Organophosphate Metabolites Produced by Electrospray Ionization and Matrix-Assisted Laser Desorption/Ionization

    NASA Astrophysics Data System (ADS)

    Asakawa, Daiki; Mizuno, Hajime; Toyo'oka, Toshimasa

    2017-12-01

    The formation mechanisms of singly and multiply charged organophosphate metabolites by electrospray ionization (ESI) and their gas phase stabilities were investigated. Metabolites containing multiple phosphate groups, such as adenosine 5'-diphosphate (ADP), adenosine 5'-triphosphate (ATP), and D- myo-inositol-1,4,5-triphosphate (IP3) were observed as doubly deprotonated ions by negative-ion ESI mass spectrometry. Organophosphates with multiple negative charges were found to be unstable and often underwent loss of PO3 -, although singly deprotonated analytes were stable. The presence of fragments due to the loss of PO3 - in the negative-ion ESI mass spectra could result in the misinterpretation of analytical results. In contrast to ESI, matrix-assisted laser desorption ionization (MALDI) produced singly charged organophosphate metabolites with no associated fragmentation, since the singly charged anions are stable. The stability of an organophosphate metabolite in the gas phase strongly depends on its charge state. The fragmentations of multiply charged organophosphates were also investigated in detail through density functional theory calculations. [Figure not available: see fulltext.

  7. The role of negatively charged lipids in lysosomal phospholipase A2 function

    PubMed Central

    Abe, Akira; Shayman, James A.

    2009-01-01

    Lysosomal phospholipase A2 (LPLA2) is characterized by increased activity toward zwitterionic phospholipid liposomes containing negatively charged lipids under acidic conditions. The effect of anionic lipids on LPLA2 activity was investigated. Mouse LPLA2 activity was assayed as C2-ceramide transacylation. Sulfatide incorporated into liposomes enhanced LPLA2 activity under acidic conditions and was weakened by NaCl or increased pH. Amiodarone, a cationic amphiphilic drug, reduced LPLA2 activity. LPLA2 exhibited esterase activity when p-nitro-phenylbutyrate (pNPB) was used as a substrate. Unlike the phospholipase A2 activity, the esterase activity was detected over wide pH range and not inhibited by NaCl or amiodarone. Presteady-state kinetics using pNPB were consistent with the formation of an acyl-enzyme intermediate. C2-ceramide was an acceptor for the acyl group of the acyl-enzyme but was not available as the acyl group acceptor when dispersed in liposomes containing amiodarone. Cosedimentation of LPLA2 with liposomes was enhanced in the presence of sulfatide and was reduced by raising NaCl, amiodarone, or pH in the reaction mixture. LPLA2 adsorption to negatively charged lipid membrane surfaces through an electrostatic attraction, therefore, enhances LPLA2 enzyme activity toward insoluble substrates. Thus, anionic lipids present within lipid membranes enhance the rate of phospholipid hydrolysis by LPLA2 at lipid-water interfaces.—Abe, A., and J. A. Shayman. The role of negatively charged lipids in lysosomal phospholipase A2 function. PMID:19321879

  8. Excitation of Kelvin Helmholtz instability by an ion beam in a plasma with negatively charged dust grains

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Rani, Kavita; Sharma, Suresh C.

    2015-02-15

    An ion beam propagating through a magnetized dusty plasma drives Kelvin Helmholtz Instability (KHI) via Cerenkov interaction. The frequency of the unstable wave increases with the relative density of negatively charged dust grains. It is observed that the beam has stabilizing effect on the growth rate of KHI for low shear parameter, but for high shear parameter, the instability is destabilized with relative density of negatively charged dust grains.

  9. High negative charge of a dust particle in a hot cathode discharge.

    PubMed

    Arnas, C; Mikikian, M; Doveil, F

    1999-12-01

    Dust particle levitation experiments in a plasma produced by a hot filament discharge, operating at low argon pressure, are presented. The basic characteristics of a dust grain trapped in a plate sheath edge in these experimental conditions are reported. Taking into account the sheath potential profiles measured with a differential emissive probe diagnostic, the forces applied to an isolated dust grain can be determined. Two different experimental methods yield approximately the same value for the dust charge. The observed high negative charge is mainly due to the contribution of the primary electrons emitted by the filaments as predicted by a simple model.

  10. Ionization Efficiency of Doubly Charged Ions Formed from Polyprotic Acids in Electrospray Negative Mode

    NASA Astrophysics Data System (ADS)

    Liigand, Piia; Kaupmees, Karl; Kruve, Anneli

    2016-07-01

    The ability of polyprotic acids to give doubly charged ions in negative mode electrospray was studied and related to physicochemical properties of the acids via linear discriminant analysis (LDA). It was discovered that the compound has to be strongly acidic (low p K a1 and p K a2) and to have high hydrophobicity (log P ow) to become multiply charged. Ability to give multiply charged ions in ESI/MS cannot be directly predicted from the solution phase acidities. Therefore, for the first time, a quantitative model to predict the charge state of the analyte in ESI/MS is proposed and validated for small anions. Also, a model to predict ionization efficiencies of these analytes was developed. Results indicate that acidity of the analyte, its octanol-water partition coefficient, and charge delocalization are important factors that influence ionization efficiencies as well as charge states of the analytes. The pH of the solvent was also found to be an important factor influencing the ionization efficiency of doubly charged ions.

  11. Controllable transition from positive space charge to negative space charge in an inverted cylindrical magnetron

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Rane, R., E-mail: ramu@ipr.res.in; Ranjan, M.; Mukherjee, S.

    2016-01-15

    The combined effect of magnetic field (B), gas pressure (P), and the corresponding discharge voltage on the discharge properties of argon in inverted cylindrical magnetron has been investigated. In the experiment, anode is biased with continuous 10 ms sinusoidal half wave. It is observed that at a comparatively higher magnetic field (i.e., >200 gauss) and lower operating pressure (i.e., <1 × 10{sup −3} mbar), the discharge extinguishes and demands a high voltage to reignite. Discharge current increases with increase in magnetic field and starts reducing at sufficiently higher magnetic field for a particular discharge voltage due to restricted electron diffusion towards the anode.more » It is observed that B/P ratio plays an important role in sustaining the discharge and is constant for a discharge voltage. The discharge is transformed to negative space charge regime from positive space charge regime at certain B/P ratio and this ratio varies linearly with the discharge voltage. The space charge reversal is indicated by the radial profile of the floating potential and plasma potential in between two electrodes for different magnetic fields. At a particular higher magnetic field (beyond 100 gauss), the floating potential increases gradually with the radial distance from cathode, whereas it remains almost constant at lower magnetic field.« less

  12. Enzyme-polyelectrolyte complexes in water-ethanol mixtures: negatively charged groups artificially introduced into alpha-chymotrypsin provide additional activation and stabilization effects.

    PubMed

    Kudryashova, E V; Gladilin, A K; Vakurov, A V; Heitz, F; Levashov, A V; Mozhaev, V V

    1997-07-20

    Formation of noncovalent complexes between alpha-chymotrypsin (CT) and a polyelectrolyte, polybrene (PB), has been shown to produce two major effects on enzymatic reactions in binary mixtures of polar organic cosolvents with water. (i) At moderate concentrations of organic cosolvents (10% to 30% v/v), enzymatic activity of CT is higher than in aqueous solutions, and this activation effect is more significant for CT in complex with PB (5- to 7-fold) than for free enzyme (1.5- to 2.5-fold). (ii) The range of cosolvent concentrations that the enzyme tolerates without complete loss of catalytic activity is much broader. For enhancement of enzyme stability in the complex with the polycation, the number of negatively charged groups in the protein has been artificially increased by using chemical modification with pyromellitic and succinic anhydrides. Additional activation effect at moderate concentrations of ethanol and enhanced resistance of the enzyme toward inactivation at high concentrations of the organic solvent have been observed for the modified preparations of CT in the complex with PB as compared with an analogous complex of the native enzyme. Structural changes behind alterations in enzyme activity in water-ethanol mixtures have been studied by the method of circular dichroism (CD). Protein conformation of all CT preparations has not changed significantly up to 30% v/v of ethanol where activation effects in enzymatic catalysis were most pronounced. At higher concentrations of ethanol, structural changes in the protein have been observed for different forms of CT that were well correlated with a decrease in enzymatic activity. (c) 1997 John Wiley & Sons, Inc. Biotechnol Bioeng 55: 267-277, 1997.

  13. The Distinction between Positive and Negative Reinforcement: Some Additional Considerations

    ERIC Educational Resources Information Center

    Sidman, Murray

    2006-01-01

    In this article, the author discusses the distinction between positive and negative reinforcement and some additional considerations. He states that the concept of negative reinforcement has caused confusion, and he believes that the difficulty stems from conventions of ordinary speech, in which the term "negative" usually denotes the opposite of…

  14. The influence of charge and the distribution of charge in the polar region of phospholipids on the activity of UDP-glucuronosyltransferase.

    PubMed

    Zakim, D; Eibl, H

    1992-07-05

    Studies of the mechanism of lipid-induced regulation of the microsomal enzyme UDP-glucuronosyltransferase have been extended by examining the influence of charge within the polar region on the ability of lipids to activate delipidated pure enzyme. The effects of net negative charge, of charge separation in phosphocholine, and of the distribution of charge in the polar region of lipids were studied using the GT2p isoform isolated from pig liver. Prior experiments have shown that lipids with net negative charge inhibit the enzyme (Zakim, D., Cantor, M., and Eibl, H. (1988) J. Biol. Chem. 263, 5164-5169). The current experiments show that the extent of inhibition on a molar basis increases as the net negative charge increases from -1 to -2. The inhibitory effect of negatively charged lipids is on the functional state of the enzyme and is not due to electrostatic repulsion of negatively charged substrates of the enzyme. Although the inhibitory effect of net negative charge is removed when negative charge is balanced by a positive charge due to a quaternary nitrogen, neutrality of the polar region is not a sufficient condition for activation of the enzyme. In addition to a balance of charge between Pi and the quaternary nitrogen, the distance between the negative and positive charges and the orientation of the dipole created by them are critical for activation of GT2p. The negative and positive charges must be separated by the equivalent of three -CH2- groups for optimal activation by a lipid. Shortening this distance by one -CH2- unit leads to a lipid that is ineffective in activating the enzyme. Reversal of the orientation of the dipole in which the negative charge is on the polymethylene side of the lipid-water interface and the positive charge extends into water also produces a lipid that is not effective for activating GT2p. On the other hand, lipids with phosphoserine as the polar region, which has the "normal" P-N distance but carries a net negative charge, do

  15. Preparation and chromatographic evaluation of zwitterionic stationary phases with controllable ratio of positively and negatively charged groups.

    PubMed

    Cheng, Xiao-Dong; Hao, Yan-Hong; Peng, Xi-Tian; Yuan, Bi-Feng; Shi, Zhi-Guo; Feng, Yu-Qi

    2015-08-15

    The present study described the preparation and application of zwitterionic stationary phases (ACS) with controllable ratio of positively charged tertiary amine groups and negatively charged carboxyl groups. Various parameters, including water content, pH values and ionic strength of the mobile phase, were investigated to study the chromatographic characteristics of ACS columns. The prepared ACS columns demonstrated a mix-mode retention mechanism composed of surface adsorption, partitioning and electrostatic interactions. The elemental analysis of different batches of the ACS phases demonstrated good reproducibility of the preparation strategy. Additionally, various categories of compounds, including nucleosides, water-soluble vitamins, benzoic acid derivatives and basic compounds were successively employed to evaluate the separation selectivity of the prepared ACS stationary phases. These ACS phases exhibited entirely different selectivity and retention behavior from each other for various polar analytes, demonstrating the excellent application potential in the analysis of polar compounds in HILIC. Copyright © 2015 Elsevier B.V. All rights reserved.

  16. Positive and negative contribution to birefringence in a family of carbonates: A Born effective charges analysis

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Jing, Qun; Yang, Guang; Hou, Juan

    It is an important topic to investigate the birefringence and reveal the contribution from ions to birefringence because it plays an important role in nonlinear optical materials. In this paper, the birefringence of carbonates with coplanar CO{sub 3} groups were investigated using the first-principles method. The results show that the lead carbonates exhibit relative large birefringence. After detailed investigate the electronic structures, and Born effective charges, the authors find out that anisotropic electron distribution in the CO{sub 3} groups and Pb atoms give positive contribution, while the negative contribution was found from fluorine atoms, meanwhile the Ca, Mg, and Cdmore » atoms give very small contribution to birefringence. - Graphical abstract: Using the DFT and Born effective charges, the birefringence and the contribution of ions were investigated, the positive and negative contribution was found from Pb and F ions, respectively. - Highlights: • Optical properties and Born effective charges of carbonates are investigated. • Lead carbonates exhibit relative large birefringence. • Coplanar CO{sub 3} groups and Pb atoms give positive contribution. • F atoms give negative contribution. • Ca, Mg, and Cd atoms give very small contribution.« less

  17. Comparison of Positively and Negatively Charged Achiral Co-Monomers Added to Cyclodextrin Monolith: Improved Chiral Separations in Capillary Electrochromatography

    PubMed Central

    Lu, Yang; Shamsi, Shahab A.

    2014-01-01

    Cyclodextrins (CDs) and their derivatives have been one of the most popular and successful chiral additives used in electrokinetic chromatography because of the presence of multiple chiral centers, which leads to multiple chiral interactions. However, there has been relatively less published work on the use of CDs as monolithic media for capillary electrochromatography (CEC). The goal of this study was to show how the addition of achiral co-monomer to a polymerizable CD such as glycidyl methacrylate β-cyclodextrin (GMA/β-CD) can affect the enantioselective separations in monolithic CEC. To achieve this goal, polymeric monoliths columns were prepared by co-polymerizing GMA/β-CD with cationic or anionic achiral co-monomers [(2-acrylamido-2-methyl-1-propanesulfonic acid (AMPS) and vinyl benzyltrimethyl-ammonium (VBTA)] in the presence of conventional crosslinker (ethylene dimethacrylate) and ternary porogen system including butanediol, propanol and water. A total of 34 negatively charged compounds, 30 positively charged compounds and 33 neutral compounds were screened to compare the enantioresolution capability on the GMA/β-CD, GMA/β-CD-VBTA and GMA/β-CD-AMPS monolithic columns. PMID:24108813

  18. Optical pumping of electron and nuclear spin in a negatively-charged quantum dot

    NASA Astrophysics Data System (ADS)

    Bracker, Allan; Gershoni, David; Korenev, Vladimir

    2005-03-01

    We report optical pumping of electron and nuclear spins in an individual negatively-charged quantum dot. With a bias-controlled heterostructure, we inject one electron into the quantum dot. Intense laser excitation produces negative photoluminescence polarization, which is easily erased by the Hanle effect, demonstrating optical pumping of a long-lived resident electron. The electron spin lifetime is consistent with the influence of nuclear spin fluctuations. Measuring the Overhauser effect in high magnetic fields, we observe a high degree of nuclear spin polarization, which is closely correlated to electron spin pumping.

  19. Internal transitions of neutral (X) and negatively charged (X(-)) magneto-excitons investigated by optically detected resonance (ODR) spectroscopy

    NASA Astrophysics Data System (ADS)

    Nickel, Hans Andreas

    Optically detected resonance (ODR) spectroscopy, an experimental technique combining spectroscopy in the far-infrared and visible regimes of the spectrum, has been applied to non-intentionally- and modulation-doped, quasi-2D GaAs/AlGaAs heterostructures at low temperatures and high magnetic fields to study internal transitions of neutral (X) and negatively charged (X--) magneto-excitons. In quasi-2D GaAs/AlGaAs heterostructures with a low density of free carriers, such as undoped multiple-quantum-wells, the ground state of optical excitations is the neutral exciton. This hydrogenic system was studied by far-infrared ODR spectroscopy, and internal excitonic transitions (IETs) 1s → np+/- from the ground state (1s) to excited states (np+/-) were found. Three samples of different well widths were studied systematically, and the behavior of the observed transitions as a function of the sample well-width was as expected. A predicted consequence of an inherent symmetry to the system was verified experimentally for the first time by the simultaneous observation of IETs and electron and hole cyclotron resonance in one sample in one experiment. In addition, it was also found, that the observability of IETs is destroyed as soon as there is a sign of X---recombination in the photoluminescence spectrum. In quantum wells with a small number of excess electrons the ground state of the system under optical excitation is the negatively charged exciton, X--. This mobile system of a hole binding two electrons differs significantly in certain aspects from its immobile impurity analogue, the negatively charged donor ion D-- . The mobility of the charged complex is tied to a hidden symmetry of magnetic translations, which leads to a new selection rule, that forbids X-- bound-to-bound transitions, in contrast to the D -- system, in which these transitions are dominant. In this dissertation, several samples that show X-- recombination in photoluminescence measurements were studied with

  20. Solvent Additive-Assisted Anisotropic Assembly and Enhanced Charge Transport of π-Conjugated Polymer Thin Films.

    PubMed

    Jeong, Jae Won; Jo, Gyounglyul; Choi, Solip; Kim, Yoong Ahm; Yoon, Hyeonseok; Ryu, Sang-Wan; Jung, Jaehan; Chang, Mincheol

    2018-05-30

    Charge transport in π-conjugated polymer films involves π-π interactions within or between polymer chains. Here, we demonstrate a facile solution processing strategy that provides enhanced intra- and interchain π-π interactions of the resultant polymer films using a good solvent additive with low volatility. These increased interactions result in enhanced charge transport properties. The effect of the good solvent additive on the intra- and intermolecular interactions, morphologies, and charge transport properties of poly(3-hexylthiophene) (P3HT) films is systematically investigated. We found that the good solvent additive facilitates the self-assembly of P3HT chains into crystalline fibrillar nanostructures by extending the solvent drying time during thin-film formation. As compared to the prior approach using a nonsolvent additive with low volatility, the solvent blend system containing a good solvent additive results in enhanced charge transport in P3HT organic field-effect transistor (OFET) devices [from ca. 1.7 × 10 -2 to ca. 8.2 × 10 -2 cm 2 V -1 s -1 for dichlorobenzene (DCB) versus 4.4 × 10 -2 cm 2 V -1 s -1 for acetonitrile]. The mobility appears to be maximized over a broad spectrum of additive concentrations (1-7 vol %), indicative of a wide processing window. Detailed analysis results regarding the charge injection and transport characteristics of the OFET devices reveal that a high-boiling-point solvent additive decreases both the contact resistance ( R c ) and channel resistance ( R ch ), contributing to the mobility enhancement of the devices. Finally, the platform presented here is proven to be applicable to alternative good solvent additives with low volatility, such as chlorobenzene (CB) and trichlorobenzene (TCB). Specifically, the mobility enhancement of the resultant P3HT films increases in the order CB (bp 131 °C) < DCB (bp 180 °C) < TCB (bp 214 °C), suggesting that solvent additives with higher boiling points provide resultant

  1. Optical pumping and negative luminescence polarization in charged GaAs quantum dots

    NASA Astrophysics Data System (ADS)

    Shabaev, Andrew; Stinaff, Eric A.; Bracker, Allan S.; Gammon, Daniel; Efros, Alexander L.; Korenev, Vladimir L.; Merkulov, Igor

    2009-01-01

    Optical pumping of electron spins and negative photoluminescence polarization are observed when interface quantum dots in a GaAs quantum well are excited nonresonantly by circularly polarized light. Both observations can be explained by the formation of long-lived dark excitons through hole spin relaxation in the GaAs quantum well prior to exciton capture. In this model, optical pumping of resident electron spins is caused by capture of dark excitons and recombination in charged quantum dots. Negative polarization results from accumulation of dark excitons in the quantum well and is enhanced by optical pumping. The dark exciton model describes the experimental results very well, including intensity and bias dependence of the photoluminescence polarization and the Hanle effect.

  2. Thermal equilibrium concentrations and effects of negatively charged Ga vacancies in n-type GaAs

    NASA Astrophysics Data System (ADS)

    Tan, T. Y.; You, H.-M.; Gösele, U. M.

    1993-03-01

    We have calculated the thermal equilibrium concentrations of the various negatively charged Ga vacancy species in GaAs. The triply-negatively-charged Ga vacancy, V {Ga/3-}, has been emphasized, since it dominates Ga self-diffusion and Ga-Al interdiffusion under intrinsic and n-doping conditions, as well as the diffusion of Si donor atoms occupying Ga sites. Under strong n-doping conditions, the thermal equilibrium V {Ga/3-}concentration, C_{V_{_{Ga} }^{3 - } }^{eq} (n), has been found to exhibit a temperature independence or a negative temperature dependence, i.e., the C_{V_{_{Ga} }^{3 - } }^{eq} (n) value is either unchanged or increases as the temperature is lowered. This is quite contrary to the normal point defect behavior for which the point defect thermal equilibrium concentration decreases as the temperature is lowered. This C_{V_{_{Ga} }^{3 - } }^{eq} (n) property provides explanations to a number of outstanding experimental results, either requiring the interpretation that V {Ga/3-}has attained its thermal equilibrium concentration at the onset of each experiment, or requiring mechanisms involving point defect non-equilibrium phenomena.

  3. Electrolyte additive enabled fast charging and stable cycling lithium metal batteries

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Zheng, Jianming; Engelhard, Mark H.; Mei, Donghai

    2017-03-01

    Lithium (Li) metal battery is an attractive energy storage system owing to the ultrahigh specific capacity and the lowest redox potential of Li metal anode. However, safety concern associated with dendrite growth and limited cycle life especially at a high charge current density are two critical challenges hindering the practical applications of rechargeable Li metal batteries. Here, we report for the first time that an optimal amount (0.05 M) of LiPF6 as additive in the LiTFSI-LiBOB dual-salt/carbonate-based electrolyte can significantly enhance the charging capability and the long-term cycle life of Li metal batteries with a moderately high cathode loading ofmore » 1.75 mAh cm-2. Unprecedented stable-cycling (97.1% capacity retention after 500 cycles) along with very limited increase in electrode over-potential has been achieved at a high current density of 1.75 mA cm-2. This unparalleled fast charging and stable cycling performance is contributed from both the stabilized Al cathode current collector, and, more importantly, the robust and conductive SEI layer formed on Li metal anode in the presence of the LiPF6 additive.« less

  4. Negatively charged silver nanoparticles with potent antibacterial activity and reduced toxicity for pharmaceutical preparations.

    PubMed

    Salvioni, Lucia; Galbiati, Elisabetta; Collico, Veronica; Alessio, Giulia; Avvakumova, Svetlana; Corsi, Fabio; Tortora, Paolo; Prosperi, Davide; Colombo, Miriam

    2017-01-01

    The discovery of new solutions with antibacterial activity as efficient and safe alternatives to common preservatives (such as parabens) and to combat emerging infections and drug-resistant bacterial pathogens is highly expected in cosmetics and pharmaceutics. Colloidal silver nanoparticles (NPs) are attracting interest as novel effective antimicrobial agents for the prevention of several infectious diseases. Water-soluble, negatively charged silver nanoparticles (AgNPs) were synthesized by reduction with citric and tannic acid and characterized by transmission electron microscopy, dynamic light scattering, zeta potential, differential centrifuge sedimentation, and ultraviolet-visible spectroscopy. AgNPs were tested with model Gram-negative and Gram-positive bacteria in comparison to two different kinds of commercially available AgNPs. In this work, AgNPs with higher antibacterial activity compared to the commercially available colloidal silver solutions were prepared and investigated. Bacteria were plated and the antibacterial activity was tested at the same concentration of silver ions in all samples. The AgNPs did not show any significant reduction in the antibacterial activity for an acceptable time period. In addition, AgNPs were transferred to organic phase and retained their antibacterial efficacy in both aqueous and nonaqueous media and exhibited no toxicity in eukaryotic cells. We developed AgNPs with a 20 nm diameter and negative zeta potential with powerful antibacterial activity and low toxicity compared to currently available colloidal silver, suitable for cosmetic preservatives and pharmaceutical preparations administrable to humans and/or animals as needed.

  5. Negatively charged silver nanoparticles with potent antibacterial activity and reduced toxicity for pharmaceutical preparations

    PubMed Central

    Salvioni, Lucia; Galbiati, Elisabetta; Collico, Veronica; Alessio, Giulia; Avvakumova, Svetlana; Corsi, Fabio; Tortora, Paolo; Prosperi, Davide; Colombo, Miriam

    2017-01-01

    Background The discovery of new solutions with antibacterial activity as efficient and safe alternatives to common preservatives (such as parabens) and to combat emerging infections and drug-resistant bacterial pathogens is highly expected in cosmetics and pharmaceutics. Colloidal silver nanoparticles (NPs) are attracting interest as novel effective antimicrobial agents for the prevention of several infectious diseases. Methods Water-soluble, negatively charged silver nanoparticles (AgNPs) were synthesized by reduction with citric and tannic acid and characterized by transmission electron microscopy, dynamic light scattering, zeta potential, differential centrifuge sedimentation, and ultraviolet–visible spectroscopy. AgNPs were tested with model Gram-negative and Gram-positive bacteria in comparison to two different kinds of commercially available AgNPs. Results In this work, AgNPs with higher antibacterial activity compared to the commercially available colloidal silver solutions were prepared and investigated. Bacteria were plated and the antibacterial activity was tested at the same concentration of silver ions in all samples. The AgNPs did not show any significant reduction in the antibacterial activity for an acceptable time period. In addition, AgNPs were transferred to organic phase and retained their antibacterial efficacy in both aqueous and nonaqueous media and exhibited no toxicity in eukaryotic cells. Conclusion We developed AgNPs with a 20 nm diameter and negative zeta potential with powerful antibacterial activity and low toxicity compared to currently available colloidal silver, suitable for cosmetic preservatives and pharmaceutical preparations administrable to humans and/or animals as needed. PMID:28408822

  6. On-Demand Generation of Neutral and Negatively Charged Silicon-Vacancy Centers in Diamond

    NASA Astrophysics Data System (ADS)

    Dhomkar, Siddharth; Zangara, Pablo R.; Henshaw, Jacob; Meriles, Carlos A.

    2018-03-01

    Point defects in wide-band-gap semiconductors are emerging as versatile resources for nanoscale sensing and quantum information science, but our understanding of the photoionization dynamics is presently incomplete. Here, we use two-color confocal microscopy to investigate the dynamics of charge in type 1b diamond hosting nitrogen-vacancy (NV) and silicon-vacancy (SiV) centers. By examining the nonlocal fluorescence patterns emerging from local laser excitation, we show that, in the simultaneous presence of photogenerated electrons and holes, SiV (NV) centers selectively transform into the negative (neutral) charge state. Unlike NVs, 532 nm illumination ionizes SiV- via a single-photon process, thus hinting at a comparatively shallower ground state. In particular, slower ionization rates at longer wavelengths suggest the latter lies approximately ˜1.9 eV below the conduction band minimum. Building on the above observations, we demonstrate on-demand SiV and NV charge initialization over large areas via green laser illumination of variable intensity.

  7. Novel colorimetric assay for paraquat detection on-silica bead using negatively charged silver nanoparticles.

    PubMed

    Siangproh, Weena; Somboonsuk, Thachkorn; Chailapakul, Orawan; Songsrirote, Kriangsak

    2017-11-01

    A simple, rapid, sensitive, and economical method based on colorimetry for the determination of paraquat, a widely used herbicide, was developed. Citrate-coated silver nanoparticles (AgNPs) were synthesized as the colorimetric probe. The mechanism of the assay is related to the aggregation of negatively charged AgNPs as induced by positively-charged paraquat resulting from coulombic attraction which causes the color to change from a deep greenish yellow to pale yellow in accordance with the concentrations of paraquat. Silica gel was exploited as the paraquat adsorbent for purification and pre-concentration prior to the direct determination with negatively charged AgNPs without the requirement of the elution step. The validity of the proposed approach was evaluated by spiking standard paraquat in water and plant samples. Recoveries of paraquat in water samples were 93.6% and 95.4% for groundwater and canal water, respectively, while those in plant samples were 89.5% and 86.6% for Chinese cabbage and green apple, respectively,after using the optimized extraction procedure. The absorbance of AgNPs at 400nm was linearly related to the concentration of paraquat over the range of 0.05-50mgL -1 , with detection limits of 0.05mgL -1 for water samples, and 0.10mgL -1 for plant samples by naked eye determination. Copyright © 2017 Elsevier B.V. All rights reserved.

  8. Electrolyte additive enabled fast charging and stable cycling lithium metal batteries

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Zheng, Jianming; Engelhard, Mark H.; Mei, Donghai

    2017-03-01

    Batteries using lithium (Li) metal as anodes are considered promising energy storage systems because of their high energy densities. However, safety concerns associated with dendrite growth along with limited cycle life, especially at high charge current densities, hinder their practical uses. Here we report that an optimal amount (0.05 M) of LiPF6 as an additive in LiTFSI-LiBOB dual-salt/carbonate-solvent-based electrolytes significantly enhances the charging capability and cycling stability of Li metal batteries. In a Li metal battery using a 4-V Li-ion cathode at a moderately high loading of 1.75mAh cm(-2), a cyclability of 97.1% capacity retention after 500 cycles along withmore » very limited increase in electrode overpotential is accomplished at a charge/discharge current density up to 1.75 mA cm(-2). The fast charging and stable cycling performances are ascribed to the generation of a robust and conductive solid electrolyte interphase at the Li metal surface and stabilization of the Al cathode current collector.« less

  9. Highly efficient bioinspired molecular Ru water oxidation catalysts with negatively charged backbone ligands.

    PubMed

    Duan, Lele; Wang, Lei; Li, Fusheng; Li, Fei; Sun, Licheng

    2015-07-21

    The oxygen evolving complex (OEC) of the natural photosynthesis system II (PSII) oxidizes water to produce oxygen and reducing equivalents (protons and electrons). The oxygen released from PSII provides the oxygen source of our atmosphere; the reducing equivalents are used to reduce carbon dioxide to organic products, which support almost all organisms on the Earth planet. The first photosynthetic organisms able to split water were proposed to be cyanobacteria-like ones appearing ca. 2.5 billion years ago. Since then, nature has chosen a sustainable way by using solar energy to develop itself. Inspired by nature, human beings started to mimic the functions of the natural photosynthesis system and proposed the concept of artificial photosynthesis (AP) with the view to creating energy-sustainable societies and reducing the impact on the Earth environments. Water oxidation is a highly energy demanding reaction and essential to produce reducing equivalents for fuel production, and thereby effective water oxidation catalysts (WOCs) are required to catalyze water oxidation and reduce the energy loss. X-ray crystallographic studies on PSII have revealed that the OEC consists of a Mn4CaO5 cluster surrounded by oxygen rich ligands, such as oxyl, oxo, and carboxylate ligands. These negatively charged, oxygen rich ligands strongly stabilize the high valent states of the Mn cluster and play vital roles in effective water oxidation catalysis with low overpotential. This Account describes our endeavors to design effective Ru WOCs with low overpotential, large turnover number, and high turnover frequency by introducing negatively charged ligands, such as carboxylate. Negatively charged ligands stabilized the high valent states of Ru catalysts, as evidenced by the low oxidation potentials. Meanwhile, the oxygen production rates of our Ru catalysts were improved dramatically as well. Thanks to the strong electron donation ability of carboxylate containing ligands, a seven

  10. Powder bed charging during electron-beam additive manufacturing

    DOE PAGES

    Cordero, Zachary C.; Meyer, Harry M.; Nandwana, Peeyush; ...

    2016-11-18

    Electrons injected into the build envelope during powder-bed electron-beam additive manufacturing can accumulate on the irradiated particles and cause them to repel each other. Furthermore, these electrostatic forces can grow so large that they drive the particles out of the build envelope in a process known as smoking. Here, a model of powder bed charging is formulated and used to develop criteria that predict the conditions under which the powder bed will smoke. These criteria suggest dependences on particle size, pre-heat temperature, and process parameters that align closely with those observed in practice.

  11. Polarization spectroscopy of positive and negative trions in an InAs quantum dot

    NASA Astrophysics Data System (ADS)

    Ware, Morgan E.; Bracker, Allan S.; Stinaff, Eric; Gammon, Daniel; Gershoni, David; Korenev, Vladimir L.

    2005-02-01

    Using polarization-sensitive photoluminescence and photoluminescence excitation spectroscopy, we study single InAs/GaAs self-assembled quantum dots. The dots were embedded in an n-type, Schottky diode structure allowing for control of the charge state. We present here the exciton, singly charged exciton (positive and negative trions), and the twice negatively charged exciton. For non-resonant excitation below the wetting layer, we observed a large degree of polarization memory from the radiative recombination of both the positive and negative trions. In excitation spectra, through the p-shell, we have found several sharp resonances in the emission from the s-shell recombination of the dot in all charged states. Some of these excitation resonances exhibit strong coulomb shifts upon addition of charges into the quantum dot. One particular resonance of the negatively charged trion was found to exhibit a fine structure doublet under circular polarization. This observation is explained in terms of resonant absorption into the triplet states of the negative trion.

  12. Establishment of cell lines from adult T-cell leukemia cells dependent on negatively charged polymers.

    PubMed

    Kagami, Yoshitoyo; Uchiyama, Susumu; Kato, Harumi; Okada, Yasutaka; Seto, Masao; Kinoshita, Tomohiro

    2017-07-05

    Growing adult T-cell leukemia/lymphoma (ATLL) cells in vitro is difficult. Here, we examined the effects of static electricity in the culture medium on the proliferation of ATLL cells. Six out of 10 ATLL cells did not proliferate in vitro and thus had to be cultured in a medium containing negatively charged polymers. In the presence of poly-γ-glutamic acid (PGA) or chondroitin sulfate (CDR), cell lines (HKOX3-PGA, HKOX3-CDR) were established from the same single ATLL case using interleukin (IL)-2, IL-4, and feeder cells expressing OX40L (OX40L + HK). Dextran sulfate inhibited growth in both HKOX3 cell lines. Both PGA and OX40L + HK were indispensable for HKOX3-PGA growth, but HKOX3-CDR could proliferate in the presence of CDR or OX40L + HK alone. Thus, the specific action of each negatively charged polymer promoted the growth of specific ATLL cells in vitro.

  13. ESI-MS of Cucurbituril Complexes Under Negative Polarity.

    PubMed

    Rodrigues, Maria A A; Mendes, Débora C; Ramamurthy, Vaidhyanathan; Da Silva, José P

    2017-11-01

    Electrospray ionization mass spectrometry (ESI-MS) is a powerful tool to study host-guest supramolecular interactions. ESI-MS can be used for detailed gas-phase reactivity studies, to clarify the structure, or simply to verify the formation of complexes. Depending on the structure of the host and of the guest, negative and/or positive ESI are used. Here we report the unexpected formation of host-guest complexes between cucurbit[n]urils (n = 7, 8, CB[n]) and amine, styryl pyridine, and styryl pyridine dimer cations, under negative ESI. Non-complexed CB[n] form double charged halide (Br - , Cl - , F - ) adducts. Under negative ESI, halide ions interact with CB[n] outer surface hydrogen atoms. One to one host-guest complexes (1:1) of CB[n] with positive charged guests were also observed as single and double charged ions under negative ESI. The positive charge of guests is neutralized by ion-pairing with halide anions. Depending on the number of positive charges guests retain in the gas phase, one or two additional halide ions are required for neutralization. Complexes 1:2 of CB[8] with styryl pyridines retain two halide ions in the gas phase, one per guest. Styryl pyridine dimers form 1:1 complexes possessing a single extra halide ion and therefore a single positive charge. Negative ESI is sensitive to small structural differences between complexes, distinguishing between 1:2 complexes of styryl pyridine-CB[8] and corresponding 1:1 complexes with the dimer. Negative ESI gives simpler spectra than positive ESI and allows the determination of guest charge state of CB[n] complexes in the gas phase. Graphical Abstract ᅟ.

  14. Characteristics of EMI generated by negative metal-positive dielectric voltage stresses due to spacecraft charging

    NASA Technical Reports Server (NTRS)

    Chaky, R. C.; Inouye, G. T.

    1985-01-01

    Charging of spacecraft surfaces by the environmental plasma can result in differential potentials between metallic structure and adjacent dielectric surfaces in which the relative polarity of the voltage stress is either negative dielectric/positive metal or negative metal/positive dielectric. Negative metal/positive dielectric is a stress condition that may arise if relatively large areas of spacecraft surface metals are shadowed from solar UV and/or if the UV intensity is reduced as in the situation in which the spacecraft is entering into or leaving eclipse. The results of experimental studies of negative metal/positive dielectric systems are given. Information is given on: enhanced electron emission I-V curves; e(3) corona noise vs e(3) steady-state current; the localized nature of e(3) and negative metal arc discharge currents; negative metal arc discharges at stress thresholds below 1 kilovolt; negative metal arc discharge characteristics; dependence of blowoff arc discharge current on spacecraft capacitance to space (linear dimension); and damage to second surface mirrors due to negative metal arcs.

  15. Ordered adsorption of coagulation factor XII on negatively charged polymer surfaces probed by sum frequency generation vibrational spectroscopy.

    PubMed

    Chen, Xiaoyun; Wang, Jie; Paszti, Zoltan; Wang, Fulin; Schrauben, Joel N; Tarabara, Volodymyr V; Schmaier, Alvin H; Chen, Zhan

    2007-05-01

    Electrostatic interactions between negatively charged polymer surfaces and factor XII (FXII), a blood coagulation factor, were investigated by sum frequency generation (SFG) vibrational spectroscopy, supplemented by several analytical techniques including attenuated total reflection Fourier transform infrared spectroscopy (ATR-FTIR), quartz crystal microbalance (QCM), zeta-potential measurement, and chromogenic assay. A series of sulfonated polystyrenes (sPS) with different sulfonation levels were synthesized as model surfaces with different surface charge densities. SFG spectra collected from FXII adsorbed onto PS and sPS surfaces with different surface charge densities showed remarkable differences in spectral features and especially in spectral intensity. Chromogenic assay experiments showed that highly charged sPS surfaces induced FXII autoactivation. ATR-FTIR and QCM results indicated that adsorption amounts on the PS and sPS surfaces were similar even though the surface charge densities were different. No significant conformational change was observed from FXII adsorbed onto surfaces studied. Using theoretical calculations, the possible contribution from the third-order nonlinear optical effect induced by the surface electric field was evaluated, and it was found to be unable to yield the SFG signal enhancement observed. Therefore it was concluded that the adsorbed FXII orientation and ordering were the main reasons for the remarkable SFG amide I signal increase on sPS surfaces. These investigations indicate that negatively charged surfaces facilitate or induce FXII autoactivation on the molecular level by imposing specific orientation and ordering on the adsorbed protein molecules.

  16. The Negatively Charged Regions of Lactoferrin Binding Protein B, an Adaptation against Anti-Microbial Peptides

    PubMed Central

    Morgenthau, Ari; Beddek, Amanda; Schryvers, Anthony B.

    2014-01-01

    Lactoferrin binding protein B (LbpB) is a bi-lobed membrane bound lipoprotein that is part of the lactoferrin receptor complex in a variety of Gram-negative pathogens. Despite high sequence diversity among LbpBs from various strains and species, a cluster of negatively charged amino acids is invariably present in the protein’s C-terminal lobe in all species except Moraxella bovis. The function of LbpB in iron acquisition has yet to be experimentally demonstrated, whereas in vitro studies have shown that LbpB confers protection against lactoferricin, a short cationic antimicrobial peptide released from the N- terminus of lactoferrin. In this study we demonstrate that the negatively charged regions can be removed from the Neisseria meningitidis LbpB without compromising stability, and this results in the inability of LbpB to protect against the bactericidal effects of lactoferricin. The release of LbpB from the cell surface by the autotransporter NalP reduces the protection against lactoferricin in the in vitro killing assay, attributed to removal of LbpB during washing steps, but is unlikely to have a similar impact in vivo. The protective effect of the negatively charged polysaccharide capsule in the killing assay was less than the protection conferred by LbpB, suggesting that LbpB plays a major role in protection against cationic antimicrobial peptides in vivo. The selective release of LbpB by NalP has been proposed to be a mechanism for evading the adaptive immune response, by reducing the antibody binding to the cell surface, but may also provide insights into the primary function of LbpB in vivo. Although TbpB and LbpB have been shown to be major targets of the human immune response, the selective release of LbpB suggests that unlike TbpB, LbpB may not be essential for iron acquisition, but important for protection against cationic antimicrobial peptides. PMID:24465982

  17. Gap state charge induced spin-dependent negative differential resistance in tunnel junctions

    NASA Astrophysics Data System (ADS)

    Jiang, Jun; Zhang, X.-G.; Han, X. F.

    2016-04-01

    We propose and demonstrate through first-principles calculation a new spin-dependent negative differential resistance (NDR) mechanism in magnetic tunnel junctions (MTJ) with cubic cation disordered crystals (CCDC) AlO x or Mg1-x Al x O as barrier materials. The CCDC is a class of insulators whose band gap can be changed by cation doping. The gap becomes arched in an ultrathin layer due to the space charge formed from metal-induced gap states. With an appropriate combination of an arched gap and a bias voltage, NDR can be produced in either spin channel. This mechanism is applicable to 2D and 3D ultrathin junctions with a sufficiently small band gap that forms a large space charge. It provides a new way of controlling the spin-dependent transport in spintronic devices by an electric field. A generalized Simmons formula for tunneling current through junction with an arched gap is derived to show the general conditions under which ultrathin junctions may exhibit NDR.

  18. Photoelectron spectroscopy of color centers in negatively charged cesium iodide nanocrystals

    NASA Astrophysics Data System (ADS)

    Sarkas, Harry W.; Kidder, Linda H.; Bowen, Kit H.

    1995-01-01

    We present the photoelectron spectra of negatively charged cesium iodide nanocrystals recorded using 2.540 eV photons. The species examined were produced using an inert gas condensation cluster ion source, and they ranged in size from (CsI)-n=13 to nanocrystal anions comprised of 330 atoms. Nanocrystals showing two distinct types of photoemission behavior were observed. For (CsI)-n=13 and (CsI)-n=36-165, a plot of cluster anion photodetachment threshold energies vs n-1/3 gives a straight line extrapolating (at n-1/3=0, i.e., n=∞) to 2.2 eV, the photoelectric threshold energy for F centers in bulk cesium iodide. The linear extrapolation of the cluster anion data to the corresponding bulk property implies that the electron localization in these gas-phase nanocrystals is qualitatively similar to that of F centers in extended alkali halide crystals. These negatively charged cesium iodide nanocrystals are thus shown to support embryonic forms of F centers, which mature with increasing cluster size toward condensed phase impurity centers. Under an alternative set of source conditions, nanocrystals were produced which showed significantly lower photodetachment thresholds than the aforementioned F-center cluster anions. For these species, containing 83-131 atoms, a plot of their cluster anion photodetachment threshold energies versus n-1/3 gives a straight line which extrapolates to 1.4 eV. This value is in accord with the expected photoelectric threshold energy for F' centers in bulk cesium iodide, i.e., color centers with two excess electrons in a single defect site. These nanocrystals are interpreted to be the embryonic F'-center containing species, Cs(CsI)-n=41-65.

  19. Effects of negatively and positively charged Ti metal surfaces on ceramic coating adhesion and cell response.

    PubMed

    do Nascimento, Rodney Marcelo; de Carvalho, Vanessa Rafaela; Govone, José Silvio; Hernandes, Antônio Carlos; da Cruz, Nilson Cristino

    2017-02-01

    This manuscript reports an evaluation of the effects of simple chemical-heat treatments on the deposition of different ceramic coatings, i.e., TiO 2 , CaTiO 3 and CaP, on commercially pure titanium (cp-Ti) and Ti6Al4V and the influence of the coatings on cells interaction with the surfaces. The ceramic materials were prepared by the sol-gel method and the coating adhesion was analyzed by pull-off bending tests. The wettability of positively or negatively charged surfaces was characterized by contact angle measurements, which also enabled the calculation of the surface free energy through the polar-apolar liquids approach. Both acid and alkaline treatments activated the cp-Ti, whereas Ti6Al4V was only activated by the alkaline treatment. Such treatment led to increased hydrophilicity with inhibition of the fibroblastic response on Ti6Al4V. On the other hand, osteoblastic cells adhered to and proliferated on the positively and negatively charged surfaces. The maximum adhesion strength (~ 3400 N) was obtained with a negative Ti6Al4V-CaTiO 3 -CaP multilayer surface.

  20. Binding of cationic pentapeptides with modified side chain lengths to negatively charged lipid membranes: Complex interplay of electrostatic and hydrophobic interactions.

    PubMed

    Hoernke, Maria; Schwieger, Christian; Kerth, Andreas; Blume, Alfred

    2012-07-01

    Basic amino acids play a key role in the binding of membrane associated proteins to negatively charged membranes. However, side chains of basic amino acids like lysine do not only provide a positive charge, but also a flexible hydrocarbon spacer that enables hydrophobic interactions. We studied the influence of hydrophobic contributions to the binding by varying the side chain length of pentapeptides with ammonium groups starting with lysine to lysine analogs with shorter side chains, namely omithine (Orn), alpha, gamma-diaminobutyric acid (Dab) and alpha, beta-diaminopropionic acid (Dap). The binding to negatively charged phosphatidylglycerol (PG) membranes was investigated by calorimetry, FT-infrared spectroscopy (FT-IR) and monolayer techniques. The binding was influenced by counteracting and sometimes compensating contributions. The influence of the bound peptides on the lipid phase behavior depends on the length of the peptide side chains. Isothermal titration calorimetry (ITC) experiments showed exothermic and endothermic effects compensating to a different extent as a function of side chain length. The increase in lipid phase transition temperature was more significant for peptides with shorter side chains. FTIR-spectroscopy revealed changes in hydration of the lipid bilayer interface after peptide binding. Using monolayer techniques, the contributions of electrostatic and hydrophobic effects could clearly be observed. Peptides with short side chains induced a pronounced decrease in surface pressure of PG monolayers whereas peptides with additional hydrophobic interactions decreased the surface pressure much less or even lead to an increase, indicating insertion of the hydrophobic part of the side chain into the lipid monolayer.

  1. Double layer of platinum electrodes: Non-monotonic surface charging phenomena and negative double layer capacitance

    NASA Astrophysics Data System (ADS)

    Huang, Jun; Zhou, Tao; Zhang, Jianbo; Eikerling, Michael

    2018-01-01

    In this study, a refined double layer model of platinum electrodes accounting for chemisorbed oxygen species, oriented interfacial water molecules, and ion size effects in solution is presented. It results in a non-monotonic surface charging relation and a peculiar capacitance vs. potential curve with a maximum and possibly negative values in the potential regime of oxide-formation.

  2. Corona Discharge Suppression in Negative Ion Mode Nanoelectrospray Ionization via Trifluoroethanol Addition.

    PubMed

    McClory, Phillip J; Håkansson, Kristina

    2017-10-03

    Negative ion mode nanoelectrospray ionization (nESI) is often utilized to analyze acidic compounds, from small molecules to proteins, with mass spectrometry (MS). Under high aqueous solvent conditions, corona discharge is commonly observed at emitter tips, resulting in low ion abundances and reduced nESI needle lifetimes. We have successfully reduced corona discharge in negative ion mode by trace addition of trifluoroethanol (TFE) to aqueous samples. The addition of as little as 0.2% TFE increases aqueous spray stability not only in nESI direct infusion, but also in nanoflow liquid chromatography (nLC)/MS experiments. Negative ion mode spray stability with 0.2% TFE is approximately 6× higher than for strictly aqueous samples. Upon addition of 0.2% TFE to the mobile phase of nLC/MS experiments, tryptic peptide identifications increased from 93 to 111 peptides, resulting in an average protein sequence coverage increase of 18%.

  3. 13 CFR 107.1130 - Leverage fees and additional charges payable by Licensee.

    Code of Federal Regulations, 2010 CFR

    2010-01-01

    ... 13 Business Credit and Assistance 1 2010-01-01 2010-01-01 false Leverage fees and additional charges payable by Licensee. 107.1130 Section 107.1130 Business Credit and Assistance SMALL BUSINESS ADMINISTRATION SMALL BUSINESS INVESTMENT COMPANIES SBA Financial Assistance for Licensees (Leverage) General...

  4. Carbon Nanotube/Conductive Additive/Space Durable Polymer Nanocomposite Films for Electrostatic Charge Dissipation

    NASA Technical Reports Server (NTRS)

    Smith, Joseph G., Jr.; Watson, Kent A.; Delozier, Donavon M.; Connell, John W.

    2003-01-01

    Thin film membranes of space environmentally stable polymeric materials possessing low color/solar absorptivity (alpha) are of interest for potential applications on Gossamer spacecraft. In addition to these properties, sufficient electrical conductivity is required in order to dissipate electrostatic charge (ESC) build-up brought about by the charged orbital environment. One approach to achieve sufficient electrical conductivity for ESC mitigation is the incorporation of single wall carbon nanotubes (SWNTs). However, when the SWNTs are dispersed throughout the polymer matrix, the nanocomposite films tend to be significantly darker than the pristine material resulting in a higher alpha. The incorporation of conductive additives in combination with a decreased loading level of SWNTs is one approach for improving alpha while retaining conductivity. Taken individually, the low loading level of conductive additives and SWNTs is insufficient in achieving the percolation level necessary for electrical conductivity. When added simultaneously to the film, conductivity is achieved through a synergistic effect. The chemistry, physical, and mechanical properties of the nanocomposite films will be presented.

  5. Spatiotemporal dynamics of charged species in the afterglow of plasmas containing negative ions.

    PubMed

    Kaganovich, I D; Ramamurthi, B N; Economou, D J

    2001-09-01

    The spatiotemporal evolution of charged species densities and wall fluxes during the afterglow of an electronegative discharge has been investigated. The decay of a plasma with negative ions consists of two stages. During the first stage of the afterglow, electrons dominate plasma diffusion and negative ions are trapped inside the vessel by the static electric field; the flux of negative ions to the walls is nearly zero. During this stage, the electron escape frequency increases considerably in the presence of negative ions, and can eventually approach free electron diffusion. During the second stage of the afterglow, electrons have disappeared, and positive and negative ions diffuse to the walls with the ion-ion ambipolar diffusion coefficient. Theories for plasma decay have been developed for equal and strongly different ion (T(i)) and electron (T(e)) temperatures. In the case T(i)=T(e), the species spatial profiles are similar and an analytic solution exists. When detachment is important in the afterglow (weakly electronegative gases, e.g., oxygen) the plasma decay crucially depends on the product of negative ion detachment frequency (gamma(d)) and diffusion time (tau(d)). If gamma(d)tau(d)>2, negative ions convert to electrons during their diffusion towards the walls. The presence of detached electrons results in "self-trapping" of the negative ions, due to emerging electric fields, and the negative ion flux to the walls is extremely small. In the case T(i)negative ion density fronts. During the afterglow, although negative ions diffuse freely in the plasma core, the negative ion fronts propagate towards the chamber walls with a nearly constant velocity. The evolution of ion fronts in the afterglow of electronegative plasmas is important, since it determines the time needed for negative ions to reach the wall, and thus influence surface reactions in plasma processing.

  6. Remarkable enhancement of charge carrier mobility of conjugated polymer field-effect transistors upon incorporating an ionic additive

    PubMed Central

    Luo, Hewei; Yu, Chenmin; Liu, Zitong; Zhang, Guanxin; Geng, Hua; Yi, Yuanping; Broch, Katharina; Hu, Yuanyuan; Sadhanala, Aditya; Jiang, Lang; Qi, Penglin; Cai, Zhengxu; Sirringhaus, Henning; Zhang, Deqing

    2016-01-01

    Organic semiconductors with high charge carrier mobilities are crucial for flexible electronic applications. Apart from designing new conjugated frameworks, different strategies have been explored to increase charge carrier mobilities. We report a new and simple approach to enhancing the charge carrier mobility of DPP-thieno[3,2-b]thiophene–conjugated polymer by incorporating an ionic additive, tetramethylammonium iodide, without extra treatments into the polymer. The resulting thin films exhibit a very high hole mobility, which is higher by a factor of 24 than that of thin films without the ionic additive under the same conditions. On the basis of spectroscopic grazing incidence wide-angle x-ray scattering and atomic force microscopy studies as well as theoretical calculations, the remarkable enhancement of charge mobility upon addition of tetramethylammonium iodide is attributed primarily to an inhibition of the torsion of the alkyl side chains by the presence of the ionic species, facilitating a more ordered lamellar packing of the alkyl side chains and interchain π-π interactions. PMID:27386541

  7. Protein charge ladders reveal that the net charge of ALS-linked superoxide dismutase can be different in sign and magnitude from predicted values

    PubMed Central

    Shi, Yunhua; Abdolvahabi, Alireza; Shaw, Bryan F

    2014-01-01

    This article utilized “protein charge ladders”—chemical derivatives of proteins with similar structure, but systematically altered net charge—to quantify how missense mutations that cause amyotrophic lateral sclerosis (ALS) affect the net negative charge (Z) of superoxide dismutase-1 (SOD1) as a function of subcellular pH and Zn2+ stoichiometry. Capillary electrophoresis revealed that the net charge of ALS-variant SOD1 can be different in sign and in magnitude—by up to 7.4 units per dimer at lysosomal pH—than values predicted from standard pKa values of amino acids and formal oxidation states of metal ions. At pH 7.4, the G85R, D90A, and G93R substitutions diminished the net negative charge of dimeric SOD1 by up to +2.29 units more than predicted; E100K lowered net charge by less than predicted. The binding of a single Zn2+ to mutant SOD1 lowered its net charge by an additional +2.33 ± 0.01 to +3.18 ± 0.02 units, however, each protein regulated net charge when binding a second, third, or fourth Zn2+ (ΔZ < 0.44 ± 0.07 per additional Zn2+). Both metalated and apo-SOD1 regulated net charge across subcellular pH, without inverting from negative to positive at the theoretical pI. Differential scanning calorimetry, hydrogen-deuterium exchange, and inductively coupled plasma mass spectrometry confirmed that the structure, stability, and metal content of mutant proteins were not significantly affected by lysine acetylation. Measured values of net charge should be used when correlating the biophysical properties of a specific ALS-variant SOD1 protein with its observed aggregation propensity or clinical phenotype. PMID:25052939

  8. Retrieval of charge mobility from apparent charge packet movements in LDPE thin films

    NASA Astrophysics Data System (ADS)

    Meng, Jia; Zhang, Yewen; Holé, Stéphane; Zheng, Feihu; An, Zhenlian

    2017-03-01

    The charge packet phenomenon observed in polyethylene materials has been reported extensively during the last decades. To explain its movement, Negative Differential Mobility (NDM) theory is a competitive model among several proposed mechanisms. However, as a key concept of this theory, a sufficiently acute relationship between charge mobility and electric field has never been reported until now, which makes it hard to precisely describe the migration of charge packets with this theory. Based on the substantial negative-charge packet observations with a sufficiently by wide electric field range from 15 kV/mm to 50 kV/mm, the present contribution successfully retrieved the negative-charge mobility from the apparent charge packet movements, which reveals a much closer relationship between the NDM theory and charge packet migrations. Back simulations of charge packets with the retrieved charge mobility offer a good agreement with the experimental data.

  9. Negative Charge Neutralization in the Loops and Turns of Outer Membrane Phospholipase A Impacts Folding Hysteresis at Neutral pH.

    PubMed

    McDonald, Sarah K; Fleming, Karen G

    2016-11-08

    Hysteresis in equilibrium protein folding titrations is an experimental barrier that must be overcome to extract meaningful thermodynamic quantities. Traditional approaches to solving this problem involve testing a spectrum of solution conditions to find ones that achieve path independence. Through this procedure, a specific pH of 3.8 was required to achieve path independence for the water-to-bilayer equilibrium folding of outer membrane protein OmpLA. We hypothesized that the neutralization of negatively charged side chains (Asp and Glu) at pH 3.8 could be the physical basis for path-independent folding at this pH. To test this idea, we engineered variants of OmpLA with Asp → Asn and Glu → Gln mutations to neutralize the negative charges within various regions of the protein and tested for reversible folding at neutral pH. Although not fully resolved, our results show that these mutations in the periplasmic turns and extracellular loops are responsible for 60% of the hysteresis in wild-type folding. Overall, our study suggests that negative charges impact the folding hysteresis in outer membrane proteins and their neutralization may aid in protein engineering applications.

  10. Tribological Properties of Nanodiamonds in Aqueous Suspensions: Effect of the Surface Charge

    NASA Astrophysics Data System (ADS)

    Krim, J.; Liu, Zijian; Leininger, D. A.; Kooviland, A.; Smirnov, A. I.; Shendarova, O.; Brenner, D. W.

    The presence of granular nanoparticulates, be they wear particles created naturally by frictional rubbing at a geological fault line or products introduced as lubricant additives, can dramatically alter friction at solid-liquid interfaces. Given the complexity of such systems, understanding system properties at a fundamental level is particularly challenging. The Quartz Crystal Microbalance (QCM) is an ideal tool for studies of material-liquid-nanoparticulate interfaces. We have employed it here to study the uptake and nanotribological properties of positively and negatively charged 5-15 nm diameter nanodiamonds dispersed in water[1] in the both the presence and absence of a macroscopic contact with the QCM electrode. The nanodiamonds were found to impact tribological performance at both nanometer and macroscopic scales. The tribological effects were highly sensitive to the sign of the charge: negatively (positively) charged particles were more weakly (strongly) bound and reduced (increased) frictional drag at the solid-liquid interface. For the macroscopic contacts, negatively charged nanodiamonds appeared to be displaced from the contact, while the positively charged ones were not. Overall, the negatively charged nanodiamonds were more stable in an aqueous dispersion for extended time periods. Work supported by NSF and DOE.

  11. Electromagnetic Radiation in the Atmosphere Generated by Excess Negative Charge in a Nuclear-Electromagnetic Cascade

    NASA Astrophysics Data System (ADS)

    Malyshevsky, V. S.; Fomin, G. V.

    2017-01-01

    On the basis of the analytical model "PARMA" (PHITS-based Analytical Radiation Model in the Atmosphere), developed to model particle fluxes of secondary cosmic radiation in the Earth's atmosphere, we have calculated the characteristics of radio waves emitted by excess negative charge in an electromagnetic cascade. The results may be of use in an analysis of experimental data on radio emission of electron-photon showers in the atmosphere.

  12. Polarization-induced surface charges in hydroxyapatite ceramics

    NASA Astrophysics Data System (ADS)

    Horiuchi, N.; Nakaguki, S.; Wada, N.; Nozaki, K.; Nakamura, M.; Nagai, A.; Katayama, K.; Yamashita, K.

    2014-07-01

    Calcium hydroxyapatite (HAp; Ca10(PO4)6(OH)2) is a well-known biomaterial that is the main inorganic component of bones and teeth. Control over the surface charge on HAp would be a key advance in the development of the material for tissue engineering. We demonstrate here that surface charge can be induced by an electrical poling process using the Kelvin method. Positive and negative charges were induced on the HAp surface in response to the applied electric field in the poling process. The surface charging is attributed to dipole polarization that is homogeneously distributed in HAp. Additionally, the surface charging is considered to originate from the organization of OH- ions into a polar phase in the structure.

  13. Lunar Surface Charging during Solar Energetic Particle Events

    NASA Astrophysics Data System (ADS)

    Halekas, Jasper S.; Delory, G. T.; Mewaldt, R. A.; Lin, R. P.; Fillingim, M. O.; Brain, D. A.; Lee, C. O.; Stubbs, T. J.; Farrell, W. M.; Hudson, M. K.

    2006-09-01

    The surface of the Moon, not protected by any substantial atmosphere, is directly exposed to the impact of both solar UV and solar wind plasma and energetic particles. This creates a complex lunar electrostatic environment, with the surface typically charging slightly positive in sunlight, and negative in shadow. Observations from the Apollo era and theoretical considerations strongly suggest that surface charging leads to dust electrification and transport, posing a potentially significant hazard for exploration. The most significant charging effects should occur when the Moon is exposed to high-temperature plasmas like those encountered in the terrestrial plasmasheet or in solar storms. We now present evidence for kilovolt-scale negative charging of the shadowed lunar surface during solar energetic particle (SEP) events, utilizing data from the Lunar Prospector Electron Reflectometer (LP ER). We find that SEP events are associated with the most extreme lunar surface charging observed during the LP mission - rivaled only by previously reported charging during traversals of the terrestrial plasmasheet. The largest charging event observed by LP is a 4 kV negative surface potential (as compared to typical values of V) during a SEP event in May 1998. We characterize lunar surface charging during several SEP events, and compare to energetic particle measurements from ACE, Wind, and SOHO in order to determine the relationship between SEP events and extreme lunar surface charging. Space weather events are already considered by NASA to be a significant hazard to lunar exploration, due to high-energy ionizing radiation. Our observations demonstrate that plasma interactions with the lunar surface during SEP events, causing extreme surface charging and potentially significant dust electrification and transport, represent an additional hazard associated with space weather.

  14. Effect of incorporation of nitrogen atoms in Al2O3 gate dielectric of wide-bandgap-semiconductor MOSFET on gate leakage current and negative fixed charge

    NASA Astrophysics Data System (ADS)

    Kojima, Eiji; Chokawa, Kenta; Shirakawa, Hiroki; Araidai, Masaaki; Hosoi, Takuji; Watanabe, Heiji; Shiraishi, Kenji

    2018-06-01

    We performed first-principle calculations to investigate the effect of incorporation of N atoms into Al2O3 gate dielectrics. Our calculations show that the defect levels generated by VO in Al2O3 are the origin of the stress-induced gate leakage current and that VOVAl complexes in Al2O3 cause negative fixed charge. We revealed that the incorporation of N atoms into Al2O3 eliminates the VO defect levels, reducing the stress-induced gate leakage current. Moreover, this suppresses the formation of negatively charged VOVAl complexes. Therefore, AlON can reduce both stress-induced gate leakage current and negative fixed charge in wide-bandgap-semiconductor MOSFETs.

  15. Negative differential conductance in InAs wire based double quantum dot induced by a charged AFM tip

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Zhukov, A. A., E-mail: azhukov@issp.ac.ru; Volk, Ch.; Winden, A.

    We investigate the conductance of an InAs nanowire in the nonlinear regime in the case of low electron density where the wire is split into quantum dots connected in series. The negative differential conductance in the wire is initiated by means of a charged atomic force microscope tip adjusting the transparency of the tunneling barrier between two adjoining quantum dots. We confirm that the negative differential conductance arises due to the resonant tunneling between these two adjoining quantum dots. The influence of the transparency of the blocking barriers and the relative position of energy states in the adjoining dots onmore » a decrease of the negative differential conductance is investigated in detail.« less

  16. Iodide uptake by negatively charged clay interlayers?

    PubMed

    Miller, Andrew; Kruichak, Jessica; Mills, Melissa; Wang, Yifeng

    2015-09-01

    Understanding iodide interactions with clay minerals is critical to quantifying risk associated with nuclear waste disposal. Current thought assumes that iodide does not interact directly with clay minerals due to electrical repulsion between the iodide and the negatively charged clay layers. However, a growing body of work indicates a weak interaction between iodide and clays. The goal of this contribution is to report a conceptual model for iodide interaction with clays by considering clay mineral structures and emergent behaviors of chemical species in confined spaces. To approach the problem, a suite of clay minerals was used with varying degrees of isomorphic substitution, chemical composition, and mineral structure. Iodide uptake experiments were completed with each of these minerals in a range of swamping electrolyte identities (NaCl, NaBr, KCl) and concentrations. Iodide uptake behaviors form distinct trends with cation exchange capacity and mineral structure. These trends change substantially with electrolyte composition and concentration, but do not appear to be affected by solution pH. The experimental results suggest that iodide may directly interact with clays by forming ion-pairs (e.g., NaI(aq)) which may concentrate within the interlayer space as well as the thin areas surrounding the clay particle where water behavior is more structured relative to bulk water. Ion pairing and iodide concentration in these zones is probably driven by the reduced dielectric constant of water in confined space and by the relatively high polarizability of the iodide species. Copyright © 2015 Elsevier Ltd. All rights reserved.

  17. Influence of Processing Additives on Charge-Transfer Time Scales and Sound Velocity in Organic Bulk Heterojunction Films.

    PubMed

    Kaake, Loren G; Welch, Gregory C; Moses, Daniel; Bazan, Guillermo C; Heeger, Alan J

    2012-05-17

    The role of processing additives in organic bulk heterojunction thin films was investigated by means of transient absorption spectroscopy. The rate of ultrafast charge transfer was found to increase when a small amount of diiodooctane was used during film formation. In addition, coherent acoustic phonons were observed, and their velocity was determined. A strong correlation between the sound velocity and the charge-transfer time scale was observed, both of which could be explained by a subtle increase in thin film density.

  18. Hydrogen Bond Acceptors and Additional Cationic Charges in Methylene Blue Derivatives: Photophysics and Antimicrobial Efficiency

    PubMed Central

    Felgenträger, Ariane; Maisch, Tim; Dobler, Daniel; Späth, Andreas

    2013-01-01

    Photodynamic inactivation of bacteria (PIB) by efficient singlet oxygen photosensitizers might be a beneficial alternative to antibiotics in the struggle against multiresistant bacteria. Phenothiazinium dyes belong to the most prominent classes of such sensitizers due to their intense absorption in the red-light region (λ abs, max ca. 600–680 nm, ε > 50000 L mol−1 cm−1), their low toxicity, and their attachment/penetration abilities. Except simple substituents like alkyl or hydroxyalkyl residues, nearly no modifications of the phenothiaziniums have been pursued at the auxochromic sites. By this, the properties of methylene blue derivatives and their fields of application are limited; it remains unclear if their potential antimicrobial efficacy may be enhanced, also to compete with porphyrins. We prepared a set of six mainly novel methylene blue derivatives with the ability of additional hydrogen bonding and/or additional cationic charges to study the substituents' effect on their activity/toxicity profiles and photophysical properties. Direct detection of singlet oxygen was performed at 1270 nm and the singlet oxygen quantum yields were determined. In suspensions with both, Gram-positive and Gram-negative bacteria, some derivatives were highly active upon illumination to inactivate S. aureus and E. coli up to 7 log10 steps (99.99999%) without inherent toxicities in the nonirradiated state. PMID:23509728

  19. Polarized Fine Structure in the Photoluminescence Excitation Spectrum of a Negatively Charged Quantum Dot

    NASA Astrophysics Data System (ADS)

    Ware, M. E.; Stinaff, E. A.; Gammon, D.; Doty, M. F.; Bracker, A. S.; Gershoni, D.; Korenev, V. L.; Bădescu, Ş. C.; Lyanda-Geller, Y.; Reinecke, T. L.

    2005-10-01

    We report polarized photoluminescence excitation spectroscopy of the negative trion in single charge-tunable InAs/GaAs quantum dots. The spectrum exhibits a p-shell resonance with polarized fine structure arising from the direct excitation of the electron spin triplet states. The energy splitting arises from the axially symmetric electron-hole exchange interaction. The magnitude and sign of the polarization are understood from the spin character of the triplet states and a small amount of quantum dot asymmetry, which mixes the wave functions through asymmetric e-e and e-h exchange interactions.

  20. Polarized fine structure in the photoluminescence excitation spectrum of a negatively charged quantum dot.

    PubMed

    Ware, M E; Stinaff, E A; Gammon, D; Doty, M F; Bracker, A S; Gershoni, D; Korenev, V L; Bădescu, S C; Lyanda-Geller, Y; Reinecke, T L

    2005-10-21

    We report polarized photoluminescence excitation spectroscopy of the negative trion in single charge-tunable quantum dots. The spectrum exhibits a p-shell resonance with polarized fine structure arising from the direct excitation of the electron spin triplet states. The energy splitting arises from the axially symmetric electron-hole exchange interaction. The magnitude and sign of the polarization are understood from the spin character of the triplet states and a small amount of quantum dot asymmetry, which mixes the wave functions through asymmetric e-e and e-h exchange interactions.

  1. Role of protein surface charge in monellin sweetness.

    PubMed

    Xue, Wei-Feng; Szczepankiewicz, Olga; Thulin, Eva; Linse, Sara; Carey, Jannette

    2009-03-01

    A small number of proteins have the unusual property of tasting intensely sweet. Despite many studies aimed at identifying their sweet taste determinants, the molecular basis of protein sweetness is not fully understood. Recent mutational studies of monellin have implicated positively charged residues in sweetness. In the present work, the effect of overall net charge was investigated using the complementary approach of negative charge alterations. Multiple substitutions of Asp/Asn and Glu/Gln residues radically altered the surface charge of single-chain monellin by removing six negative charges or adding four negative charges. Biophysical characterization using circular dichroism, fluorescence, and two-dimensional NMR demonstrates that the native fold of monellin is preserved in the variant proteins under physiological solution conditions although their stability toward chemical denaturation is altered. A human taste test was employed to determine the sweetness detection threshold of the variants. Removal of negative charges preserves monellin sweetness, whereas added negative charge has a large negative impact on sweetness. Meta-analysis of published charge variants of monellin and other sweet proteins reveals a general trend toward increasing sweetness with increasing positive net charge. Structural mapping of monellin variants identifies a hydrophobic surface predicted to face the receptor where introduced positive or negative charge reduces sweetness, and a polar surface where charges modulate long-range electrostatic complementarity.

  2. Nanoparticle coagulation in fractionally charged and charge fluctuating dusty plasmas

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Nunomura, Shota; Kondo, Michio; Shiratani, Masaharu

    2008-08-15

    The kinetics of nanoparticle coagulation has been studied in fractionally charged and charge fluctuating dusty plasmas. The coagulation occurs when the mutual collision frequency among nanoparticles exceeds their charging and decharging/neutralization frequency. Interestingly, the coagulation is suppressed while a fraction (several percent) of nanoparticles are negatively charged in a plasma, in which stochastic charging plays an important role. A model is developed to predict a phase diagram of the coagulation and its suppression.

  3. Redesign of negatively charged 111In-DTPA-octreotide derivative to reduce renal radioactivity.

    PubMed

    Oshima, Nobuhiro; Akizawa, Hiromichi; Kawashima, Hidekazu; Zhao, Songji; Zhao, Yan; Nishijima, Ken-Ichi; Kitamura, Yoji; Arano, Yasushi; Kuge, Yuji; Ohkura, Kazue

    2017-05-01

    Radiolabeled octreotide derivatives have been studied as diagnostic and therapeutic agents for somatostatin receptor-positive tumors. To prevent unnecessary radiation exposure during their clinical application, the present study aimed to develop radiolabeled peptides which could reduce radioactivity levels in the kidney at both early and late post-injection time points by introducing a negative charge with an acidic amino acid such as L-aspartic acid (Asp) at a suitable position in 111 In-DTPA-conjugated octreotide derivatives. Biodistribution of the radioactivity was evaluated in normal mice after administration of a novel radiolabeled peptide by a counting method. The radiolabeled species remaining in the kidney were identified by comparing their HPLC data with those obtained by alternative synthesis. The designed and synthesized radiolabeled peptide 111 In-DTPA-d-Phe -1 -Asp 0 -d-Phe 1 -octreotide exhibited significantly lower renal radioactivity levels than those of the known 111 In-DTPA-d-Phe 1 -octreotide at 3 and 24h post-injection. The radiolabeled species in the kidney at 24h after the injection of new octreotide derivative represented 111 In-DTPA-d-Phe-OH and 111 In-DTPA-d-Phe-Asp-OH as the metabolites. Their radiometabolites and intact 111 In-DTPA-conjugated octreotide derivative were observed in urine within 24h post-injection. The present study provided a new example of an 111 In-DTPA-conjugated octreotide derivative having the characteristics of both reduced renal uptake and shortened residence time of radioactivity in the kidney. It is considered that this kinetic control was achieved by introducing a negative charge on the octreotide derivative thereby suppressing the reabsorption in the renal tubules and affording the radiometabolites with appropriate lipophilicity. Copyright © 2017 Elsevier Inc. All rights reserved.

  4. Like-charge attraction and opposite-charge decomplexation between polymers and DNA molecules

    NASA Astrophysics Data System (ADS)

    Buyukdagli, Sahin

    2017-02-01

    We scrutinize the effect of polyvalent ions on polymer-DNA interactions. We extend a recently developed test-charge theory [S. Buyukdagli et al., Phys. Rev. E 94, 042502 (2016), 10.1103/PhysRevE.94.042502] to the case of a stiff polymer interacting with a DNA molecule in an electrolyte mixture. The theory accounts for one-loop level electrostatic correlation effects such as the ionic cloud deformation around the strongly charged DNA molecule as well as image-charge forces induced by the low DNA permittivity. Our model can reproduce and explain various characteristics of the experimental phase diagrams for polymer solutions. First, the addition of polyvalent cations to the electrolyte solution results in the attraction of the negatively charged polymer by the DNA molecule. The glue of the like-charge attraction is the enhanced shielding of the polymer charges by the dense counterion layer at the DNA surface. Second, through the shielding of the DNA-induced electrostatic potential, mono- and polyvalent cations of large concentration both suppress the like-charge attraction. Within the same formalism, we also predict a new opposite-charge repulsion effect between the DNA molecule and a positively charged polymer. In the presence of polyvalent anions such as sulfate or phosphate, their repulsion by the DNA charges leads to the charge screening deficiency of the region around the DNA molecule. This translates into a repulsive force that results in the decomplexation of the polymer from DNA. This opposite-charge repulsion phenomenon can be verified by current experiments and the underlying mechanism can be beneficial to gene therapeutic applications where the control over polymer-DNA interactions is the key factor.

  5. On the Control of the Fixed Charge Densities in Al2O3-Based Silicon Surface Passivation Schemes.

    PubMed

    Simon, Daniel K; Jordan, Paul M; Mikolajick, Thomas; Dirnstorfer, Ingo

    2015-12-30

    A controlled field-effect passivation by a well-defined density of fixed charges is crucial for modern solar cell surface passivation schemes. Al2O3 nanolayers grown by atomic layer deposition contain negative fixed charges. Electrical measurements on slant-etched layers reveal that these charges are located within a 1 nm distance to the interface with the Si substrate. When inserting additional interface layers, the fixed charge density can be continuously adjusted from 3.5 × 10(12) cm(-2) (negative polarity) to 0.0 and up to 4.0 × 10(12) cm(-2) (positive polarity). A HfO2 interface layer of one or more monolayers reduces the negative fixed charges in Al2O3 to zero. The role of HfO2 is described as an inert spacer controlling the distance between Al2O3 and the Si substrate. It is suggested that this spacer alters the nonstoichiometric initial Al2O3 growth regime, which is responsible for the charge formation. On the basis of this charge-free HfO2/Al2O3 stack, negative or positive fixed charges can be formed by introducing additional thin Al2O3 or SiO2 layers between the Si substrate and this HfO2/Al2O3 capping layer. All stacks provide very good passivation of the silicon surface. The measured effective carrier lifetimes are between 1 and 30 ms. This charge control in Al2O3 nanolayers allows the construction of zero-fixed-charge passivation layers as well as layers with tailored fixed charge densities for future solar cell concepts and other field-effect based devices.

  6. Radiation transport codes for potential applications related to radiobiology and radiotherapy using protons, neutrons, and negatively charged pions

    NASA Technical Reports Server (NTRS)

    Armstrong, T. W.

    1972-01-01

    Several Monte Carlo radiation transport computer codes are used to predict quantities of interest in the fields of radiotherapy and radiobiology. The calculational methods are described and comparisions of calculated and experimental results are presented for dose distributions produced by protons, neutrons, and negatively charged pions. Comparisons of calculated and experimental cell survival probabilities are also presented.

  7. Physico-chemical studies on the interaction of dendrimers with lipid bilayers. 1. Effect of dendrimer generation and liposome surface charge.

    PubMed

    Roy, Biplab; Panda, Amiya Kumar; Parimi, Srinivas; Ametov, Igor; Barnes, Timothy; Prestidge, Clive A

    2014-01-01

    Studies on the interaction of different generation poly (amido amine) (PAMAM) dendrimers (2G, 4G and 6G) and liposomes of different compositions were carried out by a combined turbidity, dynamic light scattering and atomic force microscopic measurements. Liposomes comprising soy lecithin (SLC, negative surface charge), 1, 2-palmitoyl-sn-glycero-3-phosphatidylcholine (DPPC, mildly positive surface charge), 1,2-dipalmitoyl-sn-glycero-3-phospho-(1'-rac-glycerol (DPPG, negatively charged) and a biologically simulated mixture of DPPC + DPPG (7:3, M/M, negatively charged) were used as model bilayers. 30 wt% cholesterol was used in each combination as it is known to control the fluidity of membrane bilayers. Silica was used as a negatively charged hard sphere model with an aim to compare the results. Both the turbidity and hydrodynamic diameter values of all the liposomes, except DPPC, passed through maxima upon the progressive addition of PAMAM; the effect was insignificant in case of DPPC. Formation of dendriosome, a complex formed between dendrimer and liposome, resulted in the charge reversal of the negatively charged liposomes. Interaction between PAMAM and liposome was found to be governed by electrostatic as well as hydrogen bonding. Generation dependent PAMAM activity followed the order: 6G >4G>2G in terms of overall dendrimer concentration. However, interestingly, the order was reverse when PAMAM activity was considered in terms of total end group concentrations. AFM studies reveal the rupture of bilayer structure upon addition of dendrimer.

  8. New effects of a long-lived negatively charged massive particle on big bang nucleosynthesis

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Kusakabe, Motohiko; Kim, K. S.; Cheoun, Myung-Ki

    Primordial {sup 7}Li abundance inferred from observations of metal-poor stars is a factor of about 3 lower than the theoretical value of standard big bang nucleosynthesis (BBN) model. One of the solutions to the Li problem is {sup 7}Be destruction during the BBN epoch caused by a long-lived negatively charged massive particle, X{sup −}. The particle can bind to nuclei, and X-bound nuclei (X-nuclei) can experience new reactions. The radiative X{sup −} capture by {sup 7}Be nuclei followed by proton capture of the bound state of {sup 7}Be and X{sup −} ({sup 7}Be{sub x}) is a possible {sup 7}Be destructionmore » reaction. Since the primordial abundance of {sup 7}Li originates mainly from {sup 7}Li produced via the electron capture of {sup 7}Be after BBN, the {sup 7}Be destruction provides a solution to the {sup 7}Li problem. We suggest a new route of {sup 7}Be{sub x} formation, that is the {sup 7}Be charge exchange at the reaction of {sup 7}Be{sup 3+} ion and X{sup −}. The formation rate depends on the ionization fraction of {sup 7}Be{sup 3+} ion, the charge exchange cross section of {sup 7}Be{sup 3+}, and the probability that excited states {sup 7}Be{sub x}* produced at the charge exchange are converted to the ground state. We find that this reaction can be equally important as or more important than ordinary radiative recombination of {sup 7}Be and X{sup −}. The effect of this new route is shown in a nuclear reaction network calculation.« less

  9. Strategies of Pre-Service Primary School Teachers for Solving Addition Problems with Negative Numbers

    ERIC Educational Resources Information Center

    Almeida, Rut; Bruno, Alicia

    2014-01-01

    This paper analyses the strategies used by pre-service primary school teachers for solving simple addition problems involving negative numbers. The findings reveal six different strategies that depend on the difficulty of the problem and, in particular, on the unknown quantity. We note that students use negative numbers in those problems they find…

  10. Spectroscopic and calorimetric investigations on the influence of calcium ions on the polyamine negatively charged phospholipid molecular interactions

    NASA Astrophysics Data System (ADS)

    Bertoluzza, Alessandro; Bonora, S.; Fini, G.; Morelli, M. A.

    1993-06-01

    Polyamines do not interact with neutral phospholipids (phosphatidylcholines) but they do interact in the presence of bivalent and trivalent cations. The effect of polyvalent cations is explained in terms of dehydration of the bilayer surface. Polyamines interact strongly with negatively charged phospholipids; the presence of bivalent and trivalent cations do not change sensitively the type of interaction between polyamines and phosphatidic acids.

  11. Effect of negatively charged cellulose nanofibers on the dispersion of hydroxyapatite nanoparticles for scaffolds in bone tissue engineering.

    PubMed

    Park, Minsung; Lee, Dajung; Shin, Sungchul; Hyun, Jinho

    2015-06-01

    Nanofibrous 2,2,6,6-tetramethylpiperidine-1-oxyl(TEMPO)-oxidized bacterial cellulose (TOBC) was used as a dispersant of hydroxyapatite (HA) nanoparticles in aqueous solution. The surfaces of TOBC nanofibers were negatively charged after the reaction with the TEMPO/NaBr/NaClO system at pH 10 and room temperature. HA nanoparticles were simply adsorbed on the TOBC nanofibers (HA-TOBC) and dispersed well in DI water. The well-dispersed HA-TOBC colloidal solution formed a hydrogel after the addition of gelatin, followed by crosslinking with glutaraldehyde (HA-TOBC-Gel). The chemical modification of the fiber surfaces and the colloidal stability of the dispersion solution confirmed TOBC as a promising HA dispersant. Both the Young's modulus and maximum tensile stress increased as the amount of gelatin increased due to the increased crosslinking of gelatin. In addition, the well-dispersed HA produced a denser scaffold structure resulting in the increase of the Young's modulus and maximum tensile stress. The well-developed porous structures of the HA-TOBC-Gel composites were incubated with Calvarial osteoblasts. The HA-TOBC-Gel significantly improved cell proliferation as well as cell differentiation confirming the material as a potential candidate for use in bone tissue engineering scaffolds. Copyright © 2015 Elsevier B.V. All rights reserved.

  12. Geoengineering with Charged Droplets

    NASA Astrophysics Data System (ADS)

    Gokturk, H.

    2011-12-01

    Water molecules in a droplet are held together by intermolecular forces generated by hydrogen bonding which has a bonding energy of only about 0.2 eV. One can create a more rugged droplet by using an ion as a condensation nucleus. In that case, water molecules are held together by the interaction between the ion and the dipole moments of the water molecules surrounding the ion, in addition to any hydrogen bonding. In this research, properties of such charged droplets were investigated using first principle quantum mechanical calculations. A molecule which exhibits positive electron affinity is a good candidate to serve as the ionic condensation nucleus, because addition of an electron to such a molecule creates an energetically more stable state than the neutral molecule. A good example is the oxygen molecule (O2) where energy of O2 negative (O2-) ion is lower than that of the neutral O2 by about 0.5 eV. Examples of other molecules which have positive electron affinity include ozone (O3), nitrogen dioxide (NO2) and sulfur oxides (SOx, x=1-3). Atomic models used in the calculations consisted of a negative ion of one of the molecules mentioned above surrounded by water molecules. Calculations were performed using the DFT method with B3LYP hybrid functional and Pople type basis sets with polarization and diffuse functions. Energy of interaction between O2- ion and the water molecule was found to be ~0.7 eV. This energy is an order of magnitude greater than the thermal energy of even the highest temperatures encountered in the atmosphere. Once created, charged rugged droplets can survive in hot and dry climates where they can be utilized to create humidity and precipitation. The ion which serves as the nucleus of the droplet can attract not only water molecules but also other dipolar gases in the atmosphere. Such dipolar gases include industrial pollutants, for example nitrogen dioxide (NO2) or sulfur dioxide (SO2). Energy of interaction between O2- ion and pollutant

  13. Describing long-range charge-separation processes with subsystem density-functional theory

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Solovyeva, Alisa; Neugebauer, Johannes, E-mail: j.neugebauer@uni-muenster.de; Pavanello, Michele, E-mail: m.pavanello@rutgers.edu

    2014-04-28

    Long-range charge-transfer processes in extended systems are difficult to describe with quantum chemical methods. In particular, cost-effective (non-hybrid) approximations within time-dependent density functional theory (DFT) are not applicable unless special precautions are taken. Here, we show that the efficient subsystem DFT can be employed as a constrained DFT variant to describe the energetics of long-range charge-separation processes. A formal analysis of the energy components in subsystem DFT for such excitation energies is presented, which demonstrates that both the distance dependence and the long-range limit are correctly described. In addition, electronic couplings for these processes as needed for rate constants inmore » Marcus theory can be obtained from this method. It is shown that the electronic structure of charge-separated states constructed by a positively charged subsystem interacting with a negatively charged one is difficult to converge — charge leaking from the negative subsystem to the positive one can occur. This problem is related to the delocalization error in DFT and can be overcome with asymptotically correct exchange–correlation (XC) potentials or XC potentials including a sufficiently large amount of exact exchange. We also outline an approximate way to obtain charge-transfer couplings between locally excited and charge-separated states.« less

  14. Enhanced performance of Zn(II)-doped lead-acid batteries with electrochemical active carbon in negative mass

    NASA Astrophysics Data System (ADS)

    Xiang, Jiayuan; Hu, Chen; Chen, Liying; Zhang, Dong; Ding, Ping; Chen, Dong; Liu, Hao; Chen, Jian; Wu, Xianzhang; Lai, Xiaokang

    2016-10-01

    The effect and mechanism of Zn(II) on improving the performances of lead-acid cell with electrochemical active carbon (EAC) in negative mass is investigated. The hydrogen evolution of the cell is significantly reduced due to the deposition of Zn on carbon surface and the increased porosity of negative mass. Zn(II) additives can also improve the low-temperature and high-rate capacities of the cell with EAC in negative mass, which ascribes to the formation of Zn on lead and carbon surface that constructs a conductive bridge among the active mass. Under the co-contribution of EAC and Zn(II), the partial-state-of-charge cycle life is greatly prolonged. EAC optimizes the NAM structure and porosity to enhance the charge acceptance and retard the lead sulfate accumulation. Zn(II) additive reduces the hydrogen evolution during charge process and improves the electric conductivity of the negative electrode. The cell with 0.6 wt% EAC and 0.006 wt% ZnO in negative mass exhibits 90% reversible capacity of the initial capacity after 2100 cycles. In contrast, the cell with 0.6 wt% EAC exhibits 84% reversible capacity after 2100 cycles and the control cell with no EAC and Zn(II) exhibits less than 80% reversible capacity after 1350 cycles.

  15. The surface charge of trypanosomatids.

    PubMed

    Souto-Padrón, Thaïs

    2002-12-01

    The surface charge of trypanosomatids was evaluated by means of the binding of cationic particles, as visualized by electron microscopy and by direct measurements of the electrophoretic mobility of cells. The results obtained indicate that most of the trypanosomatids exhibit a negatively charged surface whose value is species specific and varies according to the developmental stages. Sialic acids associated with glycoproteins, glycolipids and phosphate groups are the major components responsible for the net negative surface charge of the trypanosomatids.

  16. Charge transfer in TATB and HMX under extreme conditions.

    PubMed

    Zhang, Chaoyang; Ma, Yu; Jiang, Daojian

    2012-11-01

    Charge transfer is usually accompanied by structural changes in materials under different conditions. However, the charge transfer in energetic materials that are subjected to extreme conditions has seldom been explored by researchers. In the work described here, the charge transfer in single molecules and unit cells of the explosives TATB and HMX under high temperatures and high pressures was investigated by performing static and dynamic calculations using three DFT methods, including the PWC functional of LDA, and the BLYP and PBE functionals of GGA. The results showed that negative charge is transferred from the nitro groups of molecular or crystalline TATB and HMX when they are heated. All DFT calculations for the compressed TATB unit cell indicate that, generally, negative charge transfer occurs to its nitro groups as the compression increases. PWC and PBE calculations for crystalline HMX show that negative charge is first transferred to the nitro groups but, as the compression increases, the negative charge is transferred from the nitro groups. However, the BLYP calculations indicated that there was gradual negative charge transfer to the nitro groups of HMX, similar to the case for TATB. The unrelaxed state of the uniformly compressed TATB causes negative charge to be transferred from its nitro groups, in contrast to what is seen in the relaxed state. Charge transfer in TATB is predicted to occur much more easily than in HMX.

  17. Video, LMA and ULF observations of a negative gigantic jet in North Texas

    NASA Astrophysics Data System (ADS)

    Bruning, E. C.; Cummer, S.; Palivec, K.; Lyons, W. A.; Chmielewski, V.; MacGorman, D. R.

    2017-12-01

    On 8 September 2016 at 0125:38 UTC video of a negative gigantic jet was captured from Hawley, TX. VHF Lightning Mapping Arrays in West Texas and Oklahoma also observed the parent flash (duration of about 1 s) and, for the first time, mapped dozens of points along ascending negative leaders, lasting about 50 ms, which extended well above cloud top to about 35 km MSL altitude. A few well-located VHF sources were also detected near 50 km. Together, the video and VHF observations provide additional confirmation of the altitude at which the leader-to-streamer transition takes place in gigantic jet discharges. ULF magnetic field data from the Duke iCMC network show a current excursion associated with the onset of the upward movement of negative charge and leaders in the VHF. As the gigantic jet reached its full height, current spiked to 80 kA, followed by several hundred milliseconds of continuing current of 10-20 kA. Total charge moment change was about 6000 C km. The storm complex produced predominantly negative large charge moment change events, which is characteristic of storms that produce negative gigantic jets.

  18. Activation energy of negative fixed charges in thermal ALD Al{sub 2}O{sub 3}

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Kühnhold-Pospischil, S.; Institute of Physical Chemistry, Albert-Ludwigs-Universität Freiburg, Albertstr. 21, 79104 Freiburg; Freiburg Materials Research Center FMF, Albert-Ludwigs-Universität Freiburg, Stefan-Meier-Str. 21, 79104 Freiburg

    2016-08-08

    A study of the thermally activated negative fixed charges Q{sub tot} and the interface trap densities D{sub it} at the interface between Si and thermal atomic-layer-deposited amorphous Al{sub 2}O{sub 3} layers is presented. The thermal activation of Q{sub tot} and D{sub it} was conducted at annealing temperatures between 220 °C and 500 °C for durations between 3 s and 38 h. The temperature-induced differences in Q{sub tot} and D{sub it} were measured using the characterization method called corona oxide characterization of semiconductors. Their time dependency were fitted using stretched exponential functions, yielding activation energies of E{sub A} = (2.2 ± 0.2) eV and E{submore » A} = (2.3 ± 0.7) eV for Q{sub tot} and D{sub it}, respectively. For annealing temperatures from 350 °C to 500 °C, the changes in Q{sub tot} and D{sub it} were similar for both p- and n-type doped Si samples. In contrast, at 220 °C the charging process was enhanced for p-type samples. Based on the observations described in this contribution, a charging model leading to Q{sub tot} based on an electron hopping process between the silicon and Al{sub 2}O{sub 3} through defects is proposed.« less

  19. A thundercloud electric field sounding - Charge distribution and lightning

    NASA Technical Reports Server (NTRS)

    Weber, M. E.; Few, A. A.; Stewart, M. F.; Christian, H. J.

    1982-01-01

    An instrumented free balloon measured electric fields and field changes as it rose through a thundercloud above Langmuir Laboratory, New Mexico. The variation of the electric field with altitude implied that the cloud contained negative space charge of density -0.6 to -4 nC/cu m between 5.5 and 8.0 km MSL. The environmental temperature at these levels ranged from -5 to -20 C. The measurements imply that the areal extent of this negative charge center was significantly greater than that of the cloud's intense precipitation shafts. At altitudes greater than 8 km, the instrument ascended past net positive charge. In addition, positive space charge adjacent to the earth's surface (concentration 0.6 nC/cu m and in the lowest portion of the cloud (1.0 nC/cu m) is inferred from the measurements. Electric field changes from intracloud lightning were interpreted by using a simple model for the developing streamer of the initial phase. Thunder source reconstructions provided estimates for the orientation of lightning channels. Seven 'streamers' so analyzed propagated on the average, at 50,000 m/s and carried a current of 390 A. The mean charge dissipated during a flash was 30 C.

  20. Vertical Charge Transport and Negative Transconductance in Multilayer Molybdenum Disulfides.

    PubMed

    Liu, Yuan; Guo, Jian; He, Qiyuan; Wu, Hao; Cheng, Hung-Chieh; Ding, Mengning; Shakir, Imran; Gambin, Vincent; Huang, Yu; Duan, Xiangfeng

    2017-09-13

    Negative transconductance (NTC) devices have been heavily investigated for their potential in low power logical circuit, memory, oscillating, and high-speed switching applications. Previous NTC devices are largely attributed to two working mechanisms: quantum mechanical tunneling, and mobility degradation at high electrical field. Herein we report a systematic investigation of charge transport in multilayer two-dimensional semiconductors (2DSCs) with optimized van der Waals contact and for the first time demonstrate NTC and antibipolar characteristics in multilayer 2DSCs (such as MoS 2 , WSe 2 ). By varying the measurement temperature, bias voltage, and body thickness, we found the NTC behavior can be attributed to a vertical potential barrier in the multilayer 2DSCs and the competing mechanisms between intralayer lateral transport and interlayer vertical transport, thus representing a new working mechanism for NTC operation. Importantly, this vertical potential barrier arises from inhomogeneous carrier distribution in 2DSC from the near-substrate region to the bulk region, which is in contrast to conventional semiconductors with homogeneous doping defined by bulk dopants. We further show that the unique NTC behavior can be explored for creating frequency doublers and phase shift keying circuits with only one transistor, greatly simplifying the circuit design compared to conventional technology.

  1. Modeling the Electric Potential and Surface Charge Density Near Charged Thunderclouds

    NASA Astrophysics Data System (ADS)

    Neel, Matthew Stephen

    2018-03-01

    Thundercloud charge separation, or the process by which the bottom portion of a cloud gathers charge and the top portion of the cloud gathers the opposite charge, is still not thoroughly understood. Whatever the mechanism, though, a charge separation definitely exists and can lead to electrostatic discharge via cloud-to-cloud lightning and cloud-to-ground lightning. We wish to examine the latter form, in which upward leaders from Earth connect with downward leaders from the cloud to form a plasma channel and produce lightning. Much of the literature indicates that the lower part of a thundercloud becomes negatively charged while the upper part becomes positively charged via convective charging, although the opposite polarity can certainly exist along with various, complex intra-cloud currents. It is estimated that >90% of cloud-to-ground lightning is "negative lightning," or the flow of charges from the bottom of the cloud, while the remaining <10% of lightning strikes is "positive lightning," or the flow of charges from the top of the cloud. We wish to understand the electric potential surrounding charged thunderclouds as well as the resulting charge density on the surface of Earth below them. In this paper we construct a simple and adaptable model that captures the very basic features of the cloud/ground system and that exhibits conditions favorable for both forms of lightning. In this way, we provide a practical application of electrostatic dipole physics as well as the method of images that can serve as a starting point for further modeling and analysis by students.

  2. Maximization of DRAM yield by control of surface charge and particle addition during high dose implantation

    NASA Astrophysics Data System (ADS)

    Horvath, J.; Moffatt, S.

    1991-04-01

    Ion implantation processing exposes semiconductor devices to an energetic ion beam in order to deposit dopant ions in shallow layers. In addition to this primary process, foreign materials are deposited as particles and surface films. The deposition of particles is a major cause of IC yield loss and becomes even more significant as device dimensions are decreased. Control of particle addition in a high-volume production environment requires procedures to limit beamline and endstation sources, control of particle transport, cleaning procedures and a well grounded preventative maintenance philosophy. Control of surface charge by optimization of the ion beam and electron shower conditions and measurement with a real-time charge sensor has been effective in improving the yield of NMOS and CMOS DRAMs. Control of surface voltages to a range between 0 and -20 V was correlated with good implant yield with PI9200 implanters for p + and n + source-drain implants.

  3. Survey of International Space Station Charging Events

    NASA Technical Reports Server (NTRS)

    Craven, P. D.; Wright, Kenneth H., Jr.; Minow, Joseph I.; Coffey, Victoria N.; Schneider, Todd A.; Vaughn, Jason A.; Ferguson, Dale C.; Parker, Linda N.

    2009-01-01

    With the negative grounding of the 160V Photovoltaic (PV) arrays, the International Space Station (ISS) can experience varied and interesting charging events. Since August 2006, there has been a multi-probe p ackage, called the Floating Potential Measurement Unit (FPMU), availa ble to provide redundant measurements of the floating potential of th e ISS as well as the density and temperature of the local plasma environment. The FPMU has been operated during intermittent data campaigns since August 2006 and has collected over 160 days of information reg arding the charging of the ISS as it has progressed in configuration from one to three PV arrays and with various additional modules such as the European Space Agency?s Columbus laboratory and the Japan Aeros pace Exploration Agency's Kibo laboratory. This paper summarizes the charging of the ISS and the local environmental conditions that contr ibute to those charging events, both as measured by the FPMU.

  4. Spontaneous charged lipid transfer between lipid vesicles.

    PubMed

    Richens, Joanna L; Tyler, Arwen I I; Barriga, Hanna M G; Bramble, Jonathan P; Law, Robert V; Brooks, Nicholas J; Seddon, John M; Ces, Oscar; O'Shea, Paul

    2017-10-03

    An assay to study the spontaneous charged lipid transfer between lipid vesicles is described. A donor/acceptor vesicle system is employed, where neutrally charged acceptor vesicles are fluorescently labelled with the electrostatic membrane probe Fluoresceinphosphatidylethanolamine (FPE). Upon addition of charged donor vesicles, transfer of negatively charged lipid occurs, resulting in a fluorescently detectable change in the membrane potential of the acceptor vesicles. Using this approach we have studied the transfer properties of a range of lipids, varying both the headgroup and the chain length. At the low vesicle concentrations chosen, the transfer follows a first-order process where lipid monomers are transferred presumably through the aqueous solution phase from donor to acceptor vesicle. The rate of transfer decreases with increasing chain length which is consistent with energy models previously reported for lipid monomer vesicle interactions. Our assay improves on existing methods allowing the study of a range of unmodified lipids, continuous monitoring of transfer and simplified experimental procedures.

  5. Electronic structure of negative charge transfer CaFeO3 across the metal-insulator transition

    NASA Astrophysics Data System (ADS)

    Rogge, Paul C.; Chandrasena, Ravini U.; Cammarata, Antonio; Green, Robert J.; Shafer, Padraic; Lefler, Benjamin M.; Huon, Amanda; Arab, Arian; Arenholz, Elke; Lee, Ho Nyung; Lee, Tien-Lin; Nemšák, Slavomír; Rondinelli, James M.; Gray, Alexander X.; May, Steven J.

    2018-01-01

    We investigated the metal-insulator transition for epitaxial thin films of the perovskite CaFeO3, a material with a significant oxygen ligand hole contribution to its electronic structure. We find that biaxial tensile and compressive strain suppress the metal-insulator transition temperature. By combining hard x-ray photoelectron spectroscopy, soft x-ray absorption spectroscopy, and density functional calculations, we resolve the element-specific changes to the electronic structure across the metal-insulator transition. We demonstrate that the Fe sites undergo no observable spectroscopic change between the metallic and insulating states, whereas the O electronic configuration undergoes significant changes. This strongly supports the bond-disproportionation model of the metal-insulator transition for CaFeO3 and highlights the importance of ligand holes in its electronic structure. By sensitively measuring the ligand hole density, however, we find that it increases by ˜5 -10 % in the insulating state, which we ascribe to a further localization of electron charge on the Fe sites. These results provide detailed insight into the metal-insulator transition of negative charge transfer compounds and should prove instructive for understanding metal-insulator transitions in other late transition metal compounds such as the nickelates.

  6. Human fibrinogen adsorption on positively charged latex particles.

    PubMed

    Zeliszewska, Paulina; Bratek-Skicki, Anna; Adamczyk, Zbigniew; Cieśla, Michał

    2014-09-23

    Fibrinogen (Fb) adsorption on positively charged latex particles (average diameter of 800 nm) was studied using the microelectrophoretic and the concentration depletion methods based on AFM imaging. Monolayers on latex were adsorbed from diluted bulk solutions at pH 7.4 and an ionic strength in the range of 10(-3) to 0.15 M where fibrinogen molecules exhibited an average negative charge. The electrophoretic mobility of the latex after controlled fibrinogen adsorption was systematically measured. A monotonic decrease in the electrophoretic mobility of fibrinogen-covered latex was observed for all ionic strengths. The results of these experiments were interpreted according to the three-dimensional electrokinetic model. It was also determined using the concentration depletion method that fibrinogen adsorption was irreversible and the maximum coverage was equal to 0.6 mg m(-2) for ionic strength 10(-3) M and 1.3 mg m(-2) for ionic strength 0.15 M. The increase of the maximum coverage was confirmed by theoretical modeling based on the random sequential adsorption approach. Paradoxically, the maximum coverage of fibrinogen on positively charged latex particles was more than two times lower than the maximum coverage obtained for negative latex particles (3.2 mg m(-2)) at pH 7.4 and ionic strength of 0.15 M. This was interpreted as a result of the side-on adsorption of fibrinogen molecules with their negatively charged core attached to the positively charged latex surface. The stability and acid base properties of fibrinogen monolayers on latex were also determined in pH cycling experiments where it was observed that there were no irreversible conformational changes in the fibrinogen monolayers. Additionally, the zeta potential of monolayers was more positive than the zeta potential of fibrinogen in the bulk, which proves a heterogeneous charge distribution. These experimental data reveal a new, side-on adsorption mechanism of fibrinogen on positively charged surfaces and

  7. Electrokinetic Response of Charge-Selective Nanostructured Polymeric Membranes

    NASA Astrophysics Data System (ADS)

    Schiffbauer, Jarrod; Li, Diya; Gao, Feng; Phillip, William; Chang, Hsueh-Chia

    2017-11-01

    Nanostructured polymeric membranes, with a tunable pore size and ease of surface molecular functionalization, are a promising material for separations, filtration, and sensing applications. Recently, such membranes have been fabricated wherein the ion selectivity is imparted by self-assembled functional groups through a two-step process. Amine groups are used to provide a positive surface charge and acid groups are used to yield a negative charge. The membranes can be fabricated as either singly-charged or patterned/mosaic membranes, where there are alternating regions of amine- lined or acid-lined pores. We demonstrate that such membranes, in addition to having many features in common with other charge selective membranes (i.e. AMX or Nafion), display a unique single-membrane rectification behavior. This is due to the asymmetric distribution of charged functional groups during the fabrication process. We demonstrate this rectification effect using both dc current-voltage characteristics as well as dc-biased electrical impedance spectroscopy. Furthermore, surface charge changes due to dc concentration polarization and generation of localized pH shifts are monitored using electrical impedance spectroscopy. (formerly at University of Notre Dame).

  8. Effect of Fe{sub 3}O{sub 4} nanoparticles on space charge distribution in propylene carbonate under impulse voltage

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Sima, Wenxia, E-mail: cqsmwx@cqu.edu.cn; Song, He; Yang, Qing

    2015-12-15

    Addition of nanoparticles of the ferromagnetic material Fe{sub 3}O{sub 4} can increase the positive impulse breakdown voltage of propylene carbonate by 11.65%. To further investigate the effect of ferromagnetic nanoparticles on the space charge distribution in the discharge process, the present work set up a Kerr electro-optic field mapping measurement system using an array photodetector to carry out time-continuous measurement of the electric field and space charge distribution in propylene carbonate before and after modification. Test results show that fast electrons can be captured by Fe{sub 3}O{sub 4} nanoparticles and converted into relatively slow, negatively charged particles, inhibiting the generationmore » and transportation of the space charge, especially the negative space charge.« less

  9. Plantaricin A, a cationic peptide produced by Lactobacillus plantarum, permeabilizes eukaryotic cell membranes by a mechanism dependent on negative surface charge linked to glycosylated membrane proteins.

    PubMed

    Sand, Sverre L; Nissen-Meyer, Jon; Sand, Olav; Haug, Trude M

    2013-02-01

    Lactobacillus plantarum C11 releases plantaricin A (PlnA), a cationic peptide pheromone that has a membrane-permeabilizing, antimicrobial effect. We have previously shown that PlnA may also permeabilize eukaryotic cells, with a potency that differs between cell types. It is generally assumed that cationic antimicrobial peptides exert their effects through electrostatic attraction to negatively charged phospholipids in the membrane. The aim of the present study was to investigate if removal of the negative charge linked to glycosylated proteins at the cell surface reduces the permeabilizing potency of PlnA. The effects of PlnA were tested on clonal rat anterior pituitary cells (GH(4) cells) using patch clamp and microfluorometric techniques. In physiological extracellular solution, GH(4) cells are highly sensitive to PlnA, but the sensitivity was dramatically reduced in solutions that partly neutralize the negative surface charge of the cells, in agreement with the notion that electrostatic interactions are probably important for the PlnA effects. Trypsination of cells prior to PlnA exposure also rendered the cells less sensitive to the peptide, suggesting that negative charges linked to membrane proteins are involved in the permeabilizing action. Finally, pre-exposure of cells to a mixture of enzymes that split carbohydrate residues from the backbone of glycosylated proteins also impeded the PlnA-induced membrane permeabilization. We conclude that electrostatic attraction between PlnA and glycosylated membrane proteins is probably an essential first step before PlnA can interact with membrane phospholipids. Deviating glycosylation patterns may contribute to the variation in PlnA sensitivity of different cell types, including cancerous cells and their normal counterparts. Copyright © 2012 Elsevier B.V. All rights reserved.

  10. Ground-state oxygen holes and the metal–insulator transition in the negative charge-transfer rare-earth nickelates

    PubMed Central

    Bisogni, Valentina; Catalano, Sara; Green, Robert J.; Gibert, Marta; Scherwitzl, Raoul; Huang, Yaobo; Strocov, Vladimir N.; Zubko, Pavlo; Balandeh, Shadi; Triscone, Jean-Marc; Sawatzky, George; Schmitt, Thorsten

    2016-01-01

    The metal–insulator transition and the intriguing physical properties of rare-earth perovskite nickelates have attracted considerable attention in recent years. Nonetheless, a complete understanding of these materials remains elusive. Here we combine X-ray absorption and resonant inelastic X-ray scattering (RIXS) spectroscopies to resolve important aspects of the complex electronic structure of rare-earth nickelates, taking NdNiO3 thin film as representative example. The unusual coexistence of bound and continuum excitations observed in the RIXS spectra provides strong evidence for abundant oxygen holes in the ground state of these materials. Using cluster calculations and Anderson impurity model interpretation, we show that distinct spectral signatures arise from a Ni 3d8 configuration along with holes in the oxygen 2p valence band, confirming suggestions that these materials do not obey a conventional positive charge-transfer picture, but instead exhibit a negative charge-transfer energy in line with recent models interpreting the metal–insulator transition in terms of bond disproportionation. PMID:27725665

  11. Charge renormalization and inversion of a highly charged lipid bilayer: effects of dielectric discontinuities and charge correlations.

    PubMed

    Taheri-Araghi, Sattar; Ha, Bae-Yeun

    2005-08-01

    We reexamine the problem of charge renormalization and inversion of a highly charged surface of a low dielectric constant immersed in ionic solutions. To be specific, we consider an asymmetrically charged lipid bilayer, in which only one layer is negatively charged. In particular, we study how dielectric discontinuities and charge correlations (among lipid charges and condensed counterions) influence the effective charge of the surface. When counterions are monovalent (e.g., Na+), our mean-field approach implies that dielectric discontinuities can enhance counterion condensation. A simple scaling picture shows how the effects of dielectric discontinuities and surface-charge distributions are intertwined: Dielectric discontinuities diminish condensation if the backbone charge is uniformly smeared out while counterions are localized in space; they can, however, enhance condensation when the backbone charge is discrete. In the presence of asymmetric salts such as CaCl2 , we find that the correlation effect, treated at the Gaussian level, is more pronounced when the surface has a lower dielectric constant, inverting the sign of the charge at a smaller value of Ca2+ concentration.

  12. An Analysis of Two Thunderstorms Producing Five Negative Sprites on 12 September 2014

    NASA Astrophysics Data System (ADS)

    Boggs, L.; Liu, N.; Splitt, M. E.; Lazarus, S. M.; Cummer, S. A.; Rassoul, H.

    2015-12-01

    We present a detailed analysis of the thunderstorms and the parent lightning discharge morphologies of five confirmed negative sprites taking place in two different thunderstorms. These two thunderstorms took place in east-central and south Florida on 12 September 2014. We utilized several lightning location networks, remote magnetic field measurements, dual polarization radar, and balloon borne soundings in our analysis. Each parent discharge was immediately preceded by intra-cloud (IC) discharges between the mid-level negative and upper positive charge regions. This either allowed a second upward negative leader to escape the upper positive charge region, or encouraged a downward negative leader to be initiated and connect with ground. The discharges found in this study support the findings of Lu et al., 2012 [JGR,117, D04212, 2012] that negative sprite-parent lightning consists primarily of hybrid intra-cloud negative cloud-to-ground (IC-NCG) and bolt-from-the-blue (BFB) lightning. Our work finds these unique discharges form in thunderstorms that have an excess of mid-level negative charge and weakened upper positive charge. Due to this charge structure, these unusual discharges transfer more charge to the ground than typical negative cloud-to-ground discharges. Our study suggests that the key difference separating bolt-from-the-blue and gigantic jet discharges is an asymmetric charge structure. This acts to bring the negative leader exiting the thundercloud closer to the lateral positive screening layer, encouraging the negative leader to turn towards ground. This investigation reveals IC discharges that involve multiple convective cells and come to ground as a negative CG discharge, a breed of hybrid IC-NCG discharges, also transfer more negative charge to ground than typical negative CG discharges and are able to initiate negative sprites. From this work, the charge structures mentioned above resulted from tall, intense convective cells with low CG flash

  13. Porous composite with negative thermal expansion obtained by photopolymer additive manufacturing

    NASA Astrophysics Data System (ADS)

    Takezawa, Akihiro; Kobashi, Makoto; Kitamura, Mitsuru

    2015-07-01

    Additive manufacturing (AM) could be a novel method of fabricating composite and porous materials having various effective performances based on mechanisms of their internal geometries. Materials fabricated by AM could rapidly be used in industrial application since they could easily be embedded in the target part employing the same AM process used for the bulk material. Furthermore, multi-material AM has greater potential than usual single-material AM in producing materials with effective properties. Negative thermal expansion is a representative effective material property realized by designing a composite made of two materials with different coefficients of thermal expansion. In this study, we developed a porous composite having planar negative thermal expansion by employing multi-material photopolymer AM. After measurement of the physical properties of bulk photopolymers, the internal geometry was designed by topology optimization, which is the most effective structural optimization in terms of both minimizing thermal stress and maximizing stiffness. The designed structure was converted to a three-dimensional stereolithography (STL) model, which is a native digital format of AM, and assembled as a test piece. The thermal expansions of the specimens were measured using a laser scanning dilatometer. Negative thermal expansion corresponding to less than -1 × 10-4 K-1 was observed for each test piece of the N = 3 experiment.

  14. Detecting negative ions on board small satellites

    NASA Astrophysics Data System (ADS)

    Lepri, S. T.; Raines, J. M.; Gilbert, J. A.; Cutler, J.; Panning, M.; Zurbuchen, T. H.

    2017-04-01

    Recent measurements near comets, planets, and their satellites have shown that heavy ions, energetic neutral atoms, molecular ions, and charged dust contain a wealth of information about the origin, evolution, and interaction of celestial bodies with their space environment. Using highly sensitive plasma instruments, positively charged heavy ions have been used to trace exospheric and surface composition of comets, planets, and satellites as well as the composition of interplanetary and interstellar dust. While positive ions dominate throughout the heliosphere, negative ions are also produced from surface interactions. In fact, laboratory experiments have shown that oxygen released from rocky surfaces is mostly negatively charged. Negative ions and negatively charged nanograins have been detected with plasma electron analyzers in several different environments (e.g., by Cassini and Rosetta), though more extensive studies have been challenging without instrumentation dedicated to negative ions. We discuss an adaptation of the Fast Imaging Plasma Spectrometer (FIPS) flown on MErcury Surface, Space ENvironment, GEochemistry and Ranging (MESSENGER) for the measurement of negatively charged particles. MESSENGER/FIPS successfully measured the plasma environment of Mercury from 2011 until 2015, when the mission ended, and has been used to map multiple ion species (H+ through Na+ and beyond) throughout Mercury's space environment. Modifications to the existing instrument design fits within a 3U CubeSat volume and would provide a low mass, low power instrument, ideal for future CubeSat or distributed sensor missions seeking, for the first time, to characterize the contribution of negative particles in the heliospheric plasmas near the planets, moons, comets, and other sources.

  15. Intermetallic negative electrodes for non-aqueous lithium cells and batteries

    DOEpatents

    Thackeray, Michael M.; Vaughey, John T.; Johnson, Christopher S.; Fransson, Linda M.; Edstrom, Ester Kristina; Henriksen, Gary

    2004-05-04

    A method of operating an electrochemical cell is disclosed. The cell has an intermetallic negative electrode of Cu.sub.6-x M.sub.x Sn.sub.5, wherein x is .ltoreq.3 and M is one or more metals including Si and a positive electrode containing Li in which Li is shuttled between the positive electrode and the negative electrode during charge and discharge to form a lithiated intermetallic negative electrode during charge. The voltage of the electrochemical cell is controlled during the charge portion of the charge-discharge cycles so that the potential of the lithiated intermetallic negative electrode in the fully charged electrochemical cell is less than 0.2 V but greater than 0 V versus metallic lithium.

  16. Electrical control of optical orientation of neutral and negatively charged excitons in an n -type semiconductor quantum well

    NASA Astrophysics Data System (ADS)

    Dzhioev, R. I.; Korenev, V. L.; Lazarev, M. V.; Sapega, V. F.; Gammon, D.; Bracker, A. S.

    2007-01-01

    We report electric field induced increase of spin orientation of negatively charged excitons (trions) localized in n -type GaAs/AlGaAs quantum well. Under resonant excitation of free neutral heavy-hole excitons, the polarization of trions increases dramatically with electrical injection of electrons. The polarization enhancement correlates strongly with trion/exciton luminescence intensity ratio. This effect results from a very efficient trapping of free neutral excitons by the quantum well interfacial fluctuations (“natural” quantum dots) containing resident electrons.

  17. Interactions between similar and dissimilar charged interfaces in the presence of multivalent anions.

    PubMed

    Moazzami-Gudarzi, Mohsen; Adam, Pavel; Smith, Alexander M; Trefalt, Gregor; Szilágyi, István; Maroni, Plinio; Borkovec, Michal

    2018-04-04

    Direct force measurements involving amidine latex (AL) and sulfate latex (SL) particles in aqueous solutions containing multivalent ferrocyanide anions are presented. These measurements feature three different pairs of particles, namely SL-SL, AL-SL, and AL-AL. The force profiles are quantitatively interpreted in terms of the theory by Derjaguin, Landau, Verwey, and Overbeek (DLVO) that is combined with a short-ranged exponential attraction. In monovalent salt solutions, the AL particles are positively charged, while the SL particles are negatively charged. In solutions containing ferrocyanide, the charge of the AL particles is reversed as the concentration is increased. The longer-ranged component of all force profiles is fully compatible with DLVO theory, provided effects of charge regulation are included. At shorter distances, an additional exponential attraction must be introduced, whereby the respective decay length is about 2 nm for the AL-AL pair, and below 1 nm for the SL-SL pair. This non-DLVO force is intermediate for the asymmetric AL-SL pair. These additional forces are probably related to charge fluctuations, patch-charged interactions, or hydrophobic forces.

  18. On charging of snow particles in blizzard

    NASA Technical Reports Server (NTRS)

    Shio, Hisashi

    1991-01-01

    The causes of the charge polarity on the blizzard, which consisted of fractured snow crystals and ice particles, were investigated. As a result, the charging phenomena showed that the characteristics of the blizzard are as follows: (1) In the case of the blizzard with snowfall, the fractured snow particles drifting near the surface of snow field (lower area: height 0.3 m) had positive charge, while those drifting at higher area (height 2 m) from the surface of snow field had negative charge. However, during the series of blizzards two kinds of particles positively and negatively charged were collected in equal amounts in a Faraday Cage. It may be considered that snow crystals with electrically neutral properties were separated into two kinds of snow flakes (charged positively and negatively) by destruction of the snow crystals. (2) In the case of the blizzard which consisted of irregularly formed ice drops (generated by peeling off the hardened snow field), the charge polarity of these ice drops salting over the snow field was particularly controlled by the crystallographic characteristics of the surface of the snow field hardened by the powerful wind pressure.

  19. Fetuin mediates hepatic uptake of negatively charged nanoparticles via scavenger receptor.

    PubMed

    Nagayama, Susumu; Ogawara, Ken-ichi; Minato, Keiko; Fukuoka, Yoshiko; Takakura, Yoshinobu; Hashida, Mitsuru; Higaki, Kazutaka; Kimura, Toshikiro

    2007-02-01

    We tried to evaluate the possible involvement of fetuin in the scavenger receptors (SRs)-mediated hepatic uptake of polystyrene nanospheres with the size of 50 nm (NS-50), which has surface negative charge (zeta potential=-21.8+/-2.3 mV). The liver perfusion studies in rats revealed that the hepatic uptake of NS-50 pre-coated with fetuin (NS-50-fetuin) was significantly inhibited by poly inosinic acid (poly I), a typical inhibitor of SRs, whereas that of plain NS-50 or NS-50 pre-coated with BSA (NS-50-BSA) was not. The uptake of NS-50-fetuin by cultured Kupffer cells was also significantly inhibited by poly I, and anti-class A scavenger receptors (SR-A) antibody, suggesting that fetuin on NS-50 mediated the recognition and internalization of NS-50 by Kupffer cells and at least SR-A would be responsible for the uptake. Taken that Western blot analysis confirmed that fetuin certainly adsorbed on the surface of NS-50 after the incubation of NS-50 with serum, the results obtained in the present study indicate that fetuin would be one of the serum proteins that were substantially involved in the hepatic uptake of NS-50 via SRs.

  20. Measurement and control of electrostatic charges on solids in a gaseous suspension

    NASA Astrophysics Data System (ADS)

    Nieh, S.; Nguyen, T.

    1985-10-01

    Measurements of mean particle charges and charge distributions on Medium Volatile Bituminous (MVB) coals and Lignite A (LIGA) coals in a 51 mm ID grounded copper pipe loop have been made with the upgraded Faraday cage system. Both negative and positive charges were found for coals in all experiments. The dual polarities of charges are believed to be due to the nonuniform materials and chemical composition contained in coals. As expected, increasing velocity or decreasing air humidity has a significant effect to increase the mean particle charge and the standard deviation of distribution. Charge elimination by the addition of coal fines has been explored. Effective suppression of particle charges was achieved by adding 0.1% by mass of minus 1 micron coal dust into the pipe flow. A neutralization mechanism was proposed to interpret the measured results. The results of charge control obtained to date has been significant and encouraging. More work is needed to validate the proposed mechanism.

  1. Broad bandwidth vibration energy harvester based on thermally stable wavy fluorinated ethylene propylene electret films with negative charges

    NASA Astrophysics Data System (ADS)

    Zhang, Xiaoqing; Sessler, Gerhard M.; Ma, Xingchen; Xue, Yuan; Wu, Liming

    2018-06-01

    Wavy fluorinated ethylene propylene (FEP) electret films with negative charges were prepared by a patterning method followed by a corona charging process. The thermal stability of these films was characterized by the surface potential decay with annealing time at elevated temperatures. The results show that thermally stable electret films can be made by corona charging followed by pre-aging treatment. Vibration energy harvesters having a very simple sandwich structure, consisting of a central wavy FEP electret film and two outside metal plates, were designed and their performance, including the resonance frequency, output power, half power bandwidth, and device stability, was investigated. These harvesters show a broad bandwidth as well as high output power. Their performance can be further improved by using a wavy-shaped counter electrode. For an energy harvester with an area of 4 cm2 and a seismic mass of 80 g, the output power referred to 1 g (g is the gravity of the earth), the resonance frequency, and the 3 dB bandwidth are 1.85 mW, 90 Hz, and 24 Hz, respectively. The output power is sufficient to power some electronic devices. Such devices may be embedded in shoe soles, carpets or seat cushions where the flexibility is required and large force is available.

  2. Understanding Function and Performance of Carbon Additives in Lead-Acid Batteries

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Enos, D. G.; Ferreira, S. R.; Barkholtz, H. M.

    While the low cost and strong safety record of lead-acid batteries make them an appealing option compared to lithium-ion technologies for stationary storage, they can be rapidly degraded by the extended periods of high rate, partial state-of-charge operation required in such applications. Degradation occurs primarily through a process called hard sulfation, where large PbSO 4 crystals are formed on the negative battery plates, hindering charge acceptance and reducing battery capacity. Various researchers have found that the addition of some forms of excess carbon to the negative active mass in lead-acid batteries can mitigate hard sulfation, but the mechanism through whichmore » this is accomplished is unclear. In this work, the effect of carbon composition and morphology was explored by characterizing four discrete types of carbon additives, then evaluating their effect when added to the negative electrodes within a traditional valve-regulated lead-acid battery design. The cycle life for the carbon modified cells was significantly larger than an unmodified control, with cells containing a mixture of graphitic carbon and carbon black yielding the greatest improvement. The carbons also impacted other electrochemical aspects of the battery (e.g., float current, capacity, etc.) as well as physical characteristics of the negative active mass, such as the specific surface area.« less

  3. Understanding Function and Performance of Carbon Additives in Lead-Acid Batteries

    DOE PAGES

    Enos, D. G.; Ferreira, S. R.; Barkholtz, H. M.; ...

    2017-10-31

    While the low cost and strong safety record of lead-acid batteries make them an appealing option compared to lithium-ion technologies for stationary storage, they can be rapidly degraded by the extended periods of high rate, partial state-of-charge operation required in such applications. Degradation occurs primarily through a process called hard sulfation, where large PbSO 4 crystals are formed on the negative battery plates, hindering charge acceptance and reducing battery capacity. Various researchers have found that the addition of some forms of excess carbon to the negative active mass in lead-acid batteries can mitigate hard sulfation, but the mechanism through whichmore » this is accomplished is unclear. In this work, the effect of carbon composition and morphology was explored by characterizing four discrete types of carbon additives, then evaluating their effect when added to the negative electrodes within a traditional valve-regulated lead-acid battery design. The cycle life for the carbon modified cells was significantly larger than an unmodified control, with cells containing a mixture of graphitic carbon and carbon black yielding the greatest improvement. The carbons also impacted other electrochemical aspects of the battery (e.g., float current, capacity, etc.) as well as physical characteristics of the negative active mass, such as the specific surface area.« less

  4. Ground-state oxygen holes and the metal–insulator transition in the negative charge-transfer rare-earth nickelates

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Bisogni, Valentina; Catalano, Sara; Green, Robert J.

    The metal-insulator transitions and the intriguing physical properties of rare-earth perovskite nickelates have attracted considerable attention in recent years. However, a complete understanding of these materials remains elusive. Here, taking a NdNiO 3 thin film as a representative example, we utilize a combination of x-ray absorption (XAS) and resonant inelastic x-ray scattering (RIXS) spectroscopies to resolve important aspects of the complex electronic structure of the rare-earth nickelates. The unusual coexistence of bound and continuum excitations observed in the RIXS spectra provides strong evidence for the abundance of oxygen 2p holes in the ground state of these materials. Using cluster calculationsmore » and Anderson impurity model interpretation, we show that these distinct spectral signatures arise from a Ni 3d 8 configuration along with holes in the oxygen 2p valence band, confirming suggestions that these materials do not obey a “conventional” positive charge-transfer picture, but instead exhibit a negative charge-transfer energy, in line with recent models interpreting the metal to insulator transition in terms of bond disproportionation.« less

  5. Ground-state oxygen holes and the metal–insulator transition in the negative charge-transfer rare-earth nickelates

    DOE PAGES

    Bisogni, Valentina; Catalano, Sara; Green, Robert J.; ...

    2016-10-11

    The metal-insulator transitions and the intriguing physical properties of rare-earth perovskite nickelates have attracted considerable attention in recent years. However, a complete understanding of these materials remains elusive. Here, taking a NdNiO 3 thin film as a representative example, we utilize a combination of x-ray absorption (XAS) and resonant inelastic x-ray scattering (RIXS) spectroscopies to resolve important aspects of the complex electronic structure of the rare-earth nickelates. The unusual coexistence of bound and continuum excitations observed in the RIXS spectra provides strong evidence for the abundance of oxygen 2p holes in the ground state of these materials. Using cluster calculationsmore » and Anderson impurity model interpretation, we show that these distinct spectral signatures arise from a Ni 3d 8 configuration along with holes in the oxygen 2p valence band, confirming suggestions that these materials do not obey a “conventional” positive charge-transfer picture, but instead exhibit a negative charge-transfer energy, in line with recent models interpreting the metal to insulator transition in terms of bond disproportionation.« less

  6. Nanowires formed by the co-assembly of a negatively charged low-molecular weight gelator and a zwitterionic polythiophene.

    PubMed

    Li, Feng; Palaniswamy, Ganesan; de Jong, Menno R; Aslund, Andreas; Konradsson, Peter; Marcelis, Antonius T M; Sudhölter, Ernst J R; Stuart, Martien A Cohen; Leermakers, Frans A M

    2010-06-21

    Conjugated organic nanowires have been prepared by co-assembling a carboxylate containing low-molecular weight gelator (LMWG) and an amino acid substituted polythiophene derivative (PTT). Upon introducing the zwitterionic polyelectrolyte PTT to a basic molecular solution of the organogelator, the negative charges on the LMWG are compensated by the positive charges of the PTT. As a result, nanowires form through co-assembly. These nanowires are visualized by both transmission electron microscopy (TEM) and atomic force microscopy (AFM). Depending on the concentration and ratio of the components these nanowires can be micrometers long. These measurements further suggest that the aggregates adopt a helical conformation. The morphology of these nanowires are studied with fluorescent confocal laser scanning microscopy (CLSM). The interactions between LMWG and PTT are characterized by steady-state and time-resolved fluorescence spectroscopy studies. The steady-state spectra indicate that the backbone of the PTT adopts a more planar and more aggregated conformation when interacting with LMWG. The time- resolved fluorescence decay studies confirm this interpretation.

  7. Maintenance of coat protein N-terminal net charge and not primary sequence is essential for zucchini yellow mosaic virus systemic infectivity.

    PubMed

    Kimalov, Boaz; Gal-On, Amit; Stav, Ran; Belausov, Eduard; Arazi, Tzahi

    2004-11-01

    Zucchini yellow mosaic virus (ZYMV) surface exposed coat protein (CP) N-terminal domain (Nt) is 43 aa long and contains an equal number of positively and negatively charged amino acid residues (CP-Nt net charge = 0). A ZYMV-AGII truncation mutant lacking the first 20 aa of its CP-Nt (AGII-CP Delta 20; CP-Nt net charge = +2) was found to be systemically non-infectious even though AGII mutants harbouring larger CP-Nt deletions were previously demonstrated to be fully infectious. Nevertheless, AGII-CP Delta 20 infectivity was restored by fusion to its CP-Nt two Asp residues or a negatively charged Myc peptide, both predicted to neutralize CP-Nt net positive charge. To evaluate further the significance of CP-Nt net charge for AGII infectivity, a series of CP-Nt net charge mutants was generated and analysed for systemic infectivity of squash plants. AGII-CP(KKK) harbouring a CP-Nt amino fusion of three Lys residues (CP-Nt net charge = +3) was not systemically infectious. Addition of up to four Asp residues to CP-Nt did not abolish virus infectivity, although certain mutants were genetically unstable and had delayed infectivity. Addition of five negatively charged residues abolished infectivity (AGII-CP(DDDDD); CP-Nt net charge = -5) even though a recombinant CP(DDDDD) could assemble into potyviral-like particle in bacteria. Neutralization of CP-Nt net charge by fusing Asp or Lys residues recovered infectivity of AGII-CP(KKK) and AGII-CP(DDDDD). GFP-tagging of these mutants has demonstrated that both viruses have defective cell-to-cell movement. Together, these findings suggest that maintenance of CP-Nt net charge and not primary sequence is essential for ZYMV infectivity.

  8. A negative charge in transmembrane segment 1 of domain II of the cockroach sodium channel is critical for channel gating and action of pyrethroid insecticides

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Du Yuzhe; Song Weizhong; Groome, James R.

    2010-08-15

    Voltage-gated sodium channels are the primary target of pyrethroids, an important class of synthetic insecticides. Pyrethroids bind to a distinct receptor site on sodium channels and prolong the open state by inhibiting channel deactivation and inactivation. Recent studies have begun to reveal sodium channel residues important for pyrethroid binding. However, how pyrethroid binding leads to inhibition of sodium channel deactivation and inactivation remains elusive. In this study, we show that a negatively charged aspartic acid residue at position 802 (D802) located in the extracellular end of transmembrane segment 1 of domain II (IIS1) is critical for both the action ofmore » pyrethroids and the voltage dependence of channel activation. Charge-reversing or -neutralizing substitutions (K, G, or A) of D802 shifted the voltage dependence of activation in the depolarizing direction and reduced channel sensitivity to deltamethrin, a pyrethroid insecticide. The charge-reversing mutation D802K also accelerated open-state deactivation, which may have counteracted the inhibition of sodium channel deactivation by deltamethrin. In contrast, the D802G substitution slowed open-state deactivation, suggesting an additional mechanism for neutralizing the action of deltamethrin. Importantly, Schild analysis showed that D802 is not involved in pyrethroid binding. Thus, we have identified a sodium channel residue that is critical for regulating the action of pyrethroids on the sodium channel without affecting the receptor site of pyrethroids.« less

  9. Addition of ferrocene controls polymorphism and enhances charge mobilities in poly(3-hexylthiophene) thin-film transistors

    NASA Astrophysics Data System (ADS)

    Smith, Brandon; Clark, Michael; Grieco, Christopher; Larsen, Alec; Asbury, John; Gomez, Enrique

    2015-03-01

    Crystalline organic molecules often exhibit the ability to form multiple crystal structures depending on the processing conditions. Exploiting this polymorphism to optimize molecular orbital overlap between adjacent molecules within the unit lattice of conjugated polymers is an approach to enhance charge transport within the material. We have demonstrated the formation of tighter π- π stacking poly(3-hexylthiophene-2,5-diyl) polymorphs in films spin coated from ferrocene-containing solutions using grazing incident X-ray diffraction. As a result, we found that the addition of ferrocene to casting solutions yields thin-film transistors which exhibit significantly higher source-drain current and charge mobilities than neat polymer devices. Insights gleaned from ferrocene/poly(3-hexylthiophene) mixtures can serve as a template for selection and optimization of next generation small molecule/polymer systems possessing greater baseline charge mobilities. Ultimately, the development of such techniques to enhance the characteristics of organic transistors without imparting high costs or loss of advantageous properties will be a critical factor determining the future of organic components within the electronics market.

  10. Control of gel swelling and phase separation of weakly charged thermoreversible gels by salt addition

    PubMed Central

    Solis, Francisco J.; Vernon, Brent

    2009-01-01

    Doping of thermoreversible polymer gels with charged monomers provides a way to control phase separation and gelation conditions by coupling the properties of the gel with a tunable ionic environment. We analyze the dependence of the gelation and phase separation conditions on the amount of salt present using a mean field model of weakly charged associative polymers. The ions and co-ions present are explicitly considered at the mean field level, and we determine their concentrations in the different equilibrium phases when the system undergoes phase separation. For weak polymer charge, the entropic contributions of the ions to the free energy of the system play a central role in the determination of the location of phase equilibrium. In the simplest case, when the associative interaction responsible for gel formation is independent of the electrostatic interaction, the addition of salt changes the polymer equilibrium concentrations and indirectly changes the measurable swelling of the gel. We construct phase diagrams of these systems showing the location of the coexistence region, the gel-sol boundary and the location of the tie-lines. We determine the swelling of the gel within the co-existence region. Our main result is that the description of the effect of the salt on the properties of the weakly charged gel can be described through an extra contribution to the effective immiscibility parameter χ proportional to the square of the doping degree f2 and to the inverse square of the added salt concentration s−2. PMID:19759854

  11. Enhanced adsorption of Ca-ATPase containing vesicles on a negatively charged solid-supported-membrane for the investigation of membrane transporters.

    PubMed

    Sacconi, Alessio; Moncelli, Maria Rosa; Margheri, Giancarlo; Tadini-Buoninsegni, Francesco

    2013-11-12

    A convenient model system for a biological membrane is a solid-supported membrane (SSM), which consists of a gold-supported alkanethiol|phospholipid bilayer. In combination with a concentration jump method, SSMs have been used for the investigation of several membrane transporters. Vesicles incorporating sarcoplasmic reticulum Ca-ATPase (SERCA) were adsorbed on a negatively charged SSM (octadecanethiol|phosphatidylserine bilayer). The current signal generated by the adsorbed vesicles following an ATP concentration jump was compared to that produced by SERCA-containing vesicles adsorbed on a conventional SSM (octadecanethiol|phosphatidylcholine bilayer). A significantly higher current amplitude was recorded on the serine-based SSM. The adsorption of SERCA-incorporating vesicles on the SSM was then characterized by surface plasmon resonance (SPR). The SPR measurements clearly indicate that in the presence of Ca(2+) and Mg(2+), the amount of adsorbed vesicles on the serine-based SSM is about twice that obtained using the conventional SSM, thereby demonstrating that the higher current amplitude recorded on the negatively charged SSM is correlated with a greater quantity of adsorbed vesicles. The enhanced adsorption of membrane vesicles on the PS-based SSM may be useful to study membrane preparations with a low concentration of transport protein generating small current signals, as in the case of various recombinantly expressed proteins.

  12. Charge requirements of lipid II flippase activity in Escherichia coli.

    PubMed

    Butler, Emily K; Tan, Wee Boon; Joseph, Hildy; Ruiz, Natividad

    2014-12-01

    Peptidoglycan (PG) is an extracytoplasmic glycopeptide matrix essential for the integrity of the envelope of most bacteria. The PG building block is a disaccharide-pentapeptide that is synthesized as a lipid-linked precursor called lipid II. The translocation of the amphipathic lipid II across the cytoplasmic membrane is required for subsequent incorporation of the disaccharide-pentapeptide into PG. In Escherichia coli, the essential inner membrane protein MurJ is the lipid II flippase. Previous studies showed that 8 charged residues in the central cavity region of MurJ are crucial for function. Here, we completed the functional analysis of all 57 charged residues in MurJ and demonstrated that the respective positive or negative charge of the 8 aforementioned residues is required for proper MurJ function. Loss of the negative charge in one of these residues, D39, causes a severe defect in MurJ biogenesis; by engineering an intragenic suppressor mutation that restores MurJ biogenesis, we found that this charge is also essential for MurJ function. Because of the low level of homology between MurJ and putative orthologs from Gram-positive bacteria, we explored the conservation of these 8 charged residues in YtgP, a homolog from Streptococcus pyogenes. We found that only 3 positive charges are similarly positioned and essential in YtgP; YtgP possesses additional charged residues within its predicted cavity that are essential for function and conserved among Gram-positive bacteria. From these data, we hypothesize that some charged residues in the cavity region of MurJ homologs are required for interaction with lipid II and/or energy coupling during transport. Copyright © 2014, American Society for Microbiology. All Rights Reserved.

  13. Effects of organic silicon compounds as additives on charge-discharge cycling efficiencies of lithium in nonaqueous electrolytes for rechargeable lithium cells

    NASA Astrophysics Data System (ADS)

    Yanagisawa, Ryota; Endo, Hisayuki; Unno, Masafumi; Morimoto, Hideyuki; Tobishima, Shin-ichi

    2014-11-01

    Influence of mixing organic silicon compounds into 1 M (M: mol L-1) LiPF6-ethylene carbonate (EC)/ethylmethyl carbonate (EMC) (mixing volume ratio = 3:7) mixed solvent electrolytes on charge-discharge cycling efficiencies of lithium metal negative electrodes is examined. As organic silicon compounds, polyether-modified siloxanes with polyethylene oxide chains, chlorotrimethylsilane, tetraethoxysilane, cis-tetra [isobutyl (dimethylsiloxy)] cyclotetrasiloxane and cage-type silsesquioxane are investigated. Charge-discharge cycling tests of lithium are galvanostatically carried out using stainless steel working electrodes. Charge-discharge cycling efficiencies of lithium tend to improve by mixing organic silicon compounds. A cage-type silsesquioxane, octaphenyloctasilsesquioxane (Ph8T8) exhibits the highest cycling efficiency of approximately 80% with small mixing amount of 0.02 M Ph8T8. Mechanism of enhancement of lithium cycling efficiencies by mixing organic silicon compounds is considered to be due to the suppression of excess reduction of LiPF6-EC/EMC by lithium and the growth of surface film on lithium.

  14. Charge Storage, Conductivity and Charge Profiles of Insulators as Related to Spacecraft Charging

    NASA Technical Reports Server (NTRS)

    Dennison, J. R.; Swaminathan, Prasanna; Frederickson, A. R.

    2004-01-01

    Dissipation of charges built up near the surface of insulators due to space environment interaction is central to understanding spacecraft charging. Conductivity of insulating materials is key to determine how accumulated charge will distribute across the spacecraft and how rapidly charge imbalance will dissipate. To understand these processes requires knowledge of how charge is deposited within the insulator, the mechanisms for charge trapping and charge transport within the insulator, and how the profile of trapped charge affects the transport and emission of charges from insulators. One must consider generation of mobile electrons and holes, their trapping, thermal de-trapping, mobility and recombination. Conductivity is more appropriately measured for spacecraft charging applications as the "decay" of charge deposited on the surface of an insulator, rather than by flow of current across two electrodes around the sample. We have found that conductivity determined from charge storage decay methods is 102 to 104 smaller than values obtained from classical ASTM and IEC methods for a variety of thin film insulating samples. For typical spacecraft charging conditions, classical conductivity predicts decay times on the order of minutes to hours (less than typical orbit periods); however, the higher charge storage conductivities predict decay times on the order of weeks to months leading to accumulation of charge with subsequent orbits. We found experimental evidence that penetration profiles of radiation and light are exceedingly important, and that internal electric fields due to charge profiles and high-field conduction by trapped electrons must be considered for space applications. We have also studied whether the decay constants depend on incident voltage and flux or on internal charge distributions and electric fields; light-activated discharge of surface charge to distinguish among differing charge trapping centers; and radiation-induced conductivity. Our

  15. The interstitial distribution of macromolecules in rat tumours is influenced by the negatively charged matrix components

    PubMed Central

    Wiig, Helge; Gyenge, Christina C; Tenstad, Olav

    2005-01-01

    Knowledge of macromolecular distribution volumes is essential in understanding fluid transport within normal and pathological tissues. In this study in vivo we determined the distribution volumes of several macromolecules, including one monoclonal antibody, in tumours and tested whether charges associated with the tumour extracellular matrix influence their available volumes. Steady state levels of the monoclonal antibody trastuzumab (Herceptin) (pI = 9.2), IgG (pI = 7.6) as well as native (pI = 5.0) and cationized albumin (pI = 7.6) were established in rats bearing dimethylbenzanthracene (DMBA)-induced mammary tumours by continuous infusion using osmotic minipumps. After a 5–7 day infusion period, the rats were nephrectomized and the extracellular volume was determined with 51Cr-labelled EDTA. Plasma volumes were measured with 125I-labelled human serum albumin or rat IgM in a separate series. Steady state concentrations of probes were determined in the interstitial fluid that was isolated by centrifugation from tumours or by post mortem wick implantation in the back skin. Calculations were made for interstitial fluid volume (Vi), along with the available (Va/Vi) and excluded (Ve/Vi) relative interstitial volume fractions. The Ve/Vi for the positively charged trastuzumab in tumours averaged 0.29 ± 0.03 (n = 16), a value which was significantly lower than the corresponding one for IgG of 0.36 ± 0.02 (n = 16). Native albumin was excluded from 38% of the tumour interstitial fluid, whereas cationization of albumin reduced the excluded volume by ∼50%. Our experiments suggest that the tumour interstitium acts as a negatively charged matrix and is an important factor in determining the macromolecular distribution volume. PMID:15994186

  16. The interstitial distribution of macromolecules in rat tumours is influenced by the negatively charged matrix components.

    PubMed

    Wiig, Helge; Gyenge, Christina C; Tenstad, Olav

    2005-09-01

    Knowledge of macromolecular distribution volumes is essential in understanding fluid transport within normal and pathological tissues. In this study in vivo we determined the distribution volumes of several macromolecules, including one monoclonal antibody, in tumours and tested whether charges associated with the tumour extracellular matrix influence their available volumes. Steady state levels of the monoclonal antibody trastuzumab (Herceptin) (pI = 9.2), IgG (pI = 7.6) as well as native (pI = 5.0) and cationized albumin (pI = 7.6) were established in rats bearing dimethylbenzanthracene (DMBA)-induced mammary tumours by continuous infusion using osmotic minipumps. After a 5-7 day infusion period, the rats were nephrectomized and the extracellular volume was determined with 51Cr-labelled EDTA. Plasma volumes were measured with 125I-labelled human serum albumin or rat IgM in a separate series. Steady state concentrations of probes were determined in the interstitial fluid that was isolated by centrifugation from tumours or by post mortem wick implantation in the back skin. Calculations were made for interstitial fluid volume (Vi), along with the available (Va/Vi) and excluded (Ve/Vi) relative interstitial volume fractions. The Ve/Vi for the positively charged trastuzumab in tumours averaged 0.29 +/- 0.03 (n = 16), a value which was significantly lower than the corresponding one for IgG of 0.36 +/- 0.02 (n = 16). Native albumin was excluded from 38% of the tumour interstitial fluid, whereas cationization of albumin reduced the excluded volume by approximately 50%. Our experiments suggest that the tumour interstitium acts as a negatively charged matrix and is an important factor in determining the macromolecular distribution volume.

  17. Effect of plasma-induced surface charging on catalytic processes: application to CO2 activation

    NASA Astrophysics Data System (ADS)

    Bal, Kristof M.; Huygh, Stijn; Bogaerts, Annemie; Neyts, Erik C.

    2018-02-01

    Understanding the nature and effect of the multitude of plasma-surface interactions in plasma catalysis is a crucial requirement for further process development and improvement. A particularly intriguing and rather unique property of a plasma-catalytic setup is the ability of the plasma to modify the electronic structure, and hence chemical properties, of the catalyst through charging, i.e. the absorption of excess electrons. In this work, we develop a quantum chemical model based on density functional theory to study excess negative surface charges in a heterogeneous catalyst exposed to a plasma. This method is specifically applied to investigate plasma-catalytic CO2 activation on supported M/Al2O3 (M = Ti, Ni, Cu) single atom catalysts. We find that (1) the presence of a negative surface charge dramatically improves the reductive power of the catalyst, strongly promoting the splitting of CO2 to CO and oxygen, and (2) the relative activity of the investigated transition metals is also changed upon charging, suggesting that controlled surface charging is a powerful additional parameter to tune catalyst activity and selectivity. These results strongly point to plasma-induced surface charging of the catalyst as an important factor contributing to the plasma-catalyst synergistic effects frequently reported for plasma catalysis.

  18. The influence of negative ions in helium-oxygen barrier discharges: III. Simulation of laser photodetachment and comparison with experiment

    NASA Astrophysics Data System (ADS)

    Nemschokmichal, Sebastian; Tschiersch, Robert; Meichsner, Jürgen

    2017-11-01

    The laser photodetachment experiment in a diffuse helium-oxygen barrier discharge is evaluated by a 1D fluid simulation. As in the experiment, the simulated discharge operates in helium with 400 {ppm} oxygen admixture at 500 {mbar} inside a discharge gap of 3 {mm}. The laser photodetachment is included by the interaction of negative ions with a temporally and spatially dependent photon flux. The simulation with the usually applied set of reactions and rate coefficients provides a much lower negative ion density than needed to explain the impact on the discharge characteristics in the experiment. Further processes for an enhanced negative ion formation and their capabilities of reproducing the experimental results are discussed. These further processes are additional attachment processes in the volume and the negative ion formation at the negatively charged dielectric. Both approaches are able to reproduce the measured laser photodetachment effect partially, but the best agreement with the experimental results is achieved with the formation of negative ions at the negatively charged dielectric.

  19. The influence of space charge shielding on dielectric multipactor

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Chang, C.; Liu, G. Z.; Tang, C. X.

    2009-05-15

    A model of space charge influenced by multipactor electrons and plasma has been established. The positive space charge potential/field for vacuum dielectric multipactor is analytically studied. After considering the plasma, the positive space charge field is further shielded, and multipactor saturates at higher surface accumulated field, compared with that for only considering multipactor electrons. The negative space charge potential/field for dielectric breakdown at high pressure is analyzed. It is found that the negative potential can be nonmonotonously varied, forming a minimum potential well.

  20. Improving Charging-Breeding Simulations with Space-Charge Effects

    NASA Astrophysics Data System (ADS)

    Bilek, Ryan; Kwiatkowski, Ania; Steinbrügge, René

    2016-09-01

    Rare-isotope-beam facilities use Highly Charged Ions (HCI) for accelerators accelerating heavy ions and to improve measurement precision and resolving power of certain experiments. An Electron Beam Ion Trap (EBIT) is able to create HCI through successive electron impact, charge breeding trapped ions into higher charge states. CBSIM was created to calculate successive charge breeding with an EBIT. It was augmented by transferring it into an object-oriented programming language, including additional elements, improving ion-ion collision factors, and exploring the overlap of the electron beam with the ions. The calculation is enhanced with the effects of residual background gas by computing the space charge due to charge breeding. The program assimilates background species, ionizes and charge breeds them alongside the element being studied, and allows them to interact with the desired species through charge exchange, giving fairer overview of realistic charge breeding. Calculations of charge breeding will be shown for realistic experimental conditions. We reexamined the implementation of ionization energies, cross sections, and ion-ion interactions when charge breeding.

  1. A threshold effect for spacecraft charging

    NASA Technical Reports Server (NTRS)

    Olsen, R. C.

    1983-01-01

    The borderline case between no charging and large (kV) negative potentials for eclipse charging events on geosynchronous satellites is investigated, and the dependence of this transition on a threshold energy in the ambient plasma is examined. Data from the Applied Technology Satellite 6 and P78-2 (SCATHA) show that plasma sheet fluxes must extend above 10 keV for these satellites to charge in eclipse. The threshold effect is a result of the shape of the normal secondary yield curve, in particular the high energy crossover, where the secondary yield drops below 1. It is found that a large portion of the ambient electron flux must exceed this energy for a negative current to exist.

  2. Single charging events on colloidal particles in a nonpolar liquid with surfactant

    NASA Astrophysics Data System (ADS)

    Schreuer, Caspar; Vandewiele, Stijn; Brans, Toon; Strubbe, Filip; Neyts, Kristiaan; Beunis, Filip

    2018-01-01

    Electrical charging of colloidal particles in nonpolar liquids due to surfactant additives is investigated intensively, motivated by its importance in a variety of applications. Most methods rely on average electrophoretic mobility measurements of many particles, which provide only indirect information on the charging mechanism. In the present work, we present a method that allows us to obtain direct information on the charging mechanism, by measuring the charge fluctuations on individual particles with a precision higher than the elementary charge using optical trapping electrophoresis. We demonstrate the capabilities of the method by studying the influence of added surfactant OLOA 11000 on the charging of single colloidal PMMA particles in dodecane. The particle charge and the frequency of charging events are investigated both below and above the critical micelle concentration (CMC) and with or without applying a DC offset voltage. It is found that at least two separate charging mechanisms are present below the critical micelle concentration. One mechanism is a process where the particle is stripped from negatively charged ionic molecules. An increase in the charging frequency with increased surfactant concentration suggests a second mechanism that involves single surfactant molecules. Above the CMC, neutral inverse micelles can also be involved in the charging process.

  3. In situ NMR spectroscopy of supercapacitors: insight into the charge storage mechanism.

    PubMed

    Wang, Hao; Forse, Alexander C; Griffin, John M; Trease, Nicole M; Trognko, Lorie; Taberna, Pierre-Louis; Simon, Patrice; Grey, Clare P

    2013-12-18

    Electrochemical capacitors, commonly known as supercapacitors, are important energy storage devices with high power capabilities and long cycle lives. Here we report the development and application of in situ nuclear magnetic resonance (NMR) methodologies to study changes at the electrode-electrolyte interface in working devices as they charge and discharge. For a supercapacitor comprising activated carbon electrodes and an organic electrolyte, NMR experiments carried out at different charge states allow quantification of the number of charge storing species and show that there are at least two distinct charge storage regimes. At cell voltages below 0.75 V, electrolyte anions are increasingly desorbed from the carbon micropores at the negative electrode, while at the positive electrode there is little change in the number of anions that are adsorbed as the voltage is increased. However, above a cell voltage of 0.75 V, dramatic increases in the amount of adsorbed anions in the positive electrode are observed while anions continue to be desorbed at the negative electrode. NMR experiments with simultaneous cyclic voltammetry show that supercapacitor charging causes marked changes to the local environments of charge storing species, with periodic changes of their chemical shift observed. NMR calculations on a model carbon fragment show that the addition and removal of electrons from a delocalized system should lead to considerable increases in the nucleus-independent chemical shift of nearby species, in agreement with our experimental observations.

  4. In Situ NMR Spectroscopy of Supercapacitors: Insight into the Charge Storage Mechanism

    PubMed Central

    2013-01-01

    Electrochemical capacitors, commonly known as supercapacitors, are important energy storage devices with high power capabilities and long cycle lives. Here we report the development and application of in situ nuclear magnetic resonance (NMR) methodologies to study changes at the electrode–electrolyte interface in working devices as they charge and discharge. For a supercapacitor comprising activated carbon electrodes and an organic electrolyte, NMR experiments carried out at different charge states allow quantification of the number of charge storing species and show that there are at least two distinct charge storage regimes. At cell voltages below 0.75 V, electrolyte anions are increasingly desorbed from the carbon micropores at the negative electrode, while at the positive electrode there is little change in the number of anions that are adsorbed as the voltage is increased. However, above a cell voltage of 0.75 V, dramatic increases in the amount of adsorbed anions in the positive electrode are observed while anions continue to be desorbed at the negative electrode. NMR experiments with simultaneous cyclic voltammetry show that supercapacitor charging causes marked changes to the local environments of charge storing species, with periodic changes of their chemical shift observed. NMR calculations on a model carbon fragment show that the addition and removal of electrons from a delocalized system should lead to considerable increases in the nucleus-independent chemical shift of nearby species, in agreement with our experimental observations. PMID:24274637

  5. How trust and emotions influence policy acceptance: The case of the Irish water charges.

    PubMed

    Rodriguez-Sanchez, Carla; Schuitema, Geertje; Claudy, Marius; Sancho-Esper, Franco

    2018-02-01

    The introduction of new policies can evoke strong emotional reactions by the public. Yet, social-psychological research has paid little attention to affective determinants of individual-level policy acceptance. Building on recent theoretical and empirical advances around emotions and decision-making, we evaluate how people's trust and integral emotions function as important antecedents of cognitive evaluations, and subsequent acceptance of policies. We test our hypotheses within a sample of Irish citizens (n = 505), who were subject to the introduction of water charges in 2015. In line with our hypotheses, results show that general trust in government shapes emotions regarding water charges, which in turn, directly and via expected costs and benefits, influence policy acceptance. Additionally, we find that negative emotions have a larger direct effect on policy acceptance than positive emotions. Specifically, 'anger' was the main negative emotion that influenced the acceptance of the water charge. We conclude by discussing directions for future research around emotions and policy acceptance. © 2018 The British Psychological Society.

  6. Positively Charged Residues Are the Major Determinants of Ribosomal Velocity

    PubMed Central

    Charneski, Catherine A.; Hurst, Laurence D.

    2013-01-01

    Both for understanding mechanisms of disease and for the design of transgenes, it is important to understand the determinants of ribosome velocity, as changes in the rate of translation are important for protein folding, error attenuation, and localization. While there is great variation in ribosomal occupancy along even a single transcript, what determines a ribosome's occupancy is unclear. We examine this issue using data from a ribosomal footprinting assay in yeast. While codon usage is classically considered a major determinant, we find no evidence for this. By contrast, we find that positively charged amino acids greatly retard ribosomes downstream from where they are encoded, consistent with the suggestion that positively charged residues interact with the negatively charged ribosomal exit tunnel. Such slowing is independent of and greater than the average effect owing to mRNA folding. The effect of charged amino acids is additive, with ribosomal occupancy well-predicted by a linear fit to the density of positively charged residues. We thus expect that a translated poly-A tail, encoding for positively charged lysines regardless of the reading frame, would act as a sandtrap for the ribosome, consistent with experimental data. PMID:23554576

  7. Particle size, charge and colloidal stability of humic acids coprecipitated with Ferrihydrite.

    PubMed

    Angelico, Ruggero; Ceglie, Andrea; He, Ji-Zheng; Liu, Yu-Rong; Palumbo, Giuseppe; Colombo, Claudio

    2014-03-01

    Humic acids (HA) have a colloidal character whose size and negative charge are strictly dependent on surface functional groups. They are able to complex large amount of poorly ordered iron (hydr)oxides in soil as a function of pH and other environmental conditions. Accordingly, with the present study we intend to assess the colloidal properties of Fe(II) coprecipitated with humic acids (HA) and their effect on Fe hydroxide crystallinity under abiotic oxidation and order of addition of both Fe(II) and HA. TEM, XRD and DRS experiments showed that Fe-HA consisted of Ferrihydrite with important structural variations. DLS data of Fe-HA at acidic pH showed a bimodal size distribution, while at very low pH a slow aggregation process was observed. Electrophoretic zeta-potential measurements revealed a negative surface charge for Fe-HA macromolecules, providing a strong electrostatic barrier against aggregation. Under alkaline conditions HA chains swelled, which resulted in an enhanced stabilization of the colloid particles. The increasing of zeta potential and size of the Fe-HA macromolecules, reflects a linear dependence of both with pH. The increase in the size and negative charge of the Fe-HA precipitate seems to be more affected by the ionization of the phenolic acid groups, than by the carboxylic acid groups. The main cause of negative charge generation of Fe/HA is due to increased dissociation of phenolic groups in more expanded structure. The increased net negative surface potential induced by coprecipitation with Ferrihydrite and the correspondent changes in configuration of the HA could trigger the inter-particle aggregation with the formation of new negative surface. The Fe-HA coprecipitation can reduce electrosteric repulsive forces, which in turn may inhibit the aggregation process at different pH. Therefore, coprecipitation of Ferrihydrite would be expected to play an important role in the carbon stabilization and persistence not only in organic soils, but

  8. Effect of electric charge on the adhesion of human blood platelets.

    PubMed

    Lowkis, B; Szymonowicz, M

    1993-01-01

    The paper presents the results of research into the effect of the size and depth of the implanted electric charge on the adhesion of human blood platelets. The experiments were carried out on polyethylene terephthalate PET foil of 36 microns thickness. The electret formation process was carried out in an electron-beam device. The electrization conditions were such that electrets with the excess electric charge accumulated at various depths were obtained. The selection of conditions was verified by investigating the space charge distribution with the use of the virtual electrode method. The microscopic observation of non-electrified foils and electrets as well as the quantitative examination of the adhesion of human blood platelets has explicitly confirmed the positive influence of the electret effect on the thrombogenesis of PET foil. This made it possible to define the optimum electrization conditions. The research has additionally indicated that the relationship between the amount of adherent blood platelets and the size of the electric charge is not a simple relation of the kind: the larger negative charge, the more thrombogenic material. The decisive and positive effect of the space charge has been confirmed by analysing the effectiveness of the surface and space charge.

  9. Protein charge distribution in proteomes and its impact on translation

    PubMed Central

    Requião, Rodrigo D.; Fernandes, Luiza; de Souza, Henrique José Araujo; Rossetto, Silvana; Domitrovic, Tatiana

    2017-01-01

    As proteins are synthesized, the nascent polypeptide must pass through a negatively charged exit tunnel. During this stage, positively charged stretches can interact with the ribosome walls and slow the translation. Therefore, charged polypeptides may be important factors that affect protein expression. To determine the frequency and distribution of positively and negatively charged stretches in different proteomes, the net charge was calculated for every 30 consecutive amino acid residues, which corresponds to the length of the ribosome exit tunnel. The following annotated and reviewed proteins in the UniProt database (Swiss-Prot) were analyzed: 551,705 proteins from different organisms and a total of 180 million protein segments. We observed that there were more negative than positive stretches and that super-charged positive sequences (i.e., net charges ≥ 14) were underrepresented in the proteomes. Overall, the proteins were more positively charged at their N-termini and C-termini, and this feature was present in most organisms and subcellular localizations. To investigate whether the N-terminal charges affect the elongation rates, previously published ribosomal profiling data obtained from S. cerevisiae, without translation-interfering drugs, were analyzed. We observed a nonlinear effect of the charge on the ribosome occupancy in which values ≥ +5 and ≤ -6 showed increased and reduced ribosome densities, respectively. These groups also showed different distributions across 80S monosomes and polysomes. Basic polypeptides are more common within short proteins that are translated by monosomes, whereas negative stretches are more abundant in polysome-translated proteins. These findings suggest that the nascent peptide charge impacts translation and can be one of the factors that regulate translation efficiency and protein expression. PMID:28531225

  10. Influence of liposome charge on the association of liposomes with Kupffer cells in vitro. Effects of divalent cations and competition with latex particles.

    PubMed

    Dijkstra, J; van Galen, M; Scherphof, G

    1985-03-14

    We studied the interaction of large unilamellar liposomes carrying different surface charges with rat Kupffer cells in maintenance culture. In addition to 14C-labeled phosphatidylcholine, all liposome preparations contained either 3H-labeled inulin or 125I-labeled bovine serum albumin as a non-degradable or a degradable aqueous space marker, respectively. With vesicles carrying no net charge, intracellular processing of internalized liposomes caused nearly complete release of protein label into the medium in acid-soluble form, while phospholipid label was predominantly retained by the cells, only about one third being released. The presence of the lysosomotropic agent, ammonia, inhibited the release of both labels from the cells. At 4 degrees C, the association and degradation of the vesicles were strongly reduced. These results are very similar to what we reported on negatively charged liposomes (Dijkstra, J., Van Galen, W.J.M., Hulstaert, C.E., Kalicharan, D., Roerdink, F.H. and Scherphof, G.L. (1984) Exp. Cell Res. 150, 161-176). The interaction of both types of vesicles apparently proceeds by adsorption to the cell surface followed by virtually complete internalization by endocytosis. Similar experiments with positively charged vesicles indicated that only about half of the liposomes were taken up by the endocytic route, the other half remaining adsorbed to the cell-surface. Attachment of all types of liposomes to the cells was strongly dependent on the presence of divalent cations; Ca2+ appeared to be required for optimal binding. Neutral liposomes only slightly competed with the uptake of negatively charged vesicles, both at 4 degrees and 37 degrees C, whereas negatively charged small unilamellar vesicles and negatively charged latex beads were found to compete very effectively with the large negatively charged liposomes. Neutral vesicles competed effectively for uptake with positively charged ones. These results suggest that neutral and positively charged

  11. Impact of negative capacitance effect on Germanium Double Gate pFET for enhanced immunity to interface trap charges

    NASA Astrophysics Data System (ADS)

    Bansal, Monika; Kaur, Harsupreet

    2018-05-01

    In this work, a comprehensive drain current model has been developed for long channel Negative Capacitance Germanium Double Gate p-type Field Effect Transistor (NCGe-DG-pFET) by using 1-D Poisson's equation and Landau-Khalatnikov equation. The model takes into account interface trap charges and by using the derived model various parameters such as surface potential, gain, gate capacitance, subthreshold swing, drain current, transconductance, output conductance and Ion/Ioff ratio have been obtained and it is demonstrated that by incorporating ferroelectric material as gate insulator with Ge-channel, subthreshold swing values less than 60 mV/dec can be achieved along with improved gate controllability and current drivability. Further, to critically analyze the advantages offered by NCGe-DG-pFET, a detailed comparison has been done with Germanium Double Gate p-type Field Effect Transistor (Ge-DG-pFET) and it is shown that NCGe-DG-pFET exhibits high gain, enhanced transport efficiency in channel, very less or negligible degradation in device characteristics due to interface trap charges as compared to Ge-DG-pFET. The analytical results so obtained show good agreement with simulated results obtained from Silvaco ATLAS TCAD tool.

  12. Enabling high rate charge and discharge capability, low internal resistance, and excellent cycleability for Li-ion batteries utilizing graphene additives

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Tsai, Hsiu-Ling; Hsieh, Chien-Te; Li, Jianlin

    A liquid-phase mixing method is adopted to uniformly disperse the graphene nanosheets onto LiNi 1/3Co 1/3Mn 1/3O 2 cathode for high-performance Li-ion batteries (LIBs). The electrochemical performance was characterized using a full pouch cells with state-of-the-art electrode areal loading (compared to half coin cells). The addition of graphene sheets (i.e., only 1 wt%) significantly improves the high rate capability for charging and discharging operation. For example, 6 times improvement in 5 C charging was achieved providing further insights in enabling extreme fast charging for LIBs. Other benefits include longer cycleability, lower internal resistance, and higher lithium ion diffusion coefficient, demonstratedmore » by charge-discharge cycling tests and electrochemical impedance spectroscopy. Higher capacity retention of 88.2% and decreased internal resistance of ~0.9 Ω are observed after 400 cycles. The diffusion coefficient of Li ions is 6.49 × 10 -8 cm 2 s -1 when charged to 4.2 V, which is approximately 1.37 times higher compared to the configuration with no graphene sheet (4.74 × 10 -8 cm 2 s -1). To conclude, the improved performance is ascribed to a robust network among the active materials formed by graphene sheets, which serves as an extended current conductor and facilitates charge transfer, ionic reversibility, and ionic transportation.« less

  13. Enabling high rate charge and discharge capability, low internal resistance, and excellent cycleability for Li-ion batteries utilizing graphene additives

    DOE PAGES

    Tsai, Hsiu-Ling; Hsieh, Chien-Te; Li, Jianlin; ...

    2018-03-27

    A liquid-phase mixing method is adopted to uniformly disperse the graphene nanosheets onto LiNi 1/3Co 1/3Mn 1/3O 2 cathode for high-performance Li-ion batteries (LIBs). The electrochemical performance was characterized using a full pouch cells with state-of-the-art electrode areal loading (compared to half coin cells). The addition of graphene sheets (i.e., only 1 wt%) significantly improves the high rate capability for charging and discharging operation. For example, 6 times improvement in 5 C charging was achieved providing further insights in enabling extreme fast charging for LIBs. Other benefits include longer cycleability, lower internal resistance, and higher lithium ion diffusion coefficient, demonstratedmore » by charge-discharge cycling tests and electrochemical impedance spectroscopy. Higher capacity retention of 88.2% and decreased internal resistance of ~0.9 Ω are observed after 400 cycles. The diffusion coefficient of Li ions is 6.49 × 10 -8 cm 2 s -1 when charged to 4.2 V, which is approximately 1.37 times higher compared to the configuration with no graphene sheet (4.74 × 10 -8 cm 2 s -1). To conclude, the improved performance is ascribed to a robust network among the active materials formed by graphene sheets, which serves as an extended current conductor and facilitates charge transfer, ionic reversibility, and ionic transportation.« less

  14. Charged Residues at the First Transmembrane Region Contribute to the Voltage Dependence of the Slow Gate of Connexins*

    PubMed Central

    Pinto, Bernardo I.; García, Isaac E.; Pupo, Amaury; Retamal, Mauricio A.; Martínez, Agustín D.; Latorre, Ramón; González, Carlos

    2016-01-01

    Connexins (Cxs) are a family of membrane-spanning proteins that form gap junction channels and hemichannels. Connexin-based channels exhibit two distinct voltage-dependent gating mechanisms termed slow and fast gating. Residues located at the C terminus of the first transmembrane segment (TM-1) are important structural components of the slow gate. Here, we determined the role of the charged residues at the end of TM-1 in voltage sensing in Cx26, Cx46, and Cx50. Conductance/voltage curves obtained from tail currents together with kinetics analysis reveal that the fast and slow gates of Cx26 involves the movement of two and four charges across the electric field, respectively. Primary sequence alignment of different Cxs shows the presence of well conserved glutamate residues in the C terminus of TM-1; only Cx26 contains a lysine in that position (lysine 41). Neutralization of lysine 41 in Cx26 increases the voltage dependence of the slow gate. Swapping of lysine 41 with glutamate 42 maintains the voltage dependence. In Cx46, neutralization of negative charges or addition of a positive charge in the Cx26 equivalent region reduced the slow gate voltage dependence. In Cx50, the addition of a glutamate in the same region decreased the voltage dependence, and the neutralization of a negative charge increased it. These results indicate that the charges at the end of TM-1 are part of the slow gate voltage sensor in Cxs. The fact that Cx42, which has no charge in this region, still presents voltage-dependent slow gating suggests that charges still unidentified also contribute to the slow gate voltage sensitivity. PMID:27143357

  15. Charged rotating black holes in Einstein-Maxwell-Chern-Simons theory with a negative cosmological constant

    NASA Astrophysics Data System (ADS)

    Blázquez-Salcedo, Jose Luis; Kunz, Jutta; Navarro-Lérida, Francisco; Radu, Eugen

    2017-03-01

    We consider rotating black hole solutions in five-dimensional Einstein-Maxwell-Chern-Simons theory with a negative cosmological constant and a generic value of the Chern-Simons coupling constant λ . Using both analytical and numerical techniques, we focus on cohomogeneity-1 configurations, with two equal-magnitude angular momenta, which approach at infinity a globally anti-de Sitter background. We find that the generic solutions share a number of basic properties with the known Cvetič, Lü, and Pope black holes which have λ =1 . New features occur as well; for example, when the Chern-Simons coupling constant exceeds a critical value, the solutions are no longer uniquely determined by their global charges. Moreover, the black holes possess radial excitations which can be labelled by the node number of the magnetic gauge potential function. Solutions with small values of λ possess other distinct features. For instance, the extremal black holes there form two disconnected branches, while not all near-horizon solutions are associated with global solutions.

  16. Integration Assessment of Visiting Vehicle Induced Electrical Charging of the International Space Station Structure

    NASA Technical Reports Server (NTRS)

    Kramer, Leonard; Kerslake, Thomas W.; Galofaro, Joel T.

    2010-01-01

    The International Space Station (ISS) undergoes electrical charging in low Earth orbit (LEO) due to positively biased, exposed conductors on solar arrays that collect electrical charges from the space plasma. Exposed solar array conductors predominately collect negatively charged electrons and thus drive the metal ISS structure electrical ground to a negative floating potential (FP) relative to plasma. This FP is variable in location and time as a result of local ionospheric conditions. ISS motion through Earth s magnetic field creates an addition inductive voltage up to 20 positive and negative volts across ISS structure depending on its attitude and location in orbit. ISS Visiting Vehicles (VVs), such as the planned Orion crew exploration vehicle, contribute to the ISS plasma charging processes. Upon physical contact with ISS, the current collection properties of VVs combine with ISS. This is an ISS integration concern as FP must be controlled to minimize arcing of ISS surfaces and ensure proper management of extra vehicular activity crewman shock hazards. This report is an assessment of ISS induced charging from docked Orion vehicles employing negatively grounded, 130 volt class, UltraFlex (ATK Space Systems) solar arrays. To assess plasma electron current collection characteristics, Orion solar cell test coupons were constructed and subjected to plasma chamber current collection measurements. During these tests, coupon solar cells were biased between 0 and 120 V while immersed in a simulated LEO plasma. Tests were performed using several different simulated LEO plasma densities and temperatures. These data and associated theoretical scaling of plasma properties, were combined in a numerical model which was integrated into the Boeing Plasma Interaction Model. It was found that the solar array design for Orion will not affect the ISS FP by more than about 2 V during worst case charging conditions. This assessment also motivated a trade study to determine

  17. Kinetics and thermodynamics of chlorpromazine interaction with lipid bilayers: effect of charge and cholesterol.

    PubMed

    Martins, Patrícia T; Velazquez-Campoy, Adrian; Vaz, Winchil L C; Cardoso, Renato M S; Valério, Joana; Moreno, Maria João

    2012-03-07

    Passive transport across cell membranes is the major route for the permeation of xenobiotics through tight endothelia such as the blood–brain barrier. The rate of passive permeation through lipid bilayers for a given drug is therefore a critical step in the prediction of its pharmacodynamics. We describe a detailed study on the kinetics and thermodynamics for the interaction of chlorpromazine (CPZ), an antipsychotic drug used in the treatment of schizophrenia, with neutral and negatively charged lipid bilayers. Isothermal titration calorimetry was used to study the partition and translocation of CPZ in lipid membranes composed of pure POPC, POPC:POPS (9:1), and POPC:Chol:POPS (6:3:1). The membrane charge due to the presence of POPS as well as the additional charge resulting from the introduction of CPZ in the membrane were taken into account, allowing the calculation of the intrinsic partition coefficients (K(P)) and the enthalpy change (ΔH) associated with the process. The enthalpy change upon partition to all lipid bilayers studied is negative, but a significant entropy contribution was also observed for partition to the neutral membrane. Because of the positive charge of CPZ, the presence of negatively charged lipids in the bilayer increases both the observed amount of CPZ that partitions to the membrane (KP(obs)) and the magnitude of ΔH. However, when the electrostatic effects are discounted, the intrinsic partition coefficient was smaller, indicating that the hydrophobic contribution was less significant for the negatively charged membrane. The presence of cholesterol strongly decreases the affinity of CPZ for the bilayer in terms of both the amount of CPZ that associates with the membrane and the interaction enthalpy. A quantitative characterization of the rate of CPZ translocation through membranes composed of pure POPC and POPC:POPS (9:1) was also performed using an innovative methodology developed in this work based on the kinetics of the heat evolved

  18. Analysis of Lunar Surface Charging for a Candidate Spacecraft Using NASCAP-2K

    NASA Technical Reports Server (NTRS)

    Parker, Linda; Minow, Joseph; Blackwell, William, Jr.

    2007-01-01

    The characterization of the electromagnetic interaction for a spacecraft in the lunar environment, and identification of viable charging mitigation strategies, is a critical lunar mission design task, as spacecraft charging has important implications both for science applications and for astronaut safety. To that end, we have performed surface charging calculations of a candidate lunar spacecraft for lunar orbiting and lunar landing missions. We construct a model of the spacecraft with candidate materials having appropriate electrical properties using Object Toolkit and perform the spacecraft charging analysis using Nascap-2k, the NASA/AFRL sponsored spacecraft charging analysis tool. We use nominal and atypical lunar environments appropriate for lunar orbiting and lunar landing missions to establish current collection of lunar ions and electrons. In addition, we include a geostationary orbit case to demonstrate a bounding example of extreme (negative) charging of a lunar spacecraft in the geostationary orbit environment. Results from the charging analysis demonstrate that minimal differential potentials (and resulting threat of electrostatic discharge) occur when the spacecraft is constructed entirely of conducting materials, as expected. We compare charging results to data taken during previous lunar orbiting or lunar flyby spacecraft missions.

  19. Solute Transport of Negatively Charged Contrast Agents Across Articular Surface of Injured Cartilage.

    PubMed

    Kokkonen, H T; Chin, H C; Töyräs, J; Jurvelin, J S; Quinn, T M

    2017-04-01

    Solute transport through the extracellular matrix (ECM) is crucial to chondrocyte metabolism. Cartilage injury affects solute transport in cartilage due to alterations in ECM structure and solute-matrix interactions. Therefore, cartilage injury may be detected by using contrast agent-based clinical imaging. In the present study, effects of mechanical injury on transport of negatively charged contrast agents in cartilage were characterized. Using cartilage plugs injured by mechanical compression protocol, effective partition coefficients and diffusion fluxes of iodine- and gadolinium-based contrast agents were measured using high resolution microCT imaging. For all contrast agents studied, effective diffusion fluxes increased significantly, particularly at early times during the diffusion process (38 and 33% increase after 4 min, P < 0.05 for iodine and Gd-DTPA; and 76% increase after 10 min for diatrizoate, P < 0.05). Effective partition coefficients were unaffected in mechanically injured cartilage. Mechanical injury reduced PG content and collagen integrity in cartilage superficial zone. This study suggests that alterations in contrast agent diffusion flux, a non-equilibrium transport parameter, provides a more sensitive indicator for assessment of cartilage matrix integrity than partition coefficient and the equilibrium distribution of solute. These findings may help in developing clinical methods of contrast agent-based imaging to detect cartilage injury.

  20. Surface charge effects in protein adsorption on nanodiamonds.

    PubMed

    Aramesh, M; Shimoni, O; Ostrikov, K; Prawer, S; Cervenka, J

    2015-03-19

    Understanding the interaction of proteins with charged diamond nanoparticles is of fundamental importance for diverse biomedical applications. Here we present a thorough study of protein binding, adsorption kinetics and structure on strongly positively (hydrogen-terminated) and negatively (oxygen-terminated) charged nanodiamond particles using a quartz crystal microbalance by dissipation and infrared spectroscopy. By using two model proteins (bovine serum albumin and lysozyme) of different properties (charge, molecular weight and rigidity), the main driving mechanism responsible for the protein binding to the charged nanoparticles was identified. Electrostatic interactions were found to dominate the protein adsorption dynamics, attachment and conformation. We developed a simple electrostatic model that can qualitatively explain the observed adsorption behaviour based on charge-induced pH modifications near the charged nanoparticle surfaces. Under neutral conditions, the local pH around the positively and negatively charged nanodiamonds becomes very high (11-12) and low (1-3) respectively, which has a profound impact on the protein charge, hydration and affinity to the nanodiamonds. Small proteins (lysozyme) were found to form multilayers with significant conformational changes to screen the surface charge, while larger proteins (albumin) formed monolayers with minor conformational changes. The findings of this study provide a step forward toward understanding and eventually predicting nanoparticle interactions with biofluids.

  1. Maxwell's conjecture on three point charges with equal magnitudes

    NASA Astrophysics Data System (ADS)

    Tsai, Ya-Lun

    2015-08-01

    Maxwell's conjecture on three point charges states that the number of non-degenerate equilibrium points of the electrostatic field generated by them in R3 is at most four. We prove the conjecture in the cases when three point charges have equal magnitudes and show the number of isolated equilibrium points can only be zero, two, three, or four. Specifically, fixing positions of two positive charges in R3, we know exactly where to place the third positive charge to have two, three, or four equilibrium points. All equilibrium points are isolated and there are no other possibilities for the number of isolated equilibrium points. On the other hand, if both two of the fixed charges have negative charge values, there are always two equilibrium points except when the third positive charge lies in the line segment connecting the two negative charges. The exception cases are when the field contains only a curve of equilibrium points. In this paper, computations assisted by computer involve symbolic and exact integer computations. Therefore, all the results are proved rigorously.

  2. Evaluating stratiform cloud base charge remotely

    NASA Astrophysics Data System (ADS)

    Harrison, R. Giles; Nicoll, Keri A.; Aplin, Karen L.

    2017-06-01

    Stratiform clouds acquire charge at their upper and lower horizontal boundaries due to vertical current flow in the global electric circuit. Cloud charge is expected to influence microphysical processes, but understanding is restricted by the infrequent in situ measurements available. For stratiform cloud bases below 1 km in altitude, the cloud base charge modifies the surface electric field beneath, allowing a new method of remote determination. Combining continuous cloud height data during 2015-2016 from a laser ceilometer with electric field mill data, cloud base charge is derived using a horizontal charged disk model. The median daily cloud base charge density found was -0.86 nC m-2 from 43 days' data. This is consistent with a uniformly charged region 40 m thick at the cloud base, now confirming that negative cloud base charge is a common feature of terrestrial layer clouds. This technique can also be applied to planetary atmospheres and volcanic plumes.Plain Language SummaryThe idea that clouds in the atmosphere can <span class="hlt">charge</span> electrically has been appreciated since the time of Benjamin Franklin, but it is less widely recognized that it is not just thunderclouds which contain electric <span class="hlt">charge</span>. For example, water droplets in simple layer clouds, that are abundant and often responsible for an overcast day, carry electric <span class="hlt">charges</span>. The droplet <span class="hlt">charging</span> arises at the upper and lower edges of the layer cloud. This occurs because the small droplets at the edges draw <span class="hlt">charge</span> from the air outside the cloud. Understanding how strongly layer clouds <span class="hlt">charge</span> is important in evaluating electrical effects on the development of such clouds, for example, how thick the cloud becomes and whether it generates rain. Previously, cloud <span class="hlt">charge</span> measurement has required direct measurements within the cloud using weather balloons or aircraft. This work has monitored the lower cloud <span class="hlt">charge</span> continuously using instruments placed at the surface beneath</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1414691-direct-probing-polarization-charge-nanoscale-level','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1414691-direct-probing-polarization-charge-nanoscale-level"><span>Direct Probing of Polarization <span class="hlt">Charge</span> at Nanoscale Level</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Kwon, Owoong; Seol, Daehee; Lee, Dongkyu</p> <p></p> <p>Ferroelectric materials possess spontaneous polarization that can be used for multiple applications. Owing to a long-term development of reducing the sizes of devices, the preparation of ferroelectric materials and devices is entering the nanometer-scale regime. In order to evaluate the ferroelectricity, there is a need to investigate the polarization <span class="hlt">charge</span> at the nanoscale. Nonetheless, it is generally accepted that the detection of polarization <span class="hlt">charges</span> using a conventional conductive atomic force microscopy (CAFM) without a top electrode is not feasible because the nanometer-scale radius of an atomic force microscopy (AFM) tip yields a very low signal-to-noise ratio. But, the detection ismore » unrelated to the radius of an AFM tip and, in fact, a matter of the switched area. In this work, the direct probing of the polarization <span class="hlt">charge</span> at the nanoscale is demonstrated using the positive-up-<span class="hlt">negative</span>-down method based on the conventional CAFM approach without <span class="hlt">additional</span> corrections or circuits to reduce the parasitic capacitance. The polarization <span class="hlt">charge</span> densities of 73.7 and 119.0 µC cm -2 are successfully probed in ferroelectric nanocapacitors and thin films, respectively. The results we obtained show the feasibility of the evaluation of polarization <span class="hlt">charge</span> at the nanoscale and provide a new guideline for evaluating the ferroelectricity at the nanoscale.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010IJTFM.130..467A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010IJTFM.130..467A"><span>Lightning Channels of Cloud-to-Ground Flashes Neutralizing Multiple <span class="hlt">Charge</span> Regions Inside Winter Thunderclouds</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Akita, Manabu; Yoshida, Satoru; Nakamura, Yoshitaka; Morimoto, Takeshi; Ushio, Tomoo; Kawasaki, Zen-Ichiro; Wang, Daohong</p> <p></p> <p>Lightning Research Group of Osaka University (LRG-OU) has been developing and improving the VHF broadband digital interferometer (DITF) for thunderstorm observations. It enables us to locate the impulsive VHF radiation sources caused by lightning discharges with extremely high resolutions. As a result of the VHF observations during the 2007-2008 winter season in the Japan Sea coastal area, cloud-to-ground (CG) flashes that neutralize multiple <span class="hlt">charge</span> regions inside thunderclouds are visualized by the VHF broadband DITF. The first flash is the positive CG flash that neutralizes multiple positive <span class="hlt">charge</span> regions in a flash. The second flash is the bipolar lightning flash that neutralizes both positive and <span class="hlt">negative</span> <span class="hlt">charge</span> inside thunderclouds. In the case of bipolar lightning flashes, some tens millisecond after the return strokes, the subsequent <span class="hlt">negative</span> breakdowns initiate from the proximities of the initiation points of the preceding <span class="hlt">negative</span> stepped leaders. It was also found that the altitudes of <span class="hlt">negative</span> <span class="hlt">charge</span> regions are lower than 2km. The bipolar lightning flashes observed in this campaign neutralize positive <span class="hlt">charge</span> after lowering the <span class="hlt">negative</span> <span class="hlt">charge</span> to the ground.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27143357','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27143357"><span><span class="hlt">Charged</span> Residues at the First Transmembrane Region Contribute to the Voltage Dependence of the Slow Gate of Connexins.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Pinto, Bernardo I; García, Isaac E; Pupo, Amaury; Retamal, Mauricio A; Martínez, Agustín D; Latorre, Ramón; González, Carlos</p> <p>2016-07-22</p> <p>Connexins (Cxs) are a family of membrane-spanning proteins that form gap junction channels and hemichannels. Connexin-based channels exhibit two distinct voltage-dependent gating mechanisms termed slow and fast gating. Residues located at the C terminus of the first transmembrane segment (TM-1) are important structural components of the slow gate. Here, we determined the role of the <span class="hlt">charged</span> residues at the end of TM-1 in voltage sensing in Cx26, Cx46, and Cx50. Conductance/voltage curves obtained from tail currents together with kinetics analysis reveal that the fast and slow gates of Cx26 involves the movement of two and four <span class="hlt">charges</span> across the electric field, respectively. Primary sequence alignment of different Cxs shows the presence of well conserved glutamate residues in the C terminus of TM-1; only Cx26 contains a lysine in that position (lysine 41). Neutralization of lysine 41 in Cx26 increases the voltage dependence of the slow gate. Swapping of lysine 41 with glutamate 42 maintains the voltage dependence. In Cx46, neutralization of <span class="hlt">negative</span> <span class="hlt">charges</span> or <span class="hlt">addition</span> of a positive <span class="hlt">charge</span> in the Cx26 equivalent region reduced the slow gate voltage dependence. In Cx50, the <span class="hlt">addition</span> of a glutamate in the same region decreased the voltage dependence, and the neutralization of a <span class="hlt">negative</span> <span class="hlt">charge</span> increased it. These results indicate that the <span class="hlt">charges</span> at the end of TM-1 are part of the slow gate voltage sensor in Cxs. The fact that Cx42, which has no <span class="hlt">charge</span> in this region, still presents voltage-dependent slow gating suggests that <span class="hlt">charges</span> still unidentified also contribute to the slow gate voltage sensitivity. © 2016 by The American Society for Biochemistry and Molecular Biology, Inc.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015Nanos...7.5726A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015Nanos...7.5726A"><span>Surface <span class="hlt">charge</span> effects in protein adsorption on nanodiamonds</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Aramesh, M.; Shimoni, O.; Ostrikov, K.; Prawer, S.; Cervenka, J.</p> <p>2015-03-01</p> <p>Understanding the interaction of proteins with <span class="hlt">charged</span> diamond nanoparticles is of fundamental importance for diverse biomedical applications. Here we present a thorough study of protein binding, adsorption kinetics and structure on strongly positively (hydrogen-terminated) and <span class="hlt">negatively</span> (oxygen-terminated) <span class="hlt">charged</span> nanodiamond particles using a quartz crystal microbalance by dissipation and infrared spectroscopy. By using two model proteins (bovine serum albumin and lysozyme) of different properties (<span class="hlt">charge</span>, molecular weight and rigidity), the main driving mechanism responsible for the protein binding to the <span class="hlt">charged</span> nanoparticles was identified. Electrostatic interactions were found to dominate the protein adsorption dynamics, attachment and conformation. We developed a simple electrostatic model that can qualitatively explain the observed adsorption behaviour based on <span class="hlt">charge</span>-induced pH modifications near the <span class="hlt">charged</span> nanoparticle surfaces. Under neutral conditions, the local pH around the positively and <span class="hlt">negatively</span> <span class="hlt">charged</span> nanodiamonds becomes very high (11-12) and low (1-3) respectively, which has a profound impact on the protein <span class="hlt">charge</span>, hydration and affinity to the nanodiamonds. Small proteins (lysozyme) were found to form multilayers with significant conformational changes to screen the surface <span class="hlt">charge</span>, while larger proteins (albumin) formed monolayers with minor conformational changes. The findings of this study provide a step forward toward understanding and eventually predicting nanoparticle interactions with biofluids.Understanding the interaction of proteins with <span class="hlt">charged</span> diamond nanoparticles is of fundamental importance for diverse biomedical applications. Here we present a thorough study of protein binding, adsorption kinetics and structure on strongly positively (hydrogen-terminated) and <span class="hlt">negatively</span> (oxygen-terminated) <span class="hlt">charged</span> nanodiamond particles using a quartz crystal microbalance by dissipation and infrared spectroscopy. By using two model proteins</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015Nanos...7.7942Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015Nanos...7.7942Z"><span>Intracellular sorting of differently <span class="hlt">charged</span> chitosan derivatives and chitosan-based nanoparticles</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zubareva, A. A.; Shcherbinina, T. S.; Varlamov, V. P.; Svirshchevskaya, E. V.</p> <p>2015-04-01</p> <p>Chitosan (Chi) is a biodegradable nontoxic polycation with multiple reactive groups that is easily used to obtain derivatives with a desired <span class="hlt">charge</span> and hydrophobic properties. The aim of this work was to study the intracellular traffic of positively <span class="hlt">charged</span> hexanoyl-chitosan (HC) or HC-based nanoparticles (HCNPs) and <span class="hlt">negatively</span> <span class="hlt">charged</span> succinoyl-chitosan (SC) and SCNPs in epithelial and macrophage cell lines. By using flow cytometry we demonstrated that positively <span class="hlt">charged</span> HC adhered to cell membranes quicker and more efficiently than <span class="hlt">negatively</span> <span class="hlt">charged</span> SC or NPs. However confocal studies showed that SC and SCNPs penetrated cells much more efficiently than HC while HCNPs did not enter the epithelial cells. Macrophages also phagocyted better <span class="hlt">negatively</span> <span class="hlt">charged</span> material but were able to engulf both HC and HCNPs. Upon entering the cells, SC and SCNPs were co-localized with endosomes and lysosomes while HC was found in mitochondria and, to a lesser extent, in lysosomes of epithelial cells. Macrophages, RAW264.7, more efficiently transported all Chi samples to the lysosomal compartment while some positively <span class="hlt">charged</span> material was still found in mitochondria. Incubation of Chi derivatives and ChiNPs at pH specific to mitochondria (8.0) and lysosomes (4.5) demonstrated the neutralization of Chi <span class="hlt">charge</span>. We concluded that epithelial cells and, to a lesser extent, macrophages sort <span class="hlt">charged</span> material to the organelles neutralizing Chi <span class="hlt">charge</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29869883','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29869883"><span>Atomic Force Microscopy Study on the Stiffness of Nanosized Liposomes Containing <span class="hlt">Charged</span> Lipids.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Takechi-Haraya, Yuki; Goda, Yukihiro; Sakai-Kato, Kumiko</p> <p>2018-06-18</p> <p>It has recently been recognized that the mechanical properties of lipid nanoparticles play an important role during in vitro and in vivo behaviors such as cellular uptake, blood circulation, and biodistribution. However, there have been no quantitative investigations of the effect of commonly used <span class="hlt">charged</span> lipids on the stiffness of nanosized liposomes. In this study, by means of atomic force microscopy (AFM), we quantified the stiffness of nanosized liposomes composed of neutrally <span class="hlt">charged</span> lipids combined with positively or <span class="hlt">negatively</span> <span class="hlt">charged</span> lipids while simultaneously imaging the liposomes in aqueous medium. Our results showed that <span class="hlt">charged</span> lipids, whether <span class="hlt">negatively</span> or positively <span class="hlt">charged</span>, have the effect of reducing the stiffness of nanosized liposomes, independently of the saturation degree of the lipid acyl chains; the measured stiffness values of liposomes containing <span class="hlt">charged</span> lipids are 30-60% lower than those of their neutral counterpart liposomes. In <span class="hlt">addition</span>, we demonstrated that the Laurdan generalized polarization values, which are related to the hydration degree of the liposomal membrane interface and often used as a qualitative indicator of liposomal membrane stiffness, do not directly correlate with the physical stiffness values of the liposomes prepared in this study. However, our results indicate that direct quantitative AFM measurement is a valuable method to gain molecular-scale information about how the hydration degree of liposomal interfaces reflects (or does not reflect) liposome stiffness as a macroscopic property. Our AFM method will contribute to the quantitative characterization of the nano-bio interaction of nanoparticles and to the optimization of the lipid composition of liposomes for clinical use.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1338193-reaction-space-analysis-homogeneous-charge-compression-ignition-combustion-varying-levels-fuel-stratification-under-positive-negative-valve-overlap-conditions','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1338193-reaction-space-analysis-homogeneous-charge-compression-ignition-combustion-varying-levels-fuel-stratification-under-positive-negative-valve-overlap-conditions"><span>Reaction-space analysis of homogeneous <span class="hlt">charge</span> compression ignition combustion with varying levels of fuel stratification under positive and <span class="hlt">negative</span> valve overlap conditions</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Kodavasal, Janardhan; Lavoie, George A.; Assanis, Dennis N.; ...</p> <p>2015-10-26</p> <p>Full-cycle computational fluid dynamics simulations with gasoline chemical kinetics were performed to determine the impact of breathing and fuel injection strategies on thermal and compositional stratification, combustion and emissions during homogeneous <span class="hlt">charge</span> compression ignition combustion. The simulations examined positive valve overlap and <span class="hlt">negative</span> valve overlap strategies, along with fueling by port fuel injection and direct injection. The resulting <span class="hlt">charge</span> mass distributions were analyzed prior to ignition using ignition delay as a reactivity metric. The reactivity stratification arising from differences in the distributions of fuel–oxygen equivalence ratio (Φ FO), oxygen molar fraction (χ O2) and temperature (T) was determined for threemore » parametric studies. In the first study, the reactivity stratification and burn duration for positive valve overlap valve events with port fuel injection and early direct injection were nearly identical and were dominated by wall-driven thermal stratification. nitrogen oxide (NO) and carbon monoxide (CO) emissions were negligible for both injection strategies. In the second study, which examined <span class="hlt">negative</span> valve overlap valve events with direct injection and port fuel injection, reactivity stratification increased for direct injection as the Φ FO and T distributions associated with direct fuel injection into the hot residual gas were positively correlated; however, the latent heat absorbed from the hot residual gas by the evaporating direct injection fuel jet reduced the overall thermal and reactivity stratification. These stratification effects were offsetting, resulting in similar reactivity stratification and burn durations for the two injection strategies. The higher local burned gas temperatures with direct injection resulted in an order of magnitude increase in NO, while incomplete combustion of locally over-lean regions led to a sevenfold increase in CO emissions compared to port fuel injection. The final</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015ApPhL.106t1601W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015ApPhL.106t1601W"><span>Tantalum oxide/silicon nitride: A <span class="hlt">negatively</span> <span class="hlt">charged</span> surface passivation stack for silicon solar cells</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wan, Yimao; Bullock, James; Cuevas, Andres</p> <p>2015-05-01</p> <p>This letter reports effective passivation of crystalline silicon (c-Si) surfaces by thermal atomic layer deposited tantalum oxide (Ta2O5) underneath plasma enhanced chemical vapour deposited silicon nitride (SiNx). Cross-sectional transmission electron microscopy imaging shows an approximately 2 nm thick interfacial layer between Ta2O5 and c-Si. Surface recombination velocities as low as 5.0 cm/s and 3.2 cm/s are attained on p-type 0.8 Ω.cm and n-type 1.0 Ω.cm c-Si wafers, respectively. Recombination current densities of 25 fA/cm2 and 68 fA/cm2 are measured on 150 Ω/sq boron-diffused p+ and 120 Ω/sq phosphorus-diffused n+ c-Si, respectively. Capacitance-voltage measurements reveal a <span class="hlt">negative</span> fixed insulator <span class="hlt">charge</span> density of -1.8 × 1012 cm-2 for the Ta2O5 film and -1.0 × 1012 cm-2 for the Ta2O5/SiNx stack. The Ta2O5/SiNx stack is demonstrated to be an excellent candidate for surface passivation of high efficiency silicon solar cells.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28766928','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28766928"><span>Unusual Passivation Ability of Superconcentrated Electrolytes toward Hard Carbon <span class="hlt">Negative</span> Electrodes in Sodium-Ion Batteries.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Takada, Koji; Yamada, Yuki; Watanabe, Eriko; Wang, Jianhui; Sodeyama, Keitaro; Tateyama, Yoshitaka; Hirata, Kazuhisa; Kawase, Takeo; Yamada, Atsuo</p> <p>2017-10-04</p> <p>The passivation of <span class="hlt">negative</span> electrodes is key to achieving prolonged <span class="hlt">charge</span>-discharge cycling with Na-ion batteries. Here, we report the unusual passivation ability of superconcentrated Na-salt electrolytes. For example, a 50 mol % sodium bis(fluorosulfonyl)amide (NaFSA)/succinonitrile (SN) electrolyte enables highly reversible Na + insertion into a hard carbon <span class="hlt">negative</span> electrode without any electrolyte <span class="hlt">additive</span>, functional binder, or electrode pretreatment. Importantly, an anion-derived passivation film is formed via preferential reduction of the anion upon <span class="hlt">charging</span>, which can effectively suppress further electrolyte reduction. As a structural characteristic of the electrolyte, most anions are coordinated to multiple Na + cations at high concentration, which shifts the lowest unoccupied molecular orbitals of the anions downward, resulting in preferential anion reduction. The present work provides a new understanding of the passivation mechanism with respect to the coordination state of the anion.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvA..97d2704Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvA..97d2704Z"><span>Transmission of low-energy <span class="hlt">negative</span> ions through insulating nanocapillaries</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Qi; Liu, Zhonglin; Li, Pengfei; Jin, Bo; Song, Guangyin; Jin, Dingkun; Niu, Ben; Wei, Long; Ha, Shuai; Xie, Yiming; Ma, Yue; Wan, Chengliang; Cui, Ying; Zhou, Peng; Zhang, Hongqiang; Chen, Ximeng</p> <p>2018-04-01</p> <p>A simulation is performed to study the transmission of low-energy C l- ions through A l2O3 nanocapillaries. For the trajectory simulations, there are several processes involved: the image forces induced by the projectile; the electrostatic force from the deposited <span class="hlt">charges</span>; the scattering from the inner surface and <span class="hlt">charge</span> exchange. The simulation reproduces the main features of the experiments; i.e., the double peak structure in the transmitted angular distribution and the transmitted fractions of C l- , C l+ , and C l0 were found in the <span class="hlt">charge</span> state distribution. The transmitted C l- ions are centered around the beam direction while the transmitted fractions of C l0 and C l+ are centered around the tilt angles. The role of the deposited <span class="hlt">charge</span> is also studied by simulations. With the deposited <span class="hlt">charge</span>, it is found that C l- is dominant in the transmission and the majority of the ions, centered around the tilt angle, are mainly from the single deflection by the <span class="hlt">negative</span> <span class="hlt">charge</span> patches on the inner surfaces of the capillaries, and only a few directly transmitted C l- ions are centered around the incident direction. There are also a few transmitted fractions of C l0 and C l+ from close surface scatterings. In the case that there are no <span class="hlt">negative</span> <span class="hlt">charge</span> patches, the simulation agrees with the experiment in detail: The majority of the directly transmitted C l- ions are centered around the incident direction while only a few scattered C l- ions are centered around the tilt angle from the single close collisions with the inner surfaces of the capillaries. There is a portion, comparable to the transmitted fraction of C l- , of the transmitted fractions of C l0 and C l+ , centered around the tilt angle, from the single scatterings with the inner surfaces of the capillaries. This confirms that at the present experimental conditions there are most probably no <span class="hlt">negative</span> <span class="hlt">charge</span> patches formed to guide the <span class="hlt">negative</span> ions through insulating A l2O3 nanocapillaries.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015Nanos...7.6612T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015Nanos...7.6612T"><span>Structure and properties of composite films formed by cellulose nanocrystals and <span class="hlt">charged</span> latex nanoparticles</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Thérien-Aubin, Héloïse; Lukach, Ariella; Pitch, Natalie; Kumacheva, Eugenia</p> <p>2015-04-01</p> <p>We report the structural and optical properties of composite films formed from mixed suspensions of cellulose nanocrystals (CNCs) and fluorescent latex nanoparticles (NPs). We explored the effect of NP concentration, size, surface <span class="hlt">charge</span>, glass transition temperature and film processing conditions on film structure and properties. The chiral nematic order, typical of CNC films, was preserved in films with up to 50 wt% of <span class="hlt">negatively-charged</span> latex NPs. Composite films were characterized by macroscopically close-to-uniform fluorescence, birefringence, and circular dichroism properties. In contrast, <span class="hlt">addition</span> of positively <span class="hlt">charged</span> latex NPs led to gelation of CNC-latex suspensions and disruption of the chiral nematic order in the composite films. Large latex NPs disrupted the chiral nematic order to a larger extend than small NPs. Furthermore, the glass transition of latex NPs had a dramatic effect on the structure of CNC-latex films. Latex particles in the rubbery state were easily incorporated in the ordered CNC matrix and improved the structural integrity of its chiral nematic phase.We report the structural and optical properties of composite films formed from mixed suspensions of cellulose nanocrystals (CNCs) and fluorescent latex nanoparticles (NPs). We explored the effect of NP concentration, size, surface <span class="hlt">charge</span>, glass transition temperature and film processing conditions on film structure and properties. The chiral nematic order, typical of CNC films, was preserved in films with up to 50 wt% of <span class="hlt">negatively-charged</span> latex NPs. Composite films were characterized by macroscopically close-to-uniform fluorescence, birefringence, and circular dichroism properties. In contrast, <span class="hlt">addition</span> of positively <span class="hlt">charged</span> latex NPs led to gelation of CNC-latex suspensions and disruption of the chiral nematic order in the composite films. Large latex NPs disrupted the chiral nematic order to a larger extend than small NPs. Furthermore, the glass transition of latex NPs had a dramatic</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015ApSS..356..325R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015ApSS..356..325R"><span><span class="hlt">Charge</span> properties and bacterial contact-killing of hyperbranched polyurea-polyethyleneimine coatings with various degrees of alkylation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Roest, Steven; van der Mei, Henny C.; Loontjens, Ton J. A.; Busscher, Henk J.</p> <p>2015-11-01</p> <p>Coatings of immobilized-quaternary-ammonium-ions (QUAT) uniquely kill adhering bacteria upon contact. QUAT-coatings require a minimal cationic-<span class="hlt">charge</span> surface density for effective contact-killing of adhering bacteria of around 1014 cm-2. Quaternization of nitrogen is generally achieved through alkylation. Here, we investigate the contribution of <span class="hlt">additional</span> alkylation with methyl-iodide to the cationic-<span class="hlt">charge</span> density of hexyl-bromide alkylated, hyperbranched polyurea-polyethyleneimine coatings measuring <span class="hlt">charge</span> density with fluorescein staining. X-ray-photoelectron-spectroscopy was used to determine the at.% alkylated-nitrogen. Also streaming potentials, water contact-angles and bacterial contact-killing were measured. Cationic-<span class="hlt">charge</span> density increased with methyl-iodide alkylation times up to 18 h, accompanied by an increase in the at.% alkylated-nitrogen. Zeta-potentials became more <span class="hlt">negative</span> upon alkylation as a result of shielding of cationiccharges by hydrophobic alkyl-chains. Contact-killing of Gram-positive Staphylococci only occurred when the cationic-<span class="hlt">charge</span> density exceeded 1016 cm-2 and was carried by alkylated-nitrogen (electron-binding energy 401.3 eV). Gram-<span class="hlt">negative</span> Escherichia coli was not killed upon contact with the coatings. There with this study reveals that cationic-<span class="hlt">charge</span> density is neither appropriate nor sufficient to determine the ability of QUAT-coatings to kill adhering bacteria. Alternatively, the at.% of alkylated-nitrogen at 401.3 eV is proposed, as it reflects both cationic-<span class="hlt">charge</span> and its carrier. The at.% N401.3 eV should be above 0.45 at.% for Gram-positive bacterial contact-killing.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JPCM...29t5501B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JPCM...29t5501B"><span>Diffusivity of the double <span class="hlt">negatively</span> <span class="hlt">charged</span> mono-vacancy in silicon</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bhoodoo, Chidanand; Vines, Lasse; Monakhov, Edouard; Svensson, Bengt Gunnar</p> <p>2017-05-01</p> <p>Lightly-doped silicon (Si) samples of n-type conductivity have been irradiated with 2.0 MeV {{\\text{H}}+} ions at a temperature of 30 K and characterized in situ by deep level transient spectroscopy (DLTS) measurements using an on-line setup. Migration of the Si mono-vacancy in its double <span class="hlt">negative</span> <span class="hlt">charge</span> state (V 2-) starts to occur at temperatures above  ˜70 K and is monitored via trapping of V 2- by interstitial oxygen impurity atoms ({{\\text{O}}i} ), leading to the growth of the prominent vacancy-oxygen (V\\text{O} ) center. The V\\text{O} center gives rise to an acceptor level located at  ˜0.17 eV below the conduction band edge (E c ) and is readily detected by DLTS measurements. Post-irradiation isothermal anneals at temperatures in the range of 70 to 90 K reveal first-order kinetics for the reaction {{V}2-}+{{\\text{O}}i}\\to V\\text{O} ≤ft(+ 2{{e}-}\\right) in both Czochralski-grown and Float-zone samples subjected to low fluences of {{\\text{H}}+} ions, i.e. the irradiation-induced V concentration is dilute (≤slant 1013 cm-3). On the basis of these kinetics data and the content of {{\\text{O}}i} , the diffusivity of V 2- can be determined quantitatively and is found to exhibit an activation energy for migration of  ˜0.18 eV with a pre-exponential factor of  ˜4× {{10}-3} cm2 s-1. The latter value evidences a simple jump process without any entropy effects for the motion of V 2-. No deep level in the bandgap to be associated with V 2- is observed but the results suggest that the level is situated deeper than  ˜0.19 eV below E c , corroborating results reported previously in the literature.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMAE21A..06G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMAE21A..06G"><span>A Model-Based Investigation of <span class="hlt">Charge</span>-Generation According to the Relative Diffusional Growth Rate Theory</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Glassmeier, F.; Arnold, L.; Lohmann, U.; Dietlicher, R.; Paukert, M.</p> <p>2016-12-01</p> <p>Our current understanding of <span class="hlt">charge</span> generation in thunderclouds is based on collisional <span class="hlt">charge</span> transfer between graupel and ice crystals in the presence of liquid water droplets as dominant mechanism. The physical process of <span class="hlt">charge</span> transfer and the sign of net <span class="hlt">charge</span> generated on graupel and ice crystals under different cloud conditions is not yet understood. The Relative-Diffusional-Growth-Rate (RDGR) theory (Baker et al. 1987) suggests that the particle with the faster diffusional radius growth is <span class="hlt">charged</span> positively. In this contribution, we use simulations of idealized thunderclouds with two-moment warm and cold cloud microphysics to generate realistic combinations of RDGR-parameters. We find that these realistic parameter combinations result in a relationship between sign of <span class="hlt">charge</span>, cloud temperature and effective water content that deviates from previous theoretical and laboratory studies. This deviation indicates that the RDGR theory is sensitive to correlations between parameters that occur in clouds but are not captured in studies that vary temperature and water content while keeping other parameters at fixed values. In <span class="hlt">addition</span>, our results suggest that diffusional growth from the riming-related local water vapor field, a key component of the RDGR theory, is negligible for realistic parameter combinations. Nevertheless, we confirm that the RDGR theory results in positive or <span class="hlt">negative</span> <span class="hlt">charging</span> of particles under different cloud conditions. Under specific conditions, <span class="hlt">charge</span> generation via the RDGR theory alone might thus be sufficient to explain tripolar <span class="hlt">charge</span> structures in thunderclouds. In general, however, <span class="hlt">additional</span> <span class="hlt">charge</span> generation mechanisms and adaptations to the RDGR theory that consider riming other than via local vapor deposition seem necessary.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3328702','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3328702"><span>Toward a Molecular Understanding of Protein Solubility: Increased <span class="hlt">Negative</span> Surface <span class="hlt">Charge</span> Correlates with Increased Solubility</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Kramer, Ryan M.; Shende, Varad R.; Motl, Nicole; Pace, C. Nick; Scholtz, J. Martin</p> <p>2012-01-01</p> <p>Protein solubility is a problem for many protein chemists, including structural biologists and developers of protein pharmaceuticals. Knowledge about how intrinsic factors influence solubility is limited due to the difficulty of obtaining quantitative solubility measurements. Solubility measurements in buffer alone are difficult to reproduce, because gels or supersaturated solutions often form, making it impossible to determine solubility values for many proteins. Protein precipitants can be used to obtain comparative solubility measurements and, in some cases, estimations of solubility in buffer alone. Protein precipitants fall into three broad classes: salts, long-chain polymers, and organic solvents. Here, we compare the use of representatives from two classes of precipitants, ammonium sulfate and polyethylene glycol 8000, by measuring the solubility of seven proteins. We find that increased <span class="hlt">negative</span> surface <span class="hlt">charge</span> correlates strongly with increased protein solubility and may be due to strong binding of water by the acidic amino acids. We also find that the solubility results obtained for the two different precipitants agree closely with each other, suggesting that the two precipitants probe similar properties that are relevant to solubility in buffer alone. PMID:22768947</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=benjamin+AND+franklin&id=EJ726091','ERIC'); return false;" href="https://eric.ed.gov/?q=benjamin+AND+franklin&id=EJ726091"><span>The Origins of Positive and <span class="hlt">Negative</span> in Electricity</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Jensen, William B.</p> <p>2005-01-01</p> <p>Benjamin Franklin first introduced the terms positive and <span class="hlt">negative</span> into electrical theory in the year 1747. The positive and <span class="hlt">negative</span> terms originally had nothing to do with inherent electrical <span class="hlt">charge</span>, but rather indicated which object had an excess of electrical fluid indicating positive, and which had a deficiency, indicating <span class="hlt">negative</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4042121','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4042121"><span>New insight into the spin-conserving excitation of the <span class="hlt">negatively</span> <span class="hlt">charged</span> nitrogen-vacancy center in diamond</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Deng, Bei; Zhang, R. Q.; Shi, X. Q.</p> <p>2014-01-01</p> <p>The <span class="hlt">negatively</span> <span class="hlt">charged</span> nitrogen-vacancy (N-V−) color center in diamond is an important solid-state single photon source for applications to quantum communication and distributed quantum computation. Its full usefulness relies on sufficient radiative emission of the optical photons which requires realizable control to enhance emission into the zero-phonon line (ZPL) but until now is still a challenge. Detailed understanding of the associated excitation process would be of essential importance for such objective. Here we report a theoretical work that probes the spin-conserving optical excitation of the N-V− center. Using density-functional-theory (DFT) calculations, we find that the ZPL and the phonon-side band (PSB) depend sensitively on the axial strain of the system. Besides, we find a relatively small PSB appearing at about 100 GPa in the emission spectrum at low temperatures, which provides a means to enhance the coherent emission of the N-V− center in quantum optical networks. PMID:24888367</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29068464','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29068464"><span>Atomic <span class="hlt">charges</span> of sulfur in ionic liquids: experiments and calculations.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Fogarty, Richard M; Rowe, Rebecca; Matthews, Richard P; Clough, Matthew T; Ashworth, Claire R; Brandt, Agnieszka; Corbett, Paul J; Palgrave, Robert G; Smith, Emily F; Bourne, Richard A; Chamberlain, Thomas W; Thompson, Paul B J; Hunt, Patricia A; Lovelock, Kevin R J</p> <p>2017-12-14</p> <p>Experimental near edge X-ray absorption fine structure (NEXAFS) spectra, X-ray photoelectron (XP) spectra and Auger electron spectra are reported for sulfur in ionic liquids (ILs) with a range of chemical structures. These values provide experimental measures of the atomic <span class="hlt">charge</span> in each IL and enable the evaluation of the suitability of NEXAFS spectroscopy and XPS for probing the relative atomic <span class="hlt">charge</span> of sulfur. In <span class="hlt">addition</span>, we use Auger electron spectroscopy to show that when XPS binding energies differ by less than 0.5 eV, conclusions on atomic <span class="hlt">charge</span> should be treated with caution. Our experimental data provides a benchmark for calculations of the atomic <span class="hlt">charge</span> of sulfur obtained using different methods. Atomic <span class="hlt">charges</span> were computed for lone ions and ion pairs, both in the gas phase (GP) and in a solvation model (SMD), with a wide range of ion pair conformers considered. Three methods were used to compute the atomic <span class="hlt">charges</span>: <span class="hlt">charges</span> from the electrostatic potential using a grid based method (ChelpG), natural bond orbital (NBO) population analysis and Bader's atoms in molecules (AIM) approach. By comparing the experimental and calculated measures of the atomic <span class="hlt">charge</span> of sulfur, we provide an order for the sulfur atoms, ranging from the most <span class="hlt">negative</span> to the most positive atomic <span class="hlt">charge</span>. Furthermore, we show that both ChelpG and NBO are reasonable methods for calculating the atomic <span class="hlt">charge</span> of sulfur in ILs, based on the agreement with both the XPS and NEXAFS spectroscopy results. However, the atomic <span class="hlt">charges</span> of sulfur derived from ChelpG are found to display significant, non-physical conformational dependence. Only small differences in individual atomic <span class="hlt">charge</span> of sulfur were observed between lone ion (GP) and ion pair IL(SMD) model systems, indicating that ion-ion interactions do not strongly influence individual atomic <span class="hlt">charges</span>.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li class="active"><span>10</span></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_10 --> <div id="page_11" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li class="active"><span>11</span></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="201"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/15875834','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/15875834"><span>Altering surface <span class="hlt">charge</span> nonuniformity on individual colloidal particles.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Feick, Jason D; Chukwumah, Nkiru; Noel, Alexandra E; Velegol, Darrell</p> <p>2004-04-13</p> <p><span class="hlt">Charge</span> nonuniformity (sigmazeta) was altered on individual polystyrene latex particles and measured using the novel experimental technique of rotational electrophoresis. It has recently been shown that unaltered sulfated latices often have significant <span class="hlt">charge</span> nonuniformity (sigmazeta = 100 mV) on individual particles. Here it is shown that anionic polyelectrolytes and surfactants reduce the native <span class="hlt">charge</span> nonuniformity on <span class="hlt">negatively</span> <span class="hlt">charged</span> particles by 80% (sigmazeta = 20 mV), even while leaving the average surface <span class="hlt">charge</span> density almost unchanged. Reduction of <span class="hlt">charge</span> uniformity occurs as large domains of nonuniformity are minimized, giving a more random distribution of <span class="hlt">charge</span> on individual particle surfaces. Targeted reduction of <span class="hlt">charge</span> nonuniformity opens new opportunities for the dispersion of nanoparticles and the oriented assembly of particles.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20040111082','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20040111082"><span>Instrumentation for Studies of Electron Emission and <span class="hlt">Charging</span> From Insulators</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Thomson, C. D.; Zavyalov, V.; Dennison, J. R.</p> <p>2004-01-01</p> <p>Making measurements of electron emission properties of insulators is difficult since insulators can <span class="hlt">charge</span> either <span class="hlt">negatively</span> or positively under <span class="hlt">charge</span> particle bombardment. In <span class="hlt">addition</span>, high incident energies or high fluences can result in modification of a material s conductivity, bulk and surface <span class="hlt">charge</span> profile, structural makeup through bond breaking and defect creation, and emission properties. We discuss here some of the <span class="hlt">charging</span> difficulties associated with making insulator-yield measurements and review the methods used in previous studies of electron emission from insulators. We present work undertaken by our group to make consistent and accurate measurements of the electron/ion yield properties for numerous thin-film and thick insulator materials using innovative instrumentation and techniques. We also summarize some of the necessary instrumentation developed for this purpose including fast response, low-noise, high-sensitivity ammeters; signal isolation and interface to standard computer data acquisition apparatus using opto-isolation, sample-and-hold, and boxcar integration techniques; computer control, automation and timing using Labview software; a multiple sample carousel; a pulsed, compact, low-energy, <span class="hlt">charge</span> neutralization electron flood gun; and pulsed visible and UV light neutralization sources. This work is supported through funding from the NASA Space Environments and Effects Program and the NASA Graduate Research Fellowship Program.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvP...9a4010C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvP...9a4010C"><span>Physical Origin of Transient <span class="hlt">Negative</span> Capacitance in a Ferroelectric Capacitor</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chang, Sou-Chi; Avci, Uygar E.; Nikonov, Dmitri E.; Manipatruni, Sasikanth; Young, Ian A.</p> <p>2018-01-01</p> <p>Transient <span class="hlt">negative</span> differential capacitance, the dynamic reversal of transient capacitance in an electrical circuit, is of highly technological and scientific interest since it probes the foundation of ferroelectricity. We study a resistor-ferroelectric capacitor (R -FEC) network through a series of coupled equations based on Kirchhoff's law, electrostatics, and Landau theory. We show that transient <span class="hlt">negative</span> capacitance (NC) in a R -FEC circuit originates from the mismatch in switching rate between the free <span class="hlt">charge</span> on the metal plate and the bound <span class="hlt">charge</span> in a ferroelectric (FE) capacitor during the polarization switching. This transient free <span class="hlt">charge</span>-polarization mismatch is driven by the <span class="hlt">negative</span> curvature of the FE free-energy landscape, and it is also analytically shown that a free-energy profile with a <span class="hlt">negative</span> curvature is the only physical system that can describe transient NC in a R -FEC circuit. Furthermore, transient NC induced by the free <span class="hlt">charge</span>-polarization mismatch is justified by its dependence on both external resistance and the intrinsic FE viscosity coefficient. The depolarization effect on FE capacitors emphasizes the importance of <span class="hlt">negative</span> curvature to transient NC and also implies that transient and steady-state NC cannot be observed in a FE capacitor simultaneously. Finally, using the transient NC measurements, a procedure to experimentally determine the viscosity coefficient is presented to provide more insight into the relation between transient NC and the FE free-energy profile.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AIPC.1581.1500Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AIPC.1581.1500Y"><span><span class="hlt">Negative</span> measurement sensitivity values of planar capacitive imaging probes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yin, Xiaokang; Chen, Guoming; Li, Wei; Hutchins, David</p> <p>2014-02-01</p> <p>The measurement sensitivity distribution of planar capacitive imaging (CI) probes describes how effectively each region in the sensing area is contributing to the measured <span class="hlt">charge</span> signal on the sensing electrode. It can be used to determine the imaging ability of a CI probe. It is found in previous work that, there are regions in the sensing area where the change of the <span class="hlt">charge</span> output and the change of targeting physical parameter are of opposite trends. This opposite correlation implies that the measurement sensitivity values in such regions are <span class="hlt">negative</span>. In this work, the cause of <span class="hlt">negative</span> sensitivity is discussed. Experiments are also designed and performed so as to verify the existence of <span class="hlt">negative</span> sensitivity and study the factors that may affect the <span class="hlt">negative</span> sensitivity distributions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017NRL....12..534T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017NRL....12..534T"><span><span class="hlt">Charge</span> Splitting In Situ Recorder (CSIR) for Real-Time Examination of Plasma <span class="hlt">Charging</span> Effect in FinFET BEOL Processes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tsai, Yi-Pei; Hsieh, Ting-Huan; Lin, Chrong Jung; King, Ya-Chin</p> <p>2017-09-01</p> <p>A novel device for monitoring plasma-induced damage in the back-end-of-line (BEOL) process with <span class="hlt">charge</span> splitting capability is first-time proposed and demonstrated. This novel <span class="hlt">charge</span> splitting in situ recorder (CSIR) can independently trace the amount and polarity of plasma <span class="hlt">charging</span> effects during the manufacturing process of advanced fin field-effect transistor (FinFET) circuits. Not only does it reveal the real-time and in situ plasma <span class="hlt">charging</span> levels on the antennas, but it also separates positive and <span class="hlt">negative</span> <span class="hlt">charging</span> effect and provides two independent readings. As CMOS technologies push for finer metal lines in the future, the new <span class="hlt">charge</span> separation scheme provides a powerful tool for BEOL process optimization and further device reliability improvements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/11736101','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/11736101"><span>Positively <span class="hlt">charged</span> particles in dusty plasmas.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Samarian, A A; Vaulina, O S; Nefedov, A P; Fortov, V E; James, B W; Petrov, O F</p> <p>2001-11-01</p> <p>The trapping of dust particles has been observed in a dc abnormal glow discharge dominated by electron attachment. A dust cloud of several tens of positively <span class="hlt">charged</span> particles was found to form in the anode sheath region. An analysis of the experimental conditions revealed that these particles were positively <span class="hlt">charged</span> due to emission process, in contrast to most other experiments on the levitation of dust particles in gas-discharge plasmas where <span class="hlt">negatively</span> <span class="hlt">charged</span> particles are found. An estimate of the particle <span class="hlt">charge</span>, taking into account the processes of photoelectron and secondary electron emission from the particle surface, is in agreement with the experimental measured values.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22530971','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22530971"><span>Triboelectricity: macroscopic <span class="hlt">charge</span> patterns formed by self-arraying ions on polymer surfaces.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Burgo, Thiago A L; Ducati, Telma R D; Francisco, Kelly R; Clinckspoor, Karl J; Galembeck, Fernando; Galembeck, Sergio E</p> <p>2012-05-15</p> <p>Tribocharged polymers display macroscopically patterned positive and <span class="hlt">negative</span> domains, verifying the fractal geometry of electrostatic mosaics previously detected by electric probe microscopy. Excess <span class="hlt">charge</span> on contacting polyethylene (PE) and polytetrafluoroethylene (PTFE) follows the triboelectric series but with one caveat: net <span class="hlt">charge</span> is the arithmetic sum of patterned positive and <span class="hlt">negative</span> <span class="hlt">charges</span>, as opposed to the usual assumption of uniform but opposite signal <span class="hlt">charging</span> on each surface. Extraction with n-hexane preferentially removes positive <span class="hlt">charges</span> from PTFE, while 1,1-difluoroethane and ethanol largely remove both positive and <span class="hlt">negative</span> <span class="hlt">charges</span>. Using suitable analytical techniques (electron energy-loss spectral imaging, infrared microspectrophotometry and carbonization/colorimetry) and theoretical calculations, the positive species were identified as hydrocarbocations and the <span class="hlt">negative</span> species were identified as fluorocarbanions. A comprehensive model is presented for PTFE tribocharging with PE: mechanochemical chain homolytic rupture is followed by electron transfer from hydrocarbon free radicals to the more electronegative fluorocarbon radicals. Polymer ions self-assemble according to Flory-Huggins theory, thus forming the experimentally observed macroscopic patterns. These results show that tribocharging can only be understood by considering the complex chemical events triggered by mechanical action, coupled to well-established physicochemical concepts. Patterned polymers can be cut and mounted to make macroscopic electrets and multipoles.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002JAP....92.3162D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002JAP....92.3162D"><span>Mobile <span class="hlt">charge</span>, soft breakdown, and self-healing in hydrogen silsesquioxane based intermetal dielectric</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Devine, R. A. B.</p> <p>2002-09-01</p> <p>The electrical characteristics of hydrogen silsesquioxane based flowable oxide (FOxregistered) films proposed for interconnect isolation applications have been studied. It is demonstrated that <span class="hlt">negative</span> and positive <span class="hlt">charges</span> exist in the as-made, cured films with densities of 0.95 x1012 and 1.5 x1012 cm-2, respectively for thicknesses of 114 nm. The <span class="hlt">negative</span> <span class="hlt">charges</span> can be removed from the films by application of modest electric fields (positive or <span class="hlt">negative</span>, approx1.75 MV cm-1). The positive <span class="hlt">charge</span> can be similarly displaced but not removed from the film; this results in time dependent relaxation and redistribution of the positive <span class="hlt">charge</span> if the films are left unbiased. Time dependent irreversible evolution of the leakage current under positive and <span class="hlt">negative</span> bias (approx3 MV cm-1) shows a slow breakdown phenomena. An unusual self-healing effect is evidenced in these films.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26921608','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26921608"><span><span class="hlt">Negatively-charged</span> residues in the polar carboxy-terminal region in FSP27 are indispensable for expanding lipid droplets.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Tamori, Yoshikazu; Tateya, Sanshiro; Ijuin, Takeshi; Nishimoto, Yuki; Nakajima, Shinsuke; Ogawa, Wataru</p> <p>2016-03-01</p> <p>FSP27 has an important role in large lipid droplet (LD) formation because it exchanges lipids at the contact site between LDs. In the present study, we clarify that the amino-terminal domain of FSP27 (amino acids 1-130) is dispensable for LD enlargement, although it accelerates LD growth. LD expansion depends on the carboxy-terminal domain of FSP27 (amino acids 131-239). Especially, the <span class="hlt">negative</span> <span class="hlt">charge</span> of the acidic residues (D215, E218, E219 and E220) in the polar carboxy-terminal region (amino acids 202-239) is essential for the enlargement of LD. We propose that the carboxy-terminal domain of FSP27 has a crucial role in LD expansion, whereas the amino-terminal domain only has a supportive role. © 2016 Federation of European Biochemical Societies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28812902','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28812902"><span><span class="hlt">Charge</span> Effects on the Efflorescence in Single Levitated Droplets.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Hermann, Gunter; Zhang, Yan; Wassermann, Bernhard; Fischer, Henry; Quennet, Marcel; Rühl, Eckart</p> <p>2017-09-14</p> <p>The influence of electrical excess <span class="hlt">charges</span> on the crystallization from supersaturated aqueous sodium chloride solutions is reported. This is accomplished by efflorescence studies on single levitated microdroplets using optical and electrodynamic levitation. Specifically, a strong increase in efflorescence humidity is observed as a function of the droplet's <span class="hlt">negative</span> excess <span class="hlt">charge</span>, ranging up to -2.1 pC, with a distinct threshold behavior, increasing the relative efflorescence humidity, at which spontaneous nucleation occurs, from 44% for the neutral microparticle to 60%. These findings are interpreted by using molecular dynamics simulations for determining plausible structural patterns located near the particle surface that could serve as suitable precursors for the formation of critical clusters overcoming the nucleation barrier. These results, facilitating heterogeneous nucleation in the case of <span class="hlt">negatively</span> <span class="hlt">charged</span> microparticles, are compared to recent work on <span class="hlt">charge</span>-induced nucleation of neat supercooled water, where a distinctly different nucleation behavior as a function of droplet <span class="hlt">charge</span> has been observed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25406110','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25406110"><span>Insight into acid-base nucleation experiments by comparison of the chemical composition of positive, <span class="hlt">negative</span>, and neutral clusters.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Bianchi, Federico; Praplan, Arnaud P; Sarnela, Nina; Dommen, Josef; Kürten, Andreas; Ortega, Ismael K; Schobesberger, Siegfried; Junninen, Heikki; Simon, Mario; Tröstl, Jasmin; Jokinen, Tuija; Sipilä, Mikko; Adamov, Alexey; Amorim, Antonio; Almeida, Joao; Breitenlechner, Martin; Duplissy, Jonathan; Ehrhart, Sebastian; Flagan, Richard C; Franchin, Alessandro; Hakala, Jani; Hansel, Armin; Heinritzi, Martin; Kangasluoma, Juha; Keskinen, Helmi; Kim, Jaeseok; Kirkby, Jasper; Laaksonen, Ari; Lawler, Michael J; Lehtipalo, Katrianne; Leiminger, Markus; Makhmutov, Vladimir; Mathot, Serge; Onnela, Antti; Petäjä, Tuukka; Riccobono, Francesco; Rissanen, Matti P; Rondo, Linda; Tomé, António; Virtanen, Annele; Viisanen, Yrjö; Williamson, Christina; Wimmer, Daniela; Winkler, Paul M; Ye, Penglin; Curtius, Joachim; Kulmala, Markku; Worsnop, Douglas R; Donahue, Neil M; Baltensperger, Urs</p> <p>2014-12-02</p> <p>We investigated the nucleation of sulfuric acid together with two bases (ammonia and dimethylamine), at the CLOUD chamber at CERN. The chemical composition of positive, <span class="hlt">negative</span>, and neutral clusters was studied using three Atmospheric Pressure interface-Time Of Flight (APi-TOF) mass spectrometers: two were operated in positive and <span class="hlt">negative</span> mode to detect the chamber ions, while the third was equipped with a nitrate ion chemical ionization source allowing detection of neutral clusters. Taking into account the possible fragmentation that can happen during the <span class="hlt">charging</span> of the ions or within the first stage of the mass spectrometer, the cluster formation proceeded via essentially one-to-one acid-base <span class="hlt">addition</span> for all of the clusters, independent of the type of the base. For the positive clusters, the <span class="hlt">charge</span> is carried by one excess protonated base, while for the <span class="hlt">negative</span> clusters it is carried by a deprotonated acid; the same is true for the neutral clusters after these have been ionized. During the experiments involving sulfuric acid and dimethylamine, it was possible to study the appearance time for all the clusters (positive, <span class="hlt">negative</span>, and neutral). It appeared that, after the formation of the clusters containing three molecules of sulfuric acid, the clusters grow at a similar speed, independent of their <span class="hlt">charge</span>. The growth rate is then probably limited by the arrival rate of sulfuric acid or cluster-cluster collision.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PSST...27fLT01Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PSST...27fLT01Z"><span>Formation of stable inverse sheath in ion–ion plasma by strong <span class="hlt">negative</span> ion emission</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Zhe; Wu, Bang; Yang, Shali; Zhang, Ya; Chen, Dezhi; Fan, Mingwu; Jiang, Wei</p> <p>2018-06-01</p> <p>The effect of strong <span class="hlt">charged</span> particle emission on plasma–wall interactions is a classical, yet unresolved question in plasma physics. Previous studies on secondary electron emission have shown that with different emission coefficients, there are classical, space-<span class="hlt">charge</span>-limited, and inverse sheaths. In this letter, we demonstrate that a stable ion–ion inverse sheath and ion–ion plasma are formed with strong surface emission of <span class="hlt">negative</span> ions. The continuous space-<span class="hlt">charge</span>-limited to inverse ion–ion sheath transition is observed, and the plasma near the surface consequently transforms into pure ion–ion plasma. The results may explain the long-puzzled experimental observation that the density of <span class="hlt">negative</span> ions depends on only <span class="hlt">charge</span> not mass in <span class="hlt">negative</span> ion sources.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20090007706&hterms=Koontz&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DKoontz','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20090007706&hterms=Koontz&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DKoontz"><span>Characterizing ISS <span class="hlt">Charging</span> Environments with On-Board Ionospheric Plasma Measurements</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Minow, Jospeh I.; Craven, Paul D.; Coffey, Victoria N.; Schneider, Todd A.; Vaughn, Jason A.; Wright Jr, Kenneth; Parker, Paul D.; Mikatarian, Ronald R.; Kramer, Leonard; Hartman, William A.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20090007706'); toggleEditAbsImage('author_20090007706_show'); toggleEditAbsImage('author_20090007706_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20090007706_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20090007706_hide"></p> <p>2008-01-01</p> <p><span class="hlt">Charging</span> of the International Space Station (ISS) is dominated by interactions of the biased United States (US) 160 volt solar arrays with the relatively high density, low temperature plasma environment in low Earth orbit. Conducting surfaces on the vehicle structure <span class="hlt">charge</span> <span class="hlt">negative</span> relative to the ambient plasma environment because ISS structure is grounded to the <span class="hlt">negative</span> end of the US solar arrays. Transient <span class="hlt">charging</span> peaks reaching potentials of some tens of volts <span class="hlt">negative</span> controlled by photovoltaic array current collection typically occur at orbital sunrise and sunset as well as near orbital noon. In <span class="hlt">addition</span>, surface potentials across the vehicle structure vary due to an induced v x B (dot) L voltage generated by the high speed motion of the conducting structure across the Earth's magnetic field. Induced voltages in low Earth orbit are typically only approx.0.4 volts/meter but the approx.100 meter scale dimensions of the ISS yield maximum induced potential variations ofapprox.40 volts across the vehicle. Induced voltages are variable due to the orientation of the vehicle structure and orbital velocity vector with respect to the orientation of the Earth's magnetic field along the ISS orbit. In order to address the need to better understand the ISS spacecraft potential and plasma environments, NASA funded development and construction of the Floating Potential Measurement Unit (FPMU) which was deployed on an ISS starboard truss arm in August 2006. The suite of FPMU instruments includes two Langmuir probes, a plasma impedance probe, and a potential probe for use in in-situ monitoring of electron temperatures and densities and the vehicle potential relative to the plasma environment. This presentation will describe the use of the FPMU to better characterize interactions of the ISS with the space environment, changes in ISS <span class="hlt">charging</span> as the vehicle configuration is modified during ISS construction, and contributions of FPMU vehicle potential and plasma environment</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20090007660','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20090007660"><span>Bounding Extreme Spacecraft <span class="hlt">Charging</span> in the Lunar Environment</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Minow, Joseph I.; Parker, Linda N.</p> <p>2008-01-01</p> <p>Robotic and manned spacecraft from the Apollo era demonstrated that the lunar surface in daylight will <span class="hlt">charge</span> to positive potentials of a few tens of volts because the photoelectron current dominates the <span class="hlt">charging</span> process. In contrast, potentials of the lunar surface in darkness which were predicted to be on the order of a hundred volts <span class="hlt">negative</span> in the Apollo era have been shown more recently to reach values of a few hundred volts <span class="hlt">negative</span> with extremes on the order of a few kilovolts. The recent measurements of night time lunar surface potentials are based on electron beams in the Lunar Prospector Electron Reflectometer data sets interpreted as evidence for secondary electrons generated on the lunar surface accelerated through a plasma sheath from a <span class="hlt">negatively</span> <span class="hlt">charged</span> lunar surface. The spacecraft potential was not evaluated in these observations and therefore represents a lower limit to the magnitude of the lunar <span class="hlt">negative</span> surface potential. This paper will describe a method for obtaining bounds on the magnitude of lunar surface potentials from spacecraft measurements in low lunar orbit based on estimates of the spacecraft potential. We first use Nascap-2k surface <span class="hlt">charging</span> analyses to evaluate potentials of spacecraft in low lunar orbit and then include the potential drops between the ambient space environment and the spacecraft to the potential drop between the lunar surface and the ambient space environment to estimate the lunar surface potential from the satellite measurements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007nrao.pres...15.','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007nrao.pres...15."><span>Interstellar Chemistry Gets More Complex With New <span class="hlt">Charged</span>-Molecule Discovery</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p></p> <p>2007-07-01</p> <p>Astronomers using data from the National Science Foundation's Robert C. Byrd Green Bank Telescope (GBT) have found the largest <span class="hlt">negatively-charged</span> molecule yet seen in space. The discovery of the third <span class="hlt">negatively-charged</span> molecule, called an anion, in less than a year and the size of the latest anion will force a drastic revision of theoretical models of interstellar chemistry, the astronomers say. Molecule formation Formation Process of Large, <span class="hlt">Negatively-Charged</span> Molecule in Interstellar Space CREDIT: Bill Saxton, NRAO/AUI/NSF Click on image for page of graphics and detailed information "This discovery continues to add to the diversity and complexity that is already seen in the chemistry of interstellar space," said Anthony J. Remijan of the National Radio Astronomy Observatory (NRAO). "It also adds to the number of paths available for making the complex organic molecules and other large molecular species that may be precursors to life in the giant clouds from which stars and planets are formed," he added. Two teams of scientists found <span class="hlt">negatively-charged</span> octatetraynyl, a chain of eight carbon atoms and one hydrogen atom, in the envelope of gas around an old, evolved star and in a cold, dark cloud of molecular gas. In both cases, the molecule had an extra electron, giving it a <span class="hlt">negative</span> <span class="hlt">charge</span>. About 130 neutral and about a dozen positively-<span class="hlt">charged</span> molecules have been discovered in space, but the first <span class="hlt">negatively-charged</span> molecule was not discovered until late last year. The largest previously-discovered <span class="hlt">negative</span> ion found in space has six carbon atoms and one hydrogen atom. "Until recently, many theoretical models of how chemical reactions evolve in interstellar space have largely neglected the presence of anions. This can no longer be the case, and this means that there are many more ways to build large organic molecules in cosmic environments than have been explored," said Jan M. Hollis of NASA's Goddard Space Flight Center (GSFC). Ultraviolet light from stars can</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JAP...120e5102H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JAP...120e5102H"><span>The effects of nanoparticles and organic <span class="hlt">additives</span> with controlled dispersion on dielectric properties of polymers: <span class="hlt">Charge</span> trapping and impact excitation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Huang, Yanhui; Wu, Ke; Bell, Michael; Oakes, Andrew; Ratcliff, Tyree; Lanzillo, Nicholas A.; Breneman, Curt; Benicewicz, Brian C.; Schadler, Linda S.</p> <p>2016-08-01</p> <p>This work presents a comprehensive investigation into the effects of nanoparticles and organic <span class="hlt">additives</span> on the dielectric properties of insulating polymers using reinforced silicone rubber as a model system. TiO2 and ZrO2 nanoparticles (d = 5 nm) were well dispersed into the polymer via a bimodal surface modification approach. Organic molecules with the potential of voltage stabilization were further grafted to the nanoparticle to ensure their dispersion. These extrinsic species were found to provide deep traps for <span class="hlt">charge</span> carriers and exhibited effective <span class="hlt">charge</span> trapping properties at a rather small concentration (˜1017 cm-3). The <span class="hlt">charge</span> trapping is found to have the most significant effect on breakdown strength when the electrical stressing time is long enough that most <span class="hlt">charges</span> are trapped in the deep states. To establish a quantitative correlation between the trap depth and the molecular properties, the electron affinity and ionization energy of each species were calculated by an ab initio method and were compared with the experimentally measured values. The correlation however remains elusive and is possibly complicated by the field effect and the electronic interactions between different species that are not considered in this computation. At high field, a super-linear increase of current density was observed for TiO2 filled composites and is likely caused by impact excitation due to the low excitation energy of TiO2 compared to ZrO2. It is reasoned that the hot <span class="hlt">charge</span> carriers with energies greater than the excitation energy of TiO2 may excite an electron-hole pair upon collision with the NP, which later will be dissociated and contribute to free <span class="hlt">charge</span> carriers. This mechanism can enhance the energy dissipation and may account for the retarded electrical degradation and breakdown of TiO2 composites.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28537075','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28537075"><span>Borophene as a Promising Material for <span class="hlt">Charge</span>-Modulated Switchable CO2 Capture.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Tan, Xin; Tahini, Hassan A; Smith, Sean C</p> <p>2017-06-14</p> <p>Ideal carbon dioxide (CO 2 ) capture materials for practical applications should bind CO 2 molecules neither too weakly to limit good loading kinetics nor too strongly to limit facile release. Although <span class="hlt">charge</span>-modulated switchable CO 2 capture has been proposed to be a controllable, highly selective, and reversible CO 2 capture strategy, the development of a practical gas-adsorbent material remains a great challenge. In this study, by means of density functional theory (DFT) calculations, we have examined the possibility of conductive borophene nanosheets as promising sorbent materials for <span class="hlt">charge</span>-modulated switchable CO 2 capture. Our results reveal that the binding strength of CO 2 molecules on <span class="hlt">negatively</span> <span class="hlt">charged</span> borophene can be significantly enhanced by injecting extra electrons into the adsorbent. At saturation CO 2 capture coverage, the <span class="hlt">negatively</span> <span class="hlt">charged</span> borophene achieves CO 2 capture capacities up to 6.73 × 10 14 cm -2 . In contrast to the other CO 2 capture methods, the CO 2 capture/release processes on <span class="hlt">negatively</span> <span class="hlt">charged</span> borophene are reversible with fast kinetics and can be easily controlled via switching on/off the <span class="hlt">charges</span> carried by borophene nanosheets. Moreover, these <span class="hlt">negatively</span> <span class="hlt">charged</span> borophene nanosheets are highly selective for separating CO 2 from mixtures with CH 4 , H 2 , and/or N 2 . This theoretical exploration will provide helpful guidance for identifying experimentally feasible, controllable, highly selective, and high-capacity CO 2 capture materials with ideal thermodynamics and reversibility.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21393659','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21393659"><span>Proton transfer to <span class="hlt">charged</span> platinum electrodes. A molecular dynamics trajectory study.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wilhelm, Florian; Schmickler, Wolfgang; Spohr, Eckhard</p> <p>2010-05-05</p> <p>A recently developed empirical valence bond (EVB) model for proton transfer on Pt(111) electrodes (Wilhelm et al 2008 J. Phys. Chem. C 112 10814) has been applied in molecular dynamics (MD) simulations of a water film in contact with a <span class="hlt">charged</span> Pt surface. A total of seven <span class="hlt">negative</span> surface <span class="hlt">charge</span> densities σ between -7.5 and -18.9 µC cm(-2) were investigated. For each value of σ, between 30 and 84 initial conditions of a solvated proton within a water slab were sampled, and the trajectories were integrated until discharge of a proton occurred on the <span class="hlt">charged</span> surfaces. We have calculated the mean rates for discharge and for adsorption of solvated protons within the adsorbed water layer in contact with the metal electrode as a function of surface <span class="hlt">charge</span> density. For the less <span class="hlt">negative</span> values of σ we observe a Tafel-like exponential increase of discharge rate with decreasing σ. At the more <span class="hlt">negative</span> values this exponential increase levels off and the discharge process is apparently transport limited. Mechanistically, the Tafel regime corresponds to a stepwise proton transfer: first, a proton is transferred from the bulk into the contact water layer, which is followed by transfer of a proton to the <span class="hlt">charged</span> surface and concomitant discharge. At the more <span class="hlt">negative</span> surface <span class="hlt">charge</span> densities the proton transfer into the contact water layer and the transfer of another proton to the surface and its discharge occur almost simultaneously.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AIPA....8c5005M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AIPA....8c5005M"><span>The influence of ligand <span class="hlt">charge</span> and length on the assembly of Brome mosaic virus derived virus-like particles with magnetic core</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mieloch, Adam A.; Krecisz, Monika; Rybka, Jakub D.; Strugała, Aleksander; Krupiński, Michał; Urbanowicz, Anna; Kozak, Maciej; Skalski, Bohdan; Figlerowicz, Marek; Giersig, Michael</p> <p>2018-03-01</p> <p>Virus-like particles (VLPs) have sparked a great interest in the field of nanobiotechnology and nanomedicine. The introduction of superparamagnetic nanoparticles (SPIONs) as a core, provides potential use of VLPs in the hyperthermia therapy, MRI contrast agents and magnetically-powered delivery agents. Magnetite NPs also provide a significant improvement in terms of VLPs stability. Moreover employing viral structural proteins as self-assembling units has opened a new paths for targeted therapy, drug delivery systems, vaccines design, and many more. In many cases, the self-assembly of a virus strongly depends on electrostatic interactions between positively <span class="hlt">charged</span> groups of the capsid proteins and <span class="hlt">negatively</span> <span class="hlt">charged</span> nucleic acid. This phenomenon imposes the <span class="hlt">negative</span> net <span class="hlt">charge</span> as a key requirement for the core nanoparticle. In our experiments, Brome mosaic virus (BMV) capsid proteins isolated from infected plants Hordeum vulgare were used. Superparamagnetic iron oxide nanoparticles (Fe3O4) with 15 nm in diameter were synthesized by thermal decomposition and functionalized with COOH-PEG-PL polymer or dihexadecylphosphate (DHP) in order to provide water solubility and <span class="hlt">negative</span> <span class="hlt">charge</span> required for the assembly. Nanoparticles were characterized by Transmission Electron Microscopy (TEM), Dynamic Light Scattering (DLS), Zeta Potential, Fourier Transformed Infrared Spectroscopy (FTIR) and Superconducting Quantum Interference Device (SQUID) magnetometry. TEM and DLS study were conducted to verify VLPs creation. This study demonstrates that the increase of <span class="hlt">negative</span> surface <span class="hlt">charge</span> is not a sufficient factor determining successful assembly. <span class="hlt">Additional</span> steric interactions provided by longer ligands are crucial for the assembly of BMV SPION VLPs and may enhance the colloidal stability.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JPhD...49d5304Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JPhD...49d5304Z"><span>Comparison of the tribology performance of nano-diesel soot and graphite particles as lubricant <span class="hlt">additives</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Zu-chuan; Cai, Zhen-bing; Peng, Jin-fang; Zhu, Min-hao</p> <p>2016-02-01</p> <p>The tribology behavior of exhaust diesel soot as a lubricant <span class="hlt">additive</span> was investigated and then compared with that of a selection of commercial nano-graphite particles. Specifically, 0.01 wt% particles were dispersed in PAO4 oil with 1 wt% sorbitan monooleate (Span 80) as a dispersing agent, and wear tests based on the ball against plate mode were conducted at various temperatures. Different analytical techniques (e.g. transmission electron, scanning electron and infrared microscopy; energy dispersive x-ray and Raman spectroscopy; and <span class="hlt">charge</span> measurement) were employed to characterize the chemistry and morphology of the <span class="hlt">additives</span> and their tribology performance. The oil containing only 0.01 wt% diesel soot clearly improved wear resistance over 60 °C. In particular, at 100 °C the wear rate decreased by approximately 90% compared to the function of base oil. In the same test conditions, diesel soot exhibited better anti-wear performance than nano-graphite at high temperatures. The potential measure showed that the nano-graphite had positive <span class="hlt">charge</span> and the diesel soot had <span class="hlt">negative</span> <span class="hlt">charge</span>. Electrochemical action may play an important role in the lubricant mechanisms of diesel soot and graphite as oil <span class="hlt">additives</span>.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li class="active"><span>11</span></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_11 --> <div id="page_12" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li class="active"><span>12</span></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="221"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26076630','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26076630"><span>Integrating high electrical conductivity and photocatalytic activity in cotton fabric by cationizing for enriched coating of <span class="hlt">negatively</span> <span class="hlt">charged</span> graphene oxide.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Sahito, Iftikhar Ali; Sun, Kyung Chul; Arbab, Alvira Ayoub; Qadir, Muhammad Bilal; Jeong, Sung Hoon</p> <p>2015-10-05</p> <p>Electroconductive textiles have attended tremendous focus recently and researchers are making efforts to increase conductivity of e-textiles, in order to increase the use of such flexible and low cost textile materials. In this study, surface conductivity and photo catalytic activity of standard cotton fabric (SCF) was enhanced by modifying its surface <span class="hlt">charge</span>, from <span class="hlt">negative</span> to positive, using Bovine Serum Albumin (BSA) as a cationic agent, to convert it into cationised cotton fabric (CCF). Then, both types of fabrics were dip coated with a simple dip and dry technique for the adsorption of <span class="hlt">negatively</span> <span class="hlt">charged</span> graphene oxide (GO) sheets onto its surface. This resulted in 67.74% higher loading amount of GO on the CCF making self-assembly. Finally, this coating was chemically converted by vapor reduction using hydrazine hydrate to reduced graphene oxide (rGO) for restoration of a high electrical conductivity at the fabric surface. Our results revealed that with such high loading of GO, the surface resistance of CCF was only 40Ω/sq as compared to 510Ω/sq of the SCF and a 66% higher photo catalytic activity was also achieved through cationization for improved GO coating. Graphene coated SCF and CCF were characterized using FE-SEM, FTIR, Raman, UV-vis, WAXD, EDX and XPS spectroscopy to ascertain successful reduction of GO to rGO. The effect of BSA treatment on adsorption of cotton fabric was studied using drop shape analyzer to measure contact angle and for thermal and mechanical resistance, the fabric was tested for TGA and tensile strength, respectively. rGO coated fabric also showed slightly improved thermal stability yet a minor loss of strength was observed. The high flexibility, photocatalytic activity and excellent conductivity of this fabric suggests that it can be used as an electrode material for various applications. Copyright © 2015 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24492411','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24492411"><span><span class="hlt">Negative</span> electrospray ionization on porous supporting tips for mass spectrometric analysis: electrostatic <span class="hlt">charging</span> effect on detection sensitivity and its application to explosive detection.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wong, Melody Yee-Man; Man, Sin-Heng; Che, Chi-Ming; Lau, Kai-Chung; Ng, Kwan-Ming</p> <p>2014-03-21</p> <p>The simplicity and easy manipulation of a porous substrate-based ESI-MS technique have been widely applied to the direct analysis of different types of samples in positive ion mode. However, the study and application of this technique in <span class="hlt">negative</span> ion mode are sparse. A key challenge could be due to the ease of electrical discharge on supporting tips upon the application of <span class="hlt">negative</span> voltage. The aim of this study is to investigate the effect of supporting materials, including polyester, polyethylene and wood, on the detection sensitivity of a porous substrate-based <span class="hlt">negative</span> ESI-MS technique. By using nitrobenzene derivatives and nitrophenol derivatives as the target analytes, it was found that the hydrophobic materials (i.e., polyethylene and polyester) with a higher tendency to accumulate <span class="hlt">negative</span> <span class="hlt">charge</span> could enhance the detection sensitivity towards nitrobenzene derivatives via electron-capture ionization; whereas, compounds with electron affinities lower than the cut-off value (1.13 eV) were not detected. Nitrophenol derivatives with pKa smaller than 9.0 could be detected in the form of deprotonated ions; whereas polar materials (i.e., wood), which might undergo competitive deprotonation with the analytes, could suppress the detection sensitivity. With the investigation of the material effects on the detection sensitivity, the porous substrate-based <span class="hlt">negative</span> ESI-MS method was developed and applied to the direct detection of two commonly encountered explosives in complex samples.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140002385','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140002385"><span>Martian Atmospheric Pressure Static <span class="hlt">Charge</span> Elimination Tool</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Johansen, Michael R.</p> <p>2014-01-01</p> <p>A Martian pressure static <span class="hlt">charge</span> elimination tool is currently in development in the Electrostatics and Surface Physics Laboratory (ESPL) at NASA's Kennedy Space Center. In standard Earth atmosphere conditions, static <span class="hlt">charge</span> can be neutralized from an insulating surface using air ionizers. These air ionizers generate ions through corona breakdown. The Martian atmosphere is 7 Torr of mostly carbon dioxide, which makes it inherently difficult to use similar methods as those used for standard atmosphere static elimination tools. An initial prototype has been developed to show feasibility of static <span class="hlt">charge</span> elimination at low pressure, using corona discharge. A needle point and thin wire loop are used as the corona generating electrodes. A photo of the test apparatus is shown below. Positive and <span class="hlt">negative</span> high voltage pulses are sent to the needle point. This creates positive and <span class="hlt">negative</span> ions that can be used for static <span class="hlt">charge</span> neutralization. In a preliminary test, a floating metal plate was <span class="hlt">charged</span> to approximately 600 volts under Martian atmospheric conditions. The static elimination tool was enabled and the voltage on the metal plate dropped rapidly to -100 volts. This test data is displayed below. Optimization is necessary to improve the electrostatic balance of the static elimination tool.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27581395','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27581395"><span>Protein interactions with layers of TiO2 nanotube and nanopore arrays: Morphology and surface <span class="hlt">charge</span> influence.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kulkarni, Mukta; Mazare, Anca; Park, Jung; Gongadze, Ekaterina; Killian, Manuela Sonja; Kralj, Slavko; von der Mark, Klaus; Iglič, Aleš; Schmuki, Patrik</p> <p>2016-11-01</p> <p>In the present work we investigate the key factors involved in the interaction of small-sized <span class="hlt">charged</span> proteins with TiO 2 nanostructures, i.e. albumin (<span class="hlt">negatively</span> <span class="hlt">charged</span>), histone (positively <span class="hlt">charged</span>). We examine anodic nanotubes with specific morphology (simultaneous control over diameter and length, e.g. diameter - 15, 50 or 100nm, length - 250nm up to 10μm) and nanopores. The nanostructures surface area has a direct influence on the amount of bound protein, nonetheless the protein physical properties as electric <span class="hlt">charge</span> and size (in relation to nanotopography and biomaterial's electric <span class="hlt">charge</span>) are crucial too. The highest quantity of adsorbed protein is registered for histone, for 100nm diameter nanotubes (10μm length) while higher values are registered for 15nm diameter nanotubes when normalizing protein adsorption to nanostructures' surface unit area (evaluated from dye desorption measurements) - consistent with theoretical considerations. The proteins presence on the nanostructures is evaluated by XPS and ToF-SIMS; <span class="hlt">additionally</span>, we qualitatively assess their presence along the nanostructures length by ToF-SIMS depth profiles, with decreasing concentration towards the bottom. Surface nanostructuring of titanium biomedical devices with TiO 2 nanotubes was shown to significantly influence the adhesion, proliferation and differentiation of mesenchymal stem cells (and other cells too). A high level of control over the nanoscale topography and over the surface area of such 1D nanostructures enables a direct influence on protein adhesion. Herein, we investigate and show how the nanostructure morphology (nanotube diameter and length) influences the interactions with small-sized <span class="hlt">charged</span> proteins, using as model proteins bovine serum albumin (<span class="hlt">negatively</span> <span class="hlt">charged</span>) and histone (positively <span class="hlt">charged</span>). We show that the protein <span class="hlt">charge</span> strongly influences their adhesion to the TiO 2 nanostructures. Protein adhesion is quantified by ELISA measurements and determination of the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhDT.......151L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhDT.......151L"><span>Electrostatic <span class="hlt">Charging</span> and Particle Interactions in Microscopic Insulating Grains</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lee, Victor</p> <p></p> <p>In this thesis, we experimentally investigate the electrostatic <span class="hlt">charging</span> as well as the particle interactions in microscopic insulating grains. First, by tracking individual grains accelerated in an electric field, we quantitatively demonstrate that tribocharging of same-material grains depends on particle size. Large grains tend to <span class="hlt">charge</span> positively, and small ones tend to <span class="hlt">charge</span> <span class="hlt">negatively</span>. Theories based on the transfer of trapped electrons can explain this tendency but have not been validated. Here we show that the number of trapped electrons, measured independently by a thermoluminescence technique, is orders of magnitude too small to be responsible for the amount of <span class="hlt">charge</span> transferred. This result reveals that trapped electrons are not responsible for same-material tribocharging of dielectric particles. Second, same-material tribocharging in grains can result in important long-range electrostatic interactions. However, how these electrostatic interactions contribute to particle clustering remains elusive, primarily due to the lack of direct, detailed observations. Using a high-speed camera that falls with a stream <span class="hlt">charged</span> grains, we observe for the first time how <span class="hlt">charged</span> grains can undergo attractive as well as repulsive Kepler-like orbits. <span class="hlt">Charged</span> particles can be captured in their mutual electrostatic potential and form clusters via multiple bounces. Dielectric polarization effects are directly observed, which lead to <span class="hlt">additional</span> attractive forces and stabilize "molecule-like" arrangements of <span class="hlt">charged</span> particles. Third, we have developed a new method to study the <span class="hlt">charge</span> transfer of microscopic particles based on acoustic levitation techniques. This method allows us to narrow the complex problem of many-particle <span class="hlt">charging</span> down to precise <span class="hlt">charge</span> measurements of a single sub-millimeter particle colliding with a target plate. By simply attaching nonpolar groups onto glass surfaces, we show that the contact <span class="hlt">charging</span> of a particle is highly dependent on</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27642687','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27642687"><span>Intermolecular Interaction between Phosphatidylcholine and Sulfobetaine Lipid: A Combination of Lipids with Antiparallel Arranged Headgroup <span class="hlt">Charge</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Aikawa, Tatsuo; Yokota, Keisuke; Kondo, Takeshi; Yuasa, Makoto</p> <p>2016-10-05</p> <p>Intermolecular interactions between lipid molecules are important when designing lipid bilayer interfaces, which have many biomedical applications such as in drug delivery vehicles and biosensors. Phosphatidylcholine, a naturally occurring lipid, is the most common lipid found in organisms. Its chemical structure has a <span class="hlt">negatively</span> <span class="hlt">charged</span> phosphate linkage, adjacent to an ester linkage in a glycerol moiety, and a positively <span class="hlt">charged</span> choline group, placed at the terminus of the molecule. Recently, several types of synthetic lipids that have headgroups with the opposite <span class="hlt">charge</span> to that of phosphatidylcholine have emerged; that is, a positively <span class="hlt">charged</span> ammonium group is present adjacent to the ester linkage in their glycerol moiety and a <span class="hlt">negatively</span> <span class="hlt">charged</span> group is placed at their terminus. These types of lipids constitute a new class of soft material. The aim of this study was to determine how such lipids, with antiparallel arranged headgroup <span class="hlt">charge</span>, interact with naturally occurring phosphatidylcholines. We synthesized 1,2-dipalmitoyl-sn-glycero-3-sulfobetaine (DPSB) to represent a reversed-head lipid; 1,2-dipalmitoyl-sn-glycero-3-phosphatidylcholine (DPPC) was used to represent a naturally occurring phospholipid. The intermolecular interaction between these lipids was investigated using surface pressure-area (π-A) isotherms of the lipid monolayer at the air/water interface. We found that the extrapolated area and excess free energy of the mixed monolayer deviated <span class="hlt">negatively</span> when compared with the ideal values from <span class="hlt">additivity</span>. Moreover, differential scanning calorimetry of the lipid mixture in aqueous dispersion showed that the gel-to-liquid crystal transition temperature increased compared with that of each pure lipid composition. These results clearly indicate that DPSB preferably interacts with DPPC in the mixture. We believe that the attraction between the oppositely <span class="hlt">charged</span> headgroups of these lipids reinforces the intermolecular interaction. Our results provide</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..16.1599V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..16.1599V"><span>Dust Grain <span class="hlt">Charge</span> in the Lunar Environment</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vaverka, Jakub; Richterova, Ivana; Vysinka, Marek; Pavlu, Jiri; Safrankova, Jana; Nemecek, Zdenek</p> <p>2014-05-01</p> <p>Interaction of a lunar surface with solar wind and magnetosphere plasmas leads to it <span class="hlt">charging</span> by several processes as photoemission, a collection of primary particles and secondary electron emission. Nevertheless, <span class="hlt">charging</span> of the lunar surface is complicated by a presence of crustal magnetic anomalies with can generate a "mini-magnetosphere" capable for more or less complete shielding the surface. On the other hand, shielding of solar light and plasma particles by rocks and craters can also locally influence the surface potential as well as a presence of a plasma wake strongly changes this potential at the night side of the Moon. A typical surface potential varies from slightly positive (dayside) to <span class="hlt">negative</span> values of the order of several hundred of volts (night side). At the night side, <span class="hlt">negative</span> potentials can reach -4 kV during solar energetic particle (SEP) events. Recent measurements of the surface potential by Lunar Prospector and Artemis spacecraft have shown surprisingly high <span class="hlt">negative</span> dayside surface potentials (-500 V) during the magnetotail crossings as well as the positive surface potential higher than 100 V. One possible explanation is its non-monotonic profile above a surface where the potential minimum is formed by the space <span class="hlt">charge</span>. Dust grains presented in this complicated environment are also <span class="hlt">charged</span> by similar processes as the lunar surface. A strong dependence of the secondary electron yield on the grain size can significantly influence dust <span class="hlt">charging</span> mainly in the Earth's plasma sheet where an equilibrium grain potential can by different than the surface potential and can reach even the opposite sign. This process can lead to levitation of dust above a surface observed by the Surveyor spacecraft.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20090029274','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20090029274"><span>Modular Battery <span class="hlt">Charge</span> Controller</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Button, Robert; Gonzalez, Marcelo</p> <p>2009-01-01</p> <p>A new approach to masterless, distributed, digital-<span class="hlt">charge</span> control for batteries requiring <span class="hlt">charge</span> control has been developed and implemented. This approach is required in battery chemistries that need cell-level <span class="hlt">charge</span> control for safety and is characterized by the use of one controller per cell, resulting in redundant sensors for critical components, such as voltage, temperature, and current. The <span class="hlt">charge</span> controllers in a given battery interact in a masterless fashion for the purpose of cell balancing, <span class="hlt">charge</span> control, and state-of-<span class="hlt">charge</span> estimation. This makes the battery system invariably fault-tolerant. The solution to the single-fault failure, due to the use of a single <span class="hlt">charge</span> controller (CC), was solved by implementing one CC per cell and linking them via an isolated communication bus [e.g., controller area network (CAN)] in a masterless fashion so that the failure of one or more CCs will not impact the remaining functional CCs. Each micro-controller-based CC digitizes the cell voltage (V(sub cell)), two cell temperatures, and the voltage across the switch (V); the latter variable is used in conjunction with V(sub cell) to estimate the bypass current for a given bypass resistor. Furthermore, CC1 digitizes the battery current (I1) and battery voltage (V(sub batt) and CC5 digitizes a second battery current (I2). As a result, redundant readings are taken for temperature, battery current, and battery voltage through the summation of the individual cell voltages given that each CC knows the voltage of the other cells. For the purpose of cell balancing, each CC periodically and independently transmits its cell voltage and stores the received cell voltage of the other cells in an array. The position in the array depends on the identifier (ID) of the transmitting CC. After eight cell voltage receptions, the array is checked to see if one or more cells did not transmit. If one or more transmissions are missing, the missing cell(s) is (are) eliminated from cell</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1999APS..DPP.RP109S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1999APS..DPP.RP109S"><span>Strong Turbulence in Alkali Halide <span class="hlt">Negative</span> Ion Plasmas</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sheehan, Daniel</p> <p>1999-11-01</p> <p><span class="hlt">Negative</span> ion plasmas (NIPs) are <span class="hlt">charge</span>-neutral plasmas in which the <span class="hlt">negative</span> <span class="hlt">charge</span> is dominated by <span class="hlt">negative</span> ions rather than electrons. They are found in laser discharges, combustion products, semiconductor manufacturing processes, stellar atmospheres, pulsar magnetospheres, and the Earth's ionosphere, both naturally and man-made. They often display signatures of strong turbulence^1. Development of a novel, compact, unmagnetized alkali halide (MX) NIP source will be discussed, it incorporating a ohmically-heated incandescent (2500K) tantulum solenoid (3cm dia, 15 cm long) with heat shields. The solenoid ionizes the MX vapor and confines contaminant electrons, allowing a very dry (electron-free) source. Plasma densities of 10^10 cm-3 and positive to <span class="hlt">negative</span> ion mass ratios of 1 <= fracm_+m- <= 20 are achievable. The source will allow tests of strong turbulence theory^2. 1 Sheehan, D.P., et al., Phys. Fluids B5, 1593 (1993). 2 Tsytovich, V. and Wharton, C.W., Comm. Plasma Phys. Cont. Fusion 4, 91 (1978).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=electrostatic+AND+field&pg=3&id=EJ344430','ERIC'); return false;" href="https://eric.ed.gov/?q=electrostatic+AND+field&pg=3&id=EJ344430"><span>Trajectories of Moving <span class="hlt">Charges</span> in Static Electric Fields.</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Kirkup, L.</p> <p>1986-01-01</p> <p>Describes the implementation of a trajectory-plotting program for a microcomputer; shows how it may be used to demonstrate the focusing effect of a simple electrostatic lens. The computer program is listed and diagrams are included that show comparisons of trajectories of <span class="hlt">negative</span> <span class="hlt">charges</span> in the vicinity of positive <span class="hlt">charges</span>. (TW)</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29281243','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29281243"><span>Modulating the Electrochemical Performances of Layered Cathode Materials for Sodium Ion Batteries through Tuning Coulombic Repulsion between <span class="hlt">Negatively</span> <span class="hlt">Charged</span> TMO2 Slabs.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Li, Zheng-Yao; Wang, Huibo; Yang, Wenyun; Yang, Jinbo; Zheng, Lirong; Chen, Dongfeng; Sun, Kai; Han, Songbai; Liu, Xiangfeng</p> <p>2018-01-17</p> <p>Exploiting advanced layered transition metal oxide cathode materials is of great importance to rechargeable sodium batteries. Layered oxides are composed of <span class="hlt">negatively</span> <span class="hlt">charged</span> TMO 2 slabs (TM = transition metal) separated by Na + diffusion layers. Herein, we propose a novel insight, for the first time, to control the electrochemical properties by tuning Coulombic repulsion between <span class="hlt">negatively</span> <span class="hlt">charged</span> TMO 2 slabs. Coulombic repulsion can finely tailor the d-spacing of Na ion layers and material structural stability, which can be achieved by employing Na + cations to serve as effective shielding layers between TMO 2 layers. A series of O3-type Na x Mn 1/3 Fe 1/3 Cu 1/6 Mg 1/6 O 2 (x = 1.0, 0.9, 0.8, and 0.7) have been prepared, and Na 0.7 Mn 1/3 Fe 1/3 Cu 1/6 Mg 1/6 O 2 shows the largest Coulombic repulsion between TMO 2 layers, the largest space for Na ion diffusion, the best structural stability, and also the longest Na-O chemical bond with weaker Coulombic attraction, thus leading to the best electrochemical performance. Meanwhile, the thermal stability depends on the Na concentration in pristine materials. Ex situ X-ray absorption (XAS) analysis indicates that Mn, Fe, and Cu ions are all electrochemically active components during insertion and extraction of sodium ion. This study enables some new insights to promote the development of advanced layered Na x TMO 2 materials for rechargeable sodium batteries in the future.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25118339','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25118339"><span>Nanopipette delivery: influence of surface <span class="hlt">charge</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Shi, Wenqing; Sa, Niya; Thakar, Rahul; Baker, Lane A</p> <p>2015-07-21</p> <p>In this report, transport through a nanopipette is studied and the interplay between current rectification and ion delivery for small pipettes is examined. First, surface <span class="hlt">charge</span> dependence of concentration polarization effects in a quartz nanopipette was investigated. Electrical characterization was performed through current-potential (I-V) measurements. In <span class="hlt">addition</span>, fluorescein (an anionic fluorescent probe) was utilized to optically map ion enrichment and ion depletion in the nanopipette tip. Bare nanopipettes and polyethylenimine (PEI)-modified nanopipettes were examined. Results confirm that concentration polarization is a surface <span class="hlt">charge</span> dependent phenomenon and delivery can be controlled through modification of surface <span class="hlt">charge</span>. The relationship between concentration polarization effects and voltage-driven delivery of <span class="hlt">charged</span> electroactive species was investigated with a carbon ring/nanopore electrode fabricated from pyrolyzed parylene C (PPC). Factors such as surface <span class="hlt">charge</span> polarity of the nanopipette, electrolyte pH, and electrolyte concentration were investigated. Results indicate that with modification of surface <span class="hlt">charge</span>, <span class="hlt">additional</span> control over delivery of <span class="hlt">charged</span> species can be achieved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20701967','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20701967"><span>The influence of size and <span class="hlt">charge</span> of chitosan/polyglutamic acid hollow spheres on cellular internalization, viability and blood compatibility.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Dash, Biraja C; Réthoré, Gildas; Monaghan, Michael; Fitzgerald, Kathleen; Gallagher, William; Pandit, Abhay</p> <p>2010-11-01</p> <p>Polymeric hollow spheres can be tailored as efficient carriers of various therapeutic molecules due to their tunable properties. However, the entry of these synthetic vehicles into cells, their cell viability and blood compatibility depend on their physical and chemical properties e.g. size, surface <span class="hlt">charge</span>. Herein, we report the effect of size and surface <span class="hlt">charge</span> on cell viability and cellular internalization behaviour and their effect on various blood components using chitosan/polyglutamic acid hollow spheres as a model system. <span class="hlt">Negatively</span> <span class="hlt">charged</span> chitosan/polyglutamic acid hollow spheres of various sizes 100, 300, 500 and 1000 nm were fabricated using a template based method and covalently surface modified using linear polyethylene glycol and methoxyethanol amine to create a gradient of surface <span class="hlt">charge</span> from <span class="hlt">negative</span> to neutrally <span class="hlt">charged</span> spheres respectively. The results here suggest that both size and surface <span class="hlt">charge</span> have a significant influence on the sphere's behaviour, most prominently on haemolysis, platelet activation, plasma recalcification time, cell viability and internalization over time. <span class="hlt">Additionally</span>, cellular internalization behaviour and viability was found to vary with different cell types. These results are in agreement with those of inorganic spheres and liposomes, and can serve as guidelines for tailoring polymeric solid spheres for specific desired applications in biological and pharmaceutical fields, including the design of nanometer to submicron-sized delivery vehicles. Copyright (c) 2010 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1419770','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1419770"><span><span class="hlt">Charge</span> gradient microscopy</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Roelofs, Andreas; Hong, Seungbum</p> <p>2018-02-06</p> <p>A method for rapid imaging of a material specimen includes positioning a tip to contact the material specimen, and applying a force to a surface of the material specimen via the tip. In <span class="hlt">addition</span>, the method includes moving the tip across the surface of the material specimen while removing electrical <span class="hlt">charge</span> therefrom, generating a signal produced by contact between the tip and the surface, and detecting, based on the data, the removed electrical <span class="hlt">charge</span> induced through the tip during movement of the tip across the surface. The method further includes measuring the detected electrical <span class="hlt">charge</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20087768','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20087768"><span>Effect of surface <span class="hlt">charge</span> of immortalized mouse cerebral endothelial cell monolayer on transport of <span class="hlt">charged</span> solutes.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Yuan, Wei; Li, Guanglei; Gil, Eun Seok; Lowe, Tao Lu; Fu, Bingmei M</p> <p>2010-04-01</p> <p><span class="hlt">Charge</span> carried by the surface glycocalyx layer (SGL) of the cerebral endothelium has been shown to significantly modulate the permeability of the blood-brain barrier (BBB) to <span class="hlt">charged</span> solutes in vivo. The cultured monolayer of bEnd3, an immortalized mouse cerebral endothelial cell line, is becoming a popular in vitro BBB model due to its easy growth and maintenance of many BBB characteristics over repeated passages. To test whether the SGL of bEnd3 monolayer carries similar <span class="hlt">charge</span> as that in the intact BBB and quantify this <span class="hlt">charge</span>, which can be characterized by the SGL thickness (L(f)) and <span class="hlt">charge</span> density (C(mf)), we measured the solute permeability of bEnd3 monolayer to neutral solutes and to solutes with similar size but opposite <span class="hlt">charges</span>: <span class="hlt">negatively</span> <span class="hlt">charged</span> alpha-lactalbumin (-11) and positively <span class="hlt">charged</span> ribonuclease (+3). Combining the measured permeability data with a transport model across the cell monolayer, we predicted the L(f) and the C(mf) of bEnd3 monolayer, which is approximately 160 nm and approximately 25 mEq/L, respectively. We also investigated whether orosomucoid, a plasma glycoprotein modulating the <span class="hlt">charge</span> of the intact BBB, alters the <span class="hlt">charge</span> of bEnd3 monolayer. We found that 1 mg/mL orosomucoid would increase SGL <span class="hlt">charge</span> density of bEnd3 monolayer to approximately 2-fold of its control value.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2918278','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2918278"><span>Molecular and phenotypic aspects of CHD7 mutation in <span class="hlt">CHARGE</span> syndrome</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Zentner, Gabriel E.; Layman, Wanda S.; Martin, Donna M.; Scacheri, Peter C.</p> <p>2010-01-01</p> <p><span class="hlt">CHARGE</span> syndrome (Coloboma of the eye, Heart defects, Atresia of the choanae, Retardation of growth and/or development, Genital and/or urinary abnormalities, and Ear abnormalities (including deafness) is a genetic disorder characterized by a specific and a recognizable pattern of anomalies. De novo mutations in the gene encoding chromodomain helicase DNA binding protein 7 (CHD7) are the major cause of <span class="hlt">CHARGE</span> syndrome. Here, we review the clinical features of 379 <span class="hlt">CHARGE</span> patients who tested positive or <span class="hlt">negative</span> for mutations in CHD7. We found that <span class="hlt">CHARGE</span> individuals with CHD7 mutations more commonly have ocular colobomas, temporal bone anomalies (semicircular canal hypoplasia/dysplasia), and facial nerve paralysis compared with mutation <span class="hlt">negative</span> individuals. We also highlight recent genetic and genomic studies that have provided functional insights into CHD7 and the pathogenesis of <span class="hlt">CHARGE</span> syndrome. PMID:20186815</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20090033069&hterms=measurement+properties&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dmeasurement%2Bproperties','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20090033069&hterms=measurement+properties&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dmeasurement%2Bproperties"><span>Measurements of Lunar Dust <span class="hlt">Charging</span> Properties by Electron Impact</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Abbas, Mian M.; Tankosic, Dragana; Craven, Paul D.; Schneider, Todd A.; Vaughn, Jason A.; LeClair, Andre; Spann, James F.; Norwood, Joseph K.</p> <p>2009-01-01</p> <p>Dust grains in the lunar environment are believed to be electrostatically <span class="hlt">charged</span> predominantly by photoelectric emissions resulting from solar UV radiation on the dayside, and on the nightside by interaction with electrons in the solar wind plasma. In the high vacuum environment on the lunar surface with virtually no atmosphere, the positive and <span class="hlt">negative</span> <span class="hlt">charge</span> states of micron/submicron dust grains lead to some unusual physical and dynamical dust phenomena. Knowledge of the electrostatic <span class="hlt">charging</span> properties of dust grains in the lunar environment is required for addressing their hazardous effect on the humans and mechanical systems. It is well recognized that the <span class="hlt">charging</span> properties of individual small micron size dust grains are substantially different from the measurements on bulk materials. In this paper we present the results of measurements on <span class="hlt">charging</span> of individual Apollo 11 and Apollo 17 dust grains by exposing them to mono-energetic electron beams in the 10-100 eV energy range. The <span class="hlt">charging</span>/discharging rates of positively and <span class="hlt">negatively</span> <span class="hlt">charged</span> particles of approx. 0.1 to 5 micron radii are discussed in terms of the sticking efficiencies and secondary electron yields. The secondary electron emission process is found to be a complex and effective <span class="hlt">charging</span>/discharging mechanism for incident electron energies as low as 10-25 eV, with a strong dependence on particle size. Implications of the laboratory measurements on the nature of dust grain <span class="hlt">charging</span> in the lunar environment are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016APS..DPPPO7010H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016APS..DPPPO7010H"><span>Migration of Carbon Adatoms on the Surface of <span class="hlt">Charged</span> SWCNT</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Han, Longtao; Krstic, Predrag; Kaganovich, Igor</p> <p>2016-10-01</p> <p>In volume plasma, the growth of SWCNT from a transition metal catalyst could be enhanced by incoming carbon flux on SWCNT surface, which is generated by the adsorption and migration of carbon adatoms on SWCNT surface. In <span class="hlt">addition</span>, the nanotube can be <span class="hlt">charged</span> by the irradiation of plasma particles. How this <span class="hlt">charging</span> effect will influence the adsorption and migration behavior of carbon atom has not been revealed. Using Density Functional Theory, Nudged Elastic Band and Kinetic Monte Carlo method, we found equilibrium sites, vibrational frequency, adsorption energy, most probable pathways for migration of adatoms, and the barrier sizes along these pathways. The metallic (5,5) SWCNT can support a fast migration of the carbon adatom along a straight path with low barriers, which is further enhanced by the presence of <span class="hlt">negative</span> <span class="hlt">charge</span> on SWCNT. The enhancement is contributed by the higher adsorption energy and thence longer lifetime of adatom on the <span class="hlt">charged</span> SWCNT surface. The lifetime and migration distance of adatom increase by three and two orders of magnitude, respectively, as shown by Kinetic Monte Carlo simulation. These results support the surface migration mechanism of SWCNT growth in plasma environment. This work was supported by the U.S. Department of Energy, Office of Science, Basic Energy Sciences, Material Sciences and Engineering Division.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25548883','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25548883"><span>Magnetoresistance and <span class="hlt">charge</span> transport in graphene governed by nitrogen dopants.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Rein, Markus; Richter, Nils; Parvez, Khaled; Feng, Xinliang; Sachdev, Hermann; Kläui, Mathias; Müllen, Klaus</p> <p>2015-02-24</p> <p>We identify the influence of nitrogen-doping on <span class="hlt">charge</span>- and magnetotransport of single layer graphene by comparing doped and undoped samples. Both sample types are grown by chemical vapor deposition (CVD) and transferred in an identical process onto Si/SiO2 wafers. We characterize the samples by Raman spectroscopy as well as by variable temperature magnetotransport measurements. Over the entire temperature range, the <span class="hlt">charge</span> transport properties of all undoped samples are in line with literature values. The nitrogen doping instead leads to a 6-fold increase in the <span class="hlt">charge</span> carrier concentration up to 4 × 10(13) cm(-2) at room temperature, indicating highly effective doping. <span class="hlt">Additionally</span> it results in the opening of a <span class="hlt">charge</span> transport gap as revealed by the temperature dependence of the resistance. The magnetotransport exhibits a conspicuous sign change from positive Lorentz magnetoresistance (MR) in undoped to large <span class="hlt">negative</span> MR that we can attribute to the doping induced disorder. At low magnetic fields, we use quantum transport signals to quantify the transport properties. Analyses based on weak localization models allow us to determine an orders of magnitude decrease in the phase coherence and scattering times for doped samples, since the dopants act as effective scattering centers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25557761','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25557761"><span>Tuning transport selectivity of ionic species by phosphoric acid gradient in positively <span class="hlt">charged</span> nanochannel membranes.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Yang, Meng; Yang, Xiaohai; Wang, Kemin; Wang, Qing; Fan, Xin; Liu, Wei; Liu, Xizhen; Liu, Jianbo; Huang, Jin</p> <p>2015-02-03</p> <p>The transport of ionic species through a nanochannel plays important roles in fundamental research and practical applications of the nanofluidic device. Here, we demonstrated that ionic transport selectivity of a positively <span class="hlt">charged</span> nanochannel membrane can be tuned under a phosphoric acid gradient. When phosphoric acid solution and analyte solution were connected by the positively <span class="hlt">charged</span> nanochannel membrane, the faster-moving analyte through the positively <span class="hlt">charged</span> nanochannel membrane was the positively <span class="hlt">charged</span> dye (methylviologen, MV(2+)) instead of the <span class="hlt">negatively</span> <span class="hlt">charged</span> dye (1,5-naphthalene disulfonate, NDS(2-)). In other words, a reversed ion selectivity of the nanochannel membranes can be found. It can be explained as a result of the combination of diffusion, induced electroosmosis, and induced electrophoresis. In <span class="hlt">addition</span>, the influencing factors of transport selectivity, including concentration of phosphoric acid, penetration time, and volume of feed solution, were also investigated. The results showed that the transport selectivity can further be tuned by adjusting these factors. As a method of tuning ionic transport selectivity by establishing phosphoric acid gradient, it will be conducive to improving the separation of ionic species.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li class="active"><span>12</span></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_12 --> <div id="page_13" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li class="active"><span>13</span></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="241"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004JPhD...37..353F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004JPhD...37..353F"><span>Improved levitation and trapping of particles by <span class="hlt">negative</span> dielectrophoresis by the <span class="hlt">addition</span> of amphoteric molecules</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Flores-Rodriguez, Neftali; Markx, Gerard H.</p> <p>2004-02-01</p> <p><span class="hlt">Addition</span> of amphoteres could be used to improve the levitation and trapping of particles by <span class="hlt">negative</span> dielectrophoresis. <span class="hlt">Addition</span> of amphoteric molecules to electromanipulation media increases not only the permittivity of the medium and its viscosity but also its density. To investigate the effect of <span class="hlt">addition</span> of amphoteres on levitation and trapping by <span class="hlt">negative</span> dielectrophoresis, the electrokinetic behaviour of latex beads and viable yeast cells (Saccharomyces cerevisiae) was investigated in concentrated solutions of the amphoteric molecules N-[2-hydroxyethyl] piperazine-N'-[2-ethanesulfonic acid] (HEPES) and egr -aminocaproic acid (EACA) using different frequencies and voltages of the applied electrical signal and microelectrodes of different sizes. When using interdigitated electrodes without castellations, latex beads levitated an average of 43% higher when 0.67 M EACA solutions were used and a 54% higher after adding 0.67 M HEPES compared with the levitation heights when no amphoteres were added. Under the same conditions, yeast levitated 78% and 86% higher, respectively. At low voltages and low HEPES/EACA concentrations, the latex particles accumulated in bands between or above the electrodes. However, at the highest voltages and HEPES/EACA concentrations used, the particles formed a network of pearl chains above the electrode arrays. When using electrodes of the interdigitated castellated type of characteristic size 30 µm, latex particles levitated 32% and 40% higher when 0.67 M EACA and HEPES solutions were used in comparison with when no amphoteres were added. At these concentrations, the flow rate needed to dislodge the latex particles from the traps formed by the electric field pattern between the castellations of the interdigitated castellated electrodes was increased by 46% compared with the flow rate needed to achieve this when no amphoteres were added.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003AGUFMSH42A0500K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003AGUFMSH42A0500K"><span>Assessment and Control of International Space Station Spacecraft <span class="hlt">Charging</span> Risks</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Koontz, S.; Edeen, M.; Spetch, W.; Dalton, P.; Keeping, T.; Minow, J.</p> <p>2003-12-01</p> <p>Electrical interactions between the F2 region ionospheric plasma and the 160V photovoltaic (PV) electrical power system on the International Space Station (ISS) can produce floating potentials (FP) on ISS conducting structure of greater magnitude than are usually observed on spacecraft in low-Earth orbit. Flight through the geomagnetic field also causes magnetic induction <span class="hlt">charging</span> of ISS conducting structure. <span class="hlt">Charging</span> processes resulting from interaction of ISS with auroral electrons may also contribute to <span class="hlt">charging</span>, albeit rarely. The magnitude and frequency of occurrence of possibly hazardous <span class="hlt">charging</span> events depends on the ISS assembly stage (six more 160V PV arrays will be added to ISS), ISS flight configuration, ISS position (latitude and longitude), and the natural variability in the ionospheric flight environment. At present, ISS is equipped with two plasma contactors designed to control ISS FP to within 40 volts of the ambient F2 plasma. The <span class="hlt">negative</span>-polarity grounding scheme utilized in the ISS 160V power system leads, naturally, to <span class="hlt">negative</span> values of ISS FP. A <span class="hlt">negative</span> ISS structural FP leads to application of electrostatic fields across the dielectrics that separate conducting structure from the ambient F2 plasma, thereby enabling dielectric breakdown and arcing. Degradation of some thermal control coatings and noise in electrical systems can result. Continued review and evaluation of the putative <span class="hlt">charging</span> hazards, as required by the ISS Program Office, revealed that ISS <span class="hlt">charging</span> could produce a risk of electric shock to the ISS crew during extra vehicular activity. ISS <span class="hlt">charging</span> risks are being evaluated in ongoing ISS <span class="hlt">charging</span> measurements and analysis campaigns. The results of ISS <span class="hlt">charging</span> measurements are combined with a recently developed detailed model of the ISS <span class="hlt">charging</span> process and an extensive analysis of historical ionospheric variability data, to assess ISS <span class="hlt">charging</span> risks using Probabilistic Risk Assessment (PRA) methods. The PRA analysis</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28723072','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28723072"><span>Superposition Principle in Auger Recombination of <span class="hlt">Charged</span> and Neutral Multicarrier States in Semiconductor Quantum Dots.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wu, Kaifeng; Lim, Jaehoon; Klimov, Victor I</p> <p>2017-08-22</p> <p>Application of colloidal semiconductor quantum dots (QDs) in optical and optoelectronic devices is often complicated by unintentional generation of extra <span class="hlt">charges</span>, which opens fast nonradiative Auger recombination pathways whereby the recombination energy of an exciton is quickly transferred to the extra carrier(s) and ultimately dissipated as heat. Previous studies of Auger recombination have primarily focused on neutral and, more recently, <span class="hlt">negatively</span> <span class="hlt">charged</span> multicarrier states. Auger dynamics of positively <span class="hlt">charged</span> species remains more poorly explored due to difficulties in creating, stabilizing, and detecting excess holes in the QDs. Here we apply photochemical doping to prepare both <span class="hlt">negatively</span> and positively <span class="hlt">charged</span> CdSe/CdS QDs with two distinct core/shell interfacial profiles ("sharp" versus "smooth"). Using neutral and <span class="hlt">charged</span> QD samples we evaluate Auger lifetimes of biexcitons, <span class="hlt">negative</span> and positive trions (an exciton with an extra electron or a hole, respectively), and multiply <span class="hlt">negatively</span> <span class="hlt">charged</span> excitons. Using these measurements, we demonstrate that Auger decay of both neutral and <span class="hlt">charged</span> multicarrier states can be presented as a superposition of independent elementary three-particle Auger events. As one of the manifestations of the superposition principle, we observe that the biexciton Auger decay rate can be presented as a sum of the Auger rates for independent <span class="hlt">negative</span> and positive trion pathways. By comparing the measurements on the QDs with the "sharp" versus "smooth" interfaces, we also find that while affecting the absolute values of Auger lifetimes, manipulation of the shape of the confinement potential does not lead to violation of the superposition principle, which still allows us to accurately predict the biexciton Auger lifetimes based on the measured <span class="hlt">negative</span> and positive trion dynamics. These findings indicate considerable robustness of the superposition principle as applied to Auger decay of <span class="hlt">charged</span> and neutral multicarrier states</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22597741-effects-nanoparticles-organic-additives-controlled-dispersion-dielectric-properties-polymers-charge-trapping-impact-excitation','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22597741-effects-nanoparticles-organic-additives-controlled-dispersion-dielectric-properties-polymers-charge-trapping-impact-excitation"><span>The effects of nanoparticles and organic <span class="hlt">additives</span> with controlled dispersion on dielectric properties of polymers: <span class="hlt">Charge</span> trapping and impact excitation</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Huang, Yanhui, E-mail: huangy12@rpi.edu; Schadler, Linda S.; Wu, Ke</p> <p></p> <p>This work presents a comprehensive investigation into the effects of nanoparticles and organic <span class="hlt">additives</span> on the dielectric properties of insulating polymers using reinforced silicone rubber as a model system. TiO{sub 2} and ZrO{sub 2} nanoparticles (d = 5 nm) were well dispersed into the polymer via a bimodal surface modification approach. Organic molecules with the potential of voltage stabilization were further grafted to the nanoparticle to ensure their dispersion. These extrinsic species were found to provide deep traps for <span class="hlt">charge</span> carriers and exhibited effective <span class="hlt">charge</span> trapping properties at a rather small concentration (∼10{sup 17} cm{sup −3}). The <span class="hlt">charge</span> trapping is found to havemore » the most significant effect on breakdown strength when the electrical stressing time is long enough that most <span class="hlt">charges</span> are trapped in the deep states. To establish a quantitative correlation between the trap depth and the molecular properties, the electron affinity and ionization energy of each species were calculated by an ab initio method and were compared with the experimentally measured values. The correlation however remains elusive and is possibly complicated by the field effect and the electronic interactions between different species that are not considered in this computation. At high field, a super-linear increase of current density was observed for TiO{sub 2} filled composites and is likely caused by impact excitation due to the low excitation energy of TiO{sub 2} compared to ZrO{sub 2}. It is reasoned that the hot <span class="hlt">charge</span> carriers with energies greater than the excitation energy of TiO{sub 2} may excite an electron-hole pair upon collision with the NP, which later will be dissociated and contribute to free <span class="hlt">charge</span> carriers. This mechanism can enhance the energy dissipation and may account for the retarded electrical degradation and breakdown of TiO{sub 2} composites.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23674178','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23674178"><span>Organic n-type materials for <span class="hlt">charge</span> transport and <span class="hlt">charge</span> storage applications.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Stolar, Monika; Baumgartner, Thomas</p> <p>2013-06-21</p> <p>Conjugated materials have attracted much attention toward applications in organic electronics in recent years. These organic species offer many advantages as potential replacement for conventional materials (i.e., silicon and metals) in terms of cheap fabrication and environmentally benign devices. While p-type (electron-donating or hole-conducting) materials have been extensively reviewed and researched, their counterpart n-type (electron-accepting or electron-conducting) materials have seen much less popularity despite the greater need for improvement. In <span class="hlt">addition</span> to developing efficient <span class="hlt">charge</span> transport materials, it is equally important to provide a means of <span class="hlt">charge</span> storage, where energy can be used on an on-demand basis. This perspective is focused on discussing a selection of representative n-type materials and the efforts toward improving their <span class="hlt">charge</span>-transport efficiencies. <span class="hlt">Additionally</span>, this perspective will also highlight recent organic materials for battery components and the efforts that have been made to improve their environmental appeal.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25470772','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25470772"><span>Gating capacitive field-effect sensors by the <span class="hlt">charge</span> of nanoparticle/molecule hybrids.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Poghossian, Arshak; Bäcker, Matthias; Mayer, Dirk; Schöning, Michael J</p> <p>2015-01-21</p> <p>The semiconductor field-effect platform is a powerful tool for chemical and biological sensing with direct electrical readout. In this work, the field-effect capacitive electrolyte-insulator-semiconductor (EIS) structure - the simplest field-effect (bio-)chemical sensor - modified with citrate-capped gold nanoparticles (AuNPs) has been applied for a label-free electrostatic detection of <span class="hlt">charged</span> molecules by their intrinsic molecular <span class="hlt">charge</span>. The EIS sensor detects the <span class="hlt">charge</span> changes in AuNP/molecule inorganic/organic hybrids induced by the molecular adsorption or binding events. The feasibility of the proposed detection scheme has been exemplarily demonstrated by realizing capacitive EIS sensors consisting of an Al-p-Si-SiO2-silane-AuNP structure for the label-free detection of positively <span class="hlt">charged</span> cytochrome c and poly-d-lysine molecules as well as for monitoring the layer-by-layer formation of polyelectrolyte multilayers of poly(allylamine hydrochloride)/poly(sodium 4-styrene sulfonate), representing typical model examples of detecting small proteins and macromolecules and the consecutive adsorption of positively/<span class="hlt">negatively</span> <span class="hlt">charged</span> polyelectrolytes, respectively. For comparison, EIS sensors without AuNPs have been investigated, too. The adsorption of molecules on the surface of AuNPs has been verified via the X-ray photoelectron spectroscopy method. In <span class="hlt">addition</span>, a theoretical model of the functioning of the capacitive field-effect EIS sensor functionalized with AuNP/<span class="hlt">charged</span>-molecule hybrids has been discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GeoRL..44.8027B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GeoRL..44.8027B"><span>Flash propagation and inferred <span class="hlt">charge</span> structure relative to radar-observed ice alignment signatures in a small Florida mesoscale convective system</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Biggerstaff, Michael I.; Zounes, Zackery; Addison Alford, A.; Carrie, Gordon D.; Pilkey, John T.; Uman, Martin A.; Jordan, Douglas M.</p> <p>2017-08-01</p> <p>A series of vertical cross sections taken through a small mesoscale convective system observed over Florida by the dual-polarimetric SMART radar were combined with VHF radiation source locations from a lightning mapping array (LMA) to examine the lightning channel propagation paths relative to the radar-observed ice alignment signatures associated with regions of <span class="hlt">negative</span> specific differential phase (<fi>K</fi>DP). <span class="hlt">Additionally</span>, <span class="hlt">charge</span> layers inferred from analysis of LMA sources were related to the ice alignment signature. It was found that intracloud flashes initiated near the upper zero-<fi>K</fi>DP boundary surrounding the <span class="hlt">negative</span> <fi>K</fi>DP region. The zero-<fi>K</fi>DP boundary also delineated the propagation path of the lightning channel with the <span class="hlt">negative</span> leaders following the upper boundary and positive leaders following the lower boundary. Very few LMA sources were found in the <span class="hlt">negative</span> <fi>K</fi>DP region. We conclude that rapid dual-polarimetric radar observations can diagnose strong electric fields and may help identify surrounding regions of <span class="hlt">charge</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/9685903','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/9685903"><span>Iontophoresis of monomeric insulin analogues in vitro: effects of insulin <span class="hlt">charge</span> and skin pretreatment.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Langkjaer, L; Brange, J; Grodsky, G M; Guy, R H</p> <p>1998-01-23</p> <p>The aim of this study was to investigate the influence of association state and net <span class="hlt">charge</span> of human insulin analogues on the rate of iontophoretic transport across hairless mouse skin, and the effect of different skin pretreatments on said transport. No insulin flux was observed with anodal delivery probably because of degradation at the Ag/AgCl anode. The flux during cathodal iontophoresis through intact skin was insignificant for human hexameric insulin, and only low and variable fluxes were observed for monomeric insulins. Using stripped skin on the other hand, the fluxes of monomeric insulins with two extra <span class="hlt">negative</span> <span class="hlt">charges</span> were 50-100 times higher than that of hexameric human insulin. Introducing three <span class="hlt">additional</span> <span class="hlt">charges</span> led to a further 2-3-fold increase in flux. Wiping the skin gently with absolute alcohol prior to iontophoresis resulted in a 1000-fold increase in transdermal transport of insulin relative to that across untreated skin, i.e. to almost the same level as stripping the skin. The alcohol pretreatment reduced the electrical resistance of the skin, presumably by lipid extraction. In conclusion, monomeric insulin analogues with at least two extra <span class="hlt">negative</span> <span class="hlt">charges</span> can be iontophoretically delivered across hairless mouse skin, whereas insignificant flux is observed with human, hexameric insulin. Wiping the skin with absolute alcohol prior to iontophoresis gave substantially improved transdermal transport of monomeric insulins resulting in clinically relevant delivery rates for basal treatment.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.afdc.energy.gov/fuels/electricity_charging_home.html','SCIGOVWS'); return false;" href="https://www.afdc.energy.gov/fuels/electricity_charging_home.html"><span>Alternative Fuels Data Center: <span class="hlt">Charging</span> Plug-In Electric Vehicles at Home</span></a></p> <p><a target="_blank" href="http://www.science.gov/aboutsearch.html">Science.gov Websites</a></p> <p></p> <p></p> <p>Infrastructure Development <span class="hlt">Charging</span> at Home Multi-Unit Dwelling <span class="hlt">Charging</span> <span class="hlt">Charging</span> in <em>Public</em> Workplace <span class="hlt">Charging</span> complex requires <span class="hlt">additional</span> considerations and may be more similar to <em>public</em> <span class="hlt">charging</span> than to <span class="hlt">charging</span> at , requiring no <span class="hlt">additional</span> <em>cost</em> or installation, provided that a power outlet on a dedicated branch circuit is</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20050201639','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20050201639"><span>Flywheel <span class="hlt">Charge</span>/Discharge Control Developed</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Beach, Raymond.F.; Kenny, Barbara H.</p> <p>2001-01-01</p> <p>A control algorithm developed at the NASA Glenn Research Center will allow a flywheel energy storage system to interface with the electrical bus of a space power system. The controller allows the flywheel to operate in both <span class="hlt">charge</span> and discharge modes. <span class="hlt">Charge</span> mode is used to store <span class="hlt">additional</span> energy generated by the solar arrays on the spacecraft during insolation. During <span class="hlt">charge</span> mode, the flywheel spins up to store the <span class="hlt">additional</span> electrical energy as rotational mechanical energy. Discharge mode is used during eclipse when the flywheel provides the power to the spacecraft. During discharge mode, the flywheel spins down to release the stored rotational energy.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5677248','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5677248"><span><span class="hlt">Charge</span> Induced Dynamics of Water in a Graphene–Mica Slit Pore</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p></p> <p>2017-01-01</p> <p>We use atomic force microscopy to in situ investigate the dynamic behavior of confined water at the interface between graphene and mica. The graphene is either uncharged, <span class="hlt">negatively</span> <span class="hlt">charged</span>, or positively <span class="hlt">charged</span>. At high humidity, a third water layer will intercalate between graphene and mica. When graphene is <span class="hlt">negatively</span> <span class="hlt">charged</span>, the interface fills faster with a complete three layer water film, compared to uncharged graphene. As <span class="hlt">charged</span> positively, the third water layer dewets the interface, either by evaporation into the ambient or by the formation of three-dimensional droplets under the graphene, on top of the bilayer. Our experimental findings reveal novel phenomena of water at the nanoscale, which are interesting from a fundamental point of view and demonstrate the direct control over the wetting properties of the graphene/water interface. PMID:28985466</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002ssi..conf...73L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002ssi..conf...73L"><span>Study of the <span class="hlt">Charge</span> Transfer Process of LaNi5 Type Electrodes in Ni-MH Batteries</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Le, Xuan Que; Nguyen, Phu Thuy</p> <p>2002-12-01</p> <p>As a result of the <span class="hlt">charge</span> process of LaNi5 type electrode, hydrogen is reversibly absorbed on the electrode surface. The process consists two principal steps. During the both processes, the first reaction step occurs in the interface solid/liquid, <span class="hlt">negatively</span> <span class="hlt">charged</span>, with high static electric field, where the double layer structure became more compact. The transfer of <span class="hlt">charge</span> under high electric field depends on many factors, principally on compositions of the electrode materials. Effects on that of Co, Fe, Mn substitutes, with different concentrations, have been comparatively studied using electrochemical technique. The analyse of interface C -.V study results has been realised, respecting Mott-Schottky relation. Optimal contents of some <span class="hlt">additives</span> have been discussed. Some advantages of the applied electrochemical methods have been confirmed. The mechanism of the <span class="hlt">charges</span> transfer and of the hydrogen reversible storage in the crystal structure in the batteries has been discussed. With the proposed mechanism, one can more explicitly understand the difference of the magnetic effect of the electrode materials before and after <span class="hlt">charge</span>-discharge process can be explained.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015SurSc.631...35W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015SurSc.631...35W"><span>Electrolyte effects in a model of proton discharge on <span class="hlt">charged</span> electrodes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wiebe, Johannes; Kravchenko, Kateryna; Spohr, Eckhard</p> <p>2015-01-01</p> <p>We report results on the influence of NaCl electrolyte dissolved in water on proton discharge reactions from aqueous solution to <span class="hlt">charged</span> platinum electrodes. We have extended a recently developed combined proton transfer/proton discharge model on the basis of empirical valence bond theory to include NaCl solutions with several different concentrations of cations and anions, both stoichiometric (1:1) compositions and non-stoichiometric ones with an excess of cations. The latter solutions partially screen the electrostatic potential from the surface <span class="hlt">charge</span> of the <span class="hlt">negatively</span> <span class="hlt">charged</span> electrode. 500-1000 trajectories of a discharging proton were integrated by molecular dynamics simulations until discharge occurred, or for at most 1.5 ns. The results show a strong dependence on ionic strength, but only a weak dependence on the screening behavior, when comparing stoichiometric and non-stoichiometric solutions. Overall, the Na+ cations exert a more dominant effect on the discharge reaction, which we argue is likely due to the very rigid arrangements of the cations on the <span class="hlt">negatively</span> polarized electrode surface. Thus, our model predicts, for the given and very high <span class="hlt">negative</span> surface <span class="hlt">charge</span> densities, the fastest discharge reaction for pure water, but obviously cannot take into account the fact that such high <span class="hlt">charge</span> densities are even more out of reach experimentally than for higher electrolyte concentrations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4366815','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4366815"><span>Upregulation of BMSCs Osteogenesis by Positively-<span class="hlt">Charged</span> Tertiary Amines on Polymeric Implants via <span class="hlt">Charge</span>/iNOS Signaling Pathway</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Zhang, Wei; Liu, Na; Shi, Haigang; Liu, Jun; Shi, Lianxin; Zhang, Bo; Wang, Huaiyu; Ji, Junhui; Chu, Paul K.</p> <p>2015-01-01</p> <p>Positively-<span class="hlt">charged</span> surfaces on implants have a similar potential to upregulate osteogenesis of bone marrow-derived mesenchymal stem cells (BMSCs) as electromagnetic therapy approved for bone regeneration. Generally, their osteogenesis functions are generally considered to stem from the <span class="hlt">charge</span>-induced adhesion of extracellular matrix (ECM) proteins without exploring the underlying surface <span class="hlt">charge</span>/cell signaling molecule pathways. Herein, a positively-<span class="hlt">charged</span> surface with controllable tertiary amines is produced on a polymer implant by plasma surface modification. In <span class="hlt">addition</span> to inhibiting the TNF-α expression, the positively-<span class="hlt">charged</span> surface with tertiary amines exhibits excellent cytocompatibility as well as remarkably upregulated osteogenesis-related gene/protein expressions and calcification of the contacted BMSCs. Stimulated by the <span class="hlt">charged</span> surface, these BMSCs display high iNOS expressions among the three NOS isoforms. Meanwhile, downregulation of the iNOS by L-Can or siRNA inhibit osteogenic differentiation in the BMSCs. These findings suggest that a positively-<span class="hlt">charged</span> surface with tertiary amines induces osteogenesis of BMSCs via the surface <span class="hlt">charge</span>/iNOS signaling pathway in <span class="hlt">addition</span> to elevated ECM protein adhesion. Therefore, creating a positively-<span class="hlt">charged</span> surface with tertiary amines is a promising approach to promote osseointegration with bone tissues. PMID:25791957</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012JGRA..117.7308A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012JGRA..117.7308A"><span>Characteristics of spacecraft <span class="hlt">charging</span> in low Earth orbit</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Anderson, Phillip C.</p> <p>2012-07-01</p> <p>It has been found that the DMSP spacecraft at 840 km can <span class="hlt">charge</span> to very large <span class="hlt">negative</span> voltages (up to -2000 V) when encountering intense precipitating electron events (auroral arcs). We present an 11-year study of over 1600 <span class="hlt">charging</span> events, defined as when the spacecraft <span class="hlt">charged</span> to levels exceeding 100 V <span class="hlt">negative</span> during an auroral crossing. The occurrence frequency of events was highly correlated with the 11-year solar cycle with the largest number of events occurring during solar minimum. This was due to the requirement that the background thermal plasma density be low, at most 104 cm-3. During solar maximum, the plasma density is typically well above that level due to the solar EUV ionizing radiation, and although the occurrence frequency of auroral arcs is considerably greater than at solar minimum, the occurrence of high-level <span class="hlt">charging</span> is minimal. As a result of this study, we produced a model spectrum for precipitating electrons that can be used as a specification for the low-altitude auroral <span class="hlt">charging</span> environment. There are implications from this study on a number of LEO satellite programs, including the International Space Station, which does enter the auroral zone, particularly during geomagnetic activity when the auroral boundary can penetrate to very low latitudes. The plasma density in the ISS orbit is usually well above the minimum required density for <span class="hlt">charging</span>. However, in the wake of the ISS, the plasma density can be 2 orders of magnitude or more lower than the background density and thus conditions are ripe for <span class="hlt">charging</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title46-vol8/pdf/CFR-2010-title46-vol8-secSec-5-id759.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title46-vol8/pdf/CFR-2010-title46-vol8-secSec-5-id759.pdf"><span>46 CFR Sec. 5 - Repatriation <span class="hlt">charges</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-10-01</p> <p>... flat transportation <span class="hlt">charge</span> of $5.00 per day shall be made for every day spent aboard the repatriating vessel, including day of embarkation and day of debarkation, which <span class="hlt">charge</span> shall be in <span class="hlt">addition</span> to... fees or other <span class="hlt">charges</span> of every nature levied in connection with such repatriation. In such a case, the...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JChPh.148k4904W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JChPh.148k4904W"><span>Structure and stability of <span class="hlt">charged</span> colloid-nanoparticle mixtures</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Weight, Braden M.; Denton, Alan R.</p> <p>2018-03-01</p> <p>Physical properties of colloidal materials can be modified by <span class="hlt">addition</span> of nanoparticles. Within a model of like-<span class="hlt">charged</span> mixtures of particles governed by effective electrostatic interactions, we explore the influence of <span class="hlt">charged</span> nanoparticles on the structure and thermodynamic phase stability of <span class="hlt">charge</span>-stabilized colloidal suspensions. Focusing on salt-free mixtures of particles of high size and <span class="hlt">charge</span> asymmetry, interacting via repulsive Yukawa effective pair potentials, we perform molecular dynamics simulations and compute radial distribution functions and static structure factors. Analysis of these structural properties indicates that increasing the <span class="hlt">charge</span> and concentration of nanoparticles progressively weakens correlations between <span class="hlt">charged</span> colloids. We show that <span class="hlt">addition</span> of <span class="hlt">charged</span> nanoparticles to a suspension of like-<span class="hlt">charged</span> colloids can induce a colloidal crystal to melt and can facilitate aggregation of a fluid suspension due to attractive van der Waals interactions. We attribute the destabilizing influence of <span class="hlt">charged</span> nanoparticles to enhanced screening of electrostatic interactions, which weakens repulsion between <span class="hlt">charged</span> colloids. This interpretation is consistent with recent predictions of an effective interaction theory of <span class="hlt">charged</span> colloid-nanoparticle mixtures.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21807216','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21807216"><span>Sulfadiazine-selective determination in aquaculture environment: selective potentiometric transduction by neutral or <span class="hlt">charged</span> ionophores.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Almeida, S A A; Heitor, A M; Montenegro, M C B S M; Sales, M G F</p> <p>2011-09-15</p> <p>Solid-contact sensors for the selective screening of sulfadiazine (SDZ) in aquaculture waters are reported. Sensor surfaces were made from PVC membranes doped with tetraphenylporphyrin-manganese(III) chloride, α-cyclodextrin, β-cyclodextrin, or γ-cyclodextrin ionophores that were dispersed in plasticizer. Some membranes also presented a positive or a <span class="hlt">negatively</span> <span class="hlt">charged</span> <span class="hlt">additive</span>. Phorphyrin-based sensors relied on a <span class="hlt">charged</span> carrier mechanism. They exhibited a near-Nernstian response with slopes of 52 mV decade(-1) and detection limits of 3.91×10(-5) mol L(-1). The <span class="hlt">addition</span> of cationic lipophilic compounds to the membrane originated Nernstian behaviours, with slopes ranging 59.7-62.0 mV decade(-1) and wider linear ranges. Cyclodextrin-based sensors acted as neutral carriers. In general, sensors with positively <span class="hlt">charged</span> <span class="hlt">additives</span> showed an improved potentiometric performance when compared to those without <span class="hlt">additive</span>. Some SDZ selective membranes displayed higher slopes and extended linear concentration ranges with an increasing amount of <span class="hlt">additive</span> (always <100% ionophore). The sensors were independent from the pH of test solutions within 2-7. The sensors displayed fast response, always <15s. In general, a good discriminating ability was found in real sample environment. The sensors were successfully applied to the fast screening of SDZ in real waters samples from aquaculture fish farms. The method offered the advantages of simplicity, accuracy, and automation feasibility. The sensing membrane may contribute to the development of small devices allowing in locus measurements of sulfadiazine or parent-drugs. Copyright © 2011 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..DPPN11134O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..DPPN11134O"><span>Investigation of Dusts Effect and <span class="hlt">Negative</span> Ion in DC Plasmas by Electric Probes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Oh, Hye Taek; Kang, Inje; Bae, Min-Keun; Park, Insun; Lee, Seunghwa; Jeong, Seojin; Chung, Kyu-Sun</p> <p>2017-10-01</p> <p>Dust is typically <span class="hlt">negatively</span> <span class="hlt">charged</span> by electron attachment whose thermal velocities are fast compared to that of the heavier ions. The <span class="hlt">negatively</span> <span class="hlt">charged</span> particles can play a role of <span class="hlt">negative</span> ions which affect the quasi-neutrality of background plasma. To investigate effect of metal dusts and <span class="hlt">negative</span> ion on plasma and materials, metal dusts are injected into background Ar plasma which is generated by tungsten filament using dust dispenser on Cubical Plasma Device (CPD). The CPD has following conditions: size =24x24x24cm3, plasma source =DC filament plasma (ne 1x10x1010, Te 2eV), background gas =Ar, dusts =tungsten powder (diameter 1.89micron). The dust dispenser is developed to quantitate of metal dust by ultrasonic transducer. Electronegative plasmas are generated by adding O2 + Ar plasma to compare <span class="hlt">negative</span> ion and dust effect. A few grams of micron-sized dusts are placed in the dust dispenser which is located at the upper side of the Cubical Plasma Device. The falling particles by dust dispenser are mainly <span class="hlt">charged</span> up by the collection of the background plasma. The change in parameters due to <span class="hlt">negative</span> ion production are characterized by measuring the floating and plasma potential, electron temperature and <span class="hlt">negative</span> ion density using electric probes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/11975185','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/11975185"><span>Effect of surface material on electrostatic <span class="hlt">charging</span> of houseflies (Musca domestica L).</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>McGonigle, Daniel F; Jackson, Chris W</p> <p>2002-04-01</p> <p>Houseflies (Musca domestica L) accumulated electrostatic <span class="hlt">charges</span> when walking over clean, uncharged dielectric surfaces. The <span class="hlt">charges</span> elicited on a walking housefly by a range of materials were quantified, allowing a triboelectric series to be determined relative to M domestica. This ranged from surfaces that <span class="hlt">charged</span> individuals positively, e.g. Correx (corrugated polypropylene) [.1 (+/- 4.2)pC], to those that applied a <span class="hlt">negative</span> <span class="hlt">charge</span>, e.g. clear cast acrylic [-14.9 (+/- 2.9)pC]. Maximum positive and <span class="hlt">negative</span> <span class="hlt">charges</span> accumulated by individual M domestica were +73 and -27 pC. Replicate measurements on the same fly and surface showed little variation. Variation between individuals was not related to sex and was not consistent between surfaces. Different materials <span class="hlt">charged</span> M domestica significantly differently and individual flies had significantly different <span class="hlt">charging</span> properties. Variation in temperature between 21.3 degrees C and 24.7 degrees C and humidity between 24% and 41% RH significantly affected <span class="hlt">charge</span> accumulated by M domestica on some surfaces, although further experimentation is needed to confirm this. The implications of this work are discussed in relation to insect trap design and pollination biology.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li class="active"><span>13</span></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_13 --> <div id="page_14" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li class="active"><span>14</span></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="261"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/865058','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/865058"><span>Electrically <span class="hlt">charged</span> targets</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Goodman, Ronald K.; Hunt, Angus L.</p> <p>1984-01-01</p> <p>Electrically chargeable laser targets and method for forming such <span class="hlt">charged</span> targets in order to improve their guidance along a predetermined desired trajectory. This is accomplished by the incorporation of a small amount of an <span class="hlt">additive</span> to the target material which will increase the electrical conductivity thereof, and thereby enhance the <span class="hlt">charge</span> placed upon the target material for guidance thereof by electrostatic or magnetic steering mechanisms, without adversely affecting the target when illuminated by laser energy.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22607630','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22607630"><span>Theoretical study of <span class="hlt">negatively</span> <span class="hlt">charged</span> Fe(-)-(H2O)(n ≤ 6) clusters.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Castro, Miguel</p> <p>2012-06-14</p> <p>Interactions of a singly <span class="hlt">negatively</span> <span class="hlt">charged</span> iron atom with water molecules, Fe(-)-(H(2)O)(n≤6), in the gas phase were studied by means of density functional theory. All-electron calculations were performed using the B3LYP functional and the 6-311++G(2d,2p) basis set for the Fe, O, and H atoms. In the lowest total energy states of Fe(-)-(H(2)O)(n), the metal-hydrogen bonding is stronger than the metal-oxygen one, producing low-symmetry structures because the water molecules are directly attached to the metal by basically one of their hydrogen atoms, whereas the other ones are involved in a network of hydrogen bonds, which together with the Fe(δ-)-H(δ+) bonding accounts for the nascent hydration of the Fe(-) anion. For Fe(-)-(H(2)O)(3≤n), three-, four-, five-, and six-membered rings of water molecules are bonded to the metal, which is located at the surface of the cluster in such a way as to reduce the repulsion with the oxygen atoms. Nevertheless, internal isomers appear also, lying less than 3 or 5 kcal/mol for n = 2-3 or n = 4-6. These results are in contrast with those of classical TM(+)-(H(2)O)(n) complexes, where the direct TM(+)-O bonding usually produces high symmetry structures with the metal defining the center of the complex. They show also that the Fe(-) anions, as the TM(+) ions, have great capability for the adsorption of water molecules, forming Fe(-)-(H(2)O)(n) structures stabilized by Fe(δ-)-H(δ+) and H-bond interactions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1417812-superposition-principle-auger-recombination-charged-neutral-multicarrier-states-semiconductor-quantum-dots','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1417812-superposition-principle-auger-recombination-charged-neutral-multicarrier-states-semiconductor-quantum-dots"><span>Superposition Principle in Auger Recombination of <span class="hlt">Charged</span> and Neutral Multicarrier States in Semiconductor Quantum Dots</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Wu, Kaifeng; Lim, Jaehoon; Klimov, Victor I.</p> <p>2017-07-19</p> <p>Application of colloidal semiconductor quantum dots (QDs) in optical and optoelectronic devices is often complicated by unintentional generation of extra <span class="hlt">charges</span>, which opens fast nonradiative Auger recombination pathways whereby the recombination energy of an exciton is quickly transferred to the extra carrier(s) and ultimately dissipated as heat. Previous studies of Auger recombination have primarily focused on neutral and, more recently, <span class="hlt">negatively</span> <span class="hlt">charged</span> multicarrier states. Auger dynamics of positively <span class="hlt">charged</span> species remains more poorly explored due to difficulties in creating, stabilizing, and detecting excess holes in the QDs. Here we apply photochemical doping to prepare both <span class="hlt">negatively</span> and positively <span class="hlt">charged</span> CdSe/CdSmore » QDs with two distinct core/shell interfacial profiles (“sharp” versus “smooth”). Using neutral and <span class="hlt">charged</span> QD samples we evaluate Auger lifetimes of biexcitons, <span class="hlt">negative</span> and positive trions (an exciton with an extra electron or a hole, respectively), and multiply <span class="hlt">negatively</span> <span class="hlt">charged</span> excitons. Using these measurements, we demonstrate that Auger decay of both neutral and <span class="hlt">charged</span> multicarrier states can be presented as a superposition of independent elementary three-particle Auger events. As one of the manifestations of the superposition principle, we observe that the biexciton Auger decay rate can be presented as a sum of the Auger rates for independent <span class="hlt">negative</span> and positive trion pathways. Furthermore, by comparing the measurements on the QDs with the “sharp” versus “smooth” interfaces, we also find that while affecting the absolute values of Auger lifetimes, manipulation of the shape of the confinement potential does not lead to violation of the superposition principle, which still allows us to accurately predict the biexciton Auger lifetimes based on the measured <span class="hlt">negative</span> and positive trion dynamics. Our findings indicate considerable robustness of the superposition principle as applied to Auger decay of <span class="hlt">charged</span> and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1233556-differential-algebra-based-multiple-level-fast-multipole-algorithm-space-charge-field-calculation-photoemission-simulation','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1233556-differential-algebra-based-multiple-level-fast-multipole-algorithm-space-charge-field-calculation-photoemission-simulation"><span>The differential algebra based multiple level fast multipole algorithm for 3D space <span class="hlt">charge</span> field calculation and photoemission simulation</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>None, None</p> <p>2015-09-28</p> <p>Coulomb interaction between <span class="hlt">charged</span> particles inside a bunch is one of the most importance collective effects in beam dynamics, becoming even more significant as the energy of the particle beam is lowered to accommodate analytical and low-Z material imaging purposes such as in the time resolved Ultrafast Electron Microscope (UEM) development currently underway at Michigan State University. In <span class="hlt">addition</span>, space <span class="hlt">charge</span> effects are the key limiting factor in the development of ultrafast atomic resolution electron imaging and diffraction technologies and are also correlated with an irreversible growth in rms beam emittance due to fluctuating components of the nonlinear electron dynamics.more » In the short pulse regime used in the UEM, space <span class="hlt">charge</span> effects also lead to virtual cathode formation in which the <span class="hlt">negative</span> <span class="hlt">charge</span> of the electrons emitted at earlier times, combined with the attractive surface field, hinders further emission of particles and causes a degradation of the pulse properties. Space <span class="hlt">charge</span> and virtual cathode effects and their remediation are core issues for the development of the next generation of high-brightness UEMs. Since the analytical models are only applicable for special cases, numerical simulations, in <span class="hlt">addition</span> to experiments, are usually necessary to accurately understand the space <span class="hlt">charge</span> effect. In this paper we will introduce a grid-free differential algebra based multiple level fast multipole algorithm, which calculates the 3D space <span class="hlt">charge</span> field for n <span class="hlt">charged</span> particles in arbitrary distribution with an efficiency of O(n), and the implementation of the algorithm to a simulation code for space <span class="hlt">charge</span> dominated photoemission processes.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28035963','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28035963"><span>Threshold-Based Random <span class="hlt">Charging</span> Scheme for Decentralized PEV <span class="hlt">Charging</span> Operation in a Smart Grid.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kwon, Ojin; Kim, Pilkee; Yoon, Yong-Jin</p> <p>2016-12-26</p> <p>Smart grids have been introduced to replace conventional power distribution systems without real time monitoring for accommodating the future market penetration of plug-in electric vehicles (PEVs). When a large number of PEVs require simultaneous battery <span class="hlt">charging</span>, <span class="hlt">charging</span> coordination techniques have become one of the most critical factors to optimize the PEV <span class="hlt">charging</span> performance and the conventional distribution system. In this case, considerable computational complexity of a central controller and exchange of real time information among PEVs may occur. To alleviate these problems, a novel threshold-based random <span class="hlt">charging</span> (TBRC) operation for a decentralized <span class="hlt">charging</span> system is proposed. Using PEV <span class="hlt">charging</span> thresholds and random access rates, the PEVs themselves can participate in the <span class="hlt">charging</span> requests. As PEVs with a high battery state do not transmit the <span class="hlt">charging</span> requests to the central controller, the complexity of the central controller decreases due to the reduction of the <span class="hlt">charging</span> requests. In <span class="hlt">addition</span>, both the <span class="hlt">charging</span> threshold and the random access rate are statistically calculated based on the average of supply power of the PEV <span class="hlt">charging</span> system that do not require a real time update. By using the proposed TBRC with a tolerable PEV <span class="hlt">charging</span> degradation, a 51% reduction of the PEV <span class="hlt">charging</span> requests is achieved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5298612','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5298612"><span>Threshold-Based Random <span class="hlt">Charging</span> Scheme for Decentralized PEV <span class="hlt">Charging</span> Operation in a Smart Grid</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Kwon, Ojin; Kim, Pilkee; Yoon, Yong-Jin</p> <p>2016-01-01</p> <p>Smart grids have been introduced to replace conventional power distribution systems without real time monitoring for accommodating the future market penetration of plug-in electric vehicles (PEVs). When a large number of PEVs require simultaneous battery <span class="hlt">charging</span>, <span class="hlt">charging</span> coordination techniques have become one of the most critical factors to optimize the PEV <span class="hlt">charging</span> performance and the conventional distribution system. In this case, considerable computational complexity of a central controller and exchange of real time information among PEVs may occur. To alleviate these problems, a novel threshold-based random <span class="hlt">charging</span> (TBRC) operation for a decentralized <span class="hlt">charging</span> system is proposed. Using PEV <span class="hlt">charging</span> thresholds and random access rates, the PEVs themselves can participate in the <span class="hlt">charging</span> requests. As PEVs with a high battery state do not transmit the <span class="hlt">charging</span> requests to the central controller, the complexity of the central controller decreases due to the reduction of the <span class="hlt">charging</span> requests. In <span class="hlt">addition</span>, both the <span class="hlt">charging</span> threshold and the random access rate are statistically calculated based on the average of supply power of the PEV <span class="hlt">charging</span> system that do not require a real time update. By using the proposed TBRC with a tolerable PEV <span class="hlt">charging</span> degradation, a 51% reduction of the PEV <span class="hlt">charging</span> requests is achieved. PMID:28035963</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3144725','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3144725"><span>The role of surface <span class="hlt">charge</span> on the uptake and biocompatibility of hydroxyapatite nanoparticles with osteoblast cells</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Chen, Liang; Mccrate, Joseph M.; Lee, James C-M.; Li, Hao</p> <p>2011-01-01</p> <p>The objective of this study is to evaluate the effect of hydroxyapatite (HAP) nanoparticles with different surface <span class="hlt">charges</span> on the cellular uptake behavior and in vitro cell viability and proliferation of MC3T3-E1 cell lines (osteoblast). The nanoparticles surface <span class="hlt">charge</span> was varied by the surface modification with two carboxylic acids: 12-aminododecanoic acid (positive) and dodecanedioic acid (<span class="hlt">negative</span>). The untreated HAP nanoparticles and dodecanoic acid modified HAP nanoparticles (neutral) were used as the control. X-ray diffraction (XRD) revealed that surface modifications by the three carboxylic acids did not change the crystal structure of HAP nanoparticles; Fourier transform infrared spectroscopy (FTIR) confirmed the adsorption and binding of the carboxylic acids on HAP nanoparticle surface; and zeta potential measurement confirmed that the chemicals successfully modified the surface <span class="hlt">charge</span> of HAP nanoparticles in water based solution. Transmission electron microscopy (TEM) images showed that positively <span class="hlt">charged</span>, <span class="hlt">negatively</span> <span class="hlt">charged</span> and untreated HAP nanoparticles, with similar size and shape, all penetrated into the cells and cells had more uptake of HAP nanoparticles with positive <span class="hlt">charge</span> compared to those with <span class="hlt">negative</span> <span class="hlt">charge</span>, which might be attributed to the attractive or repulsive interaction between the <span class="hlt">negatively</span> <span class="hlt">charged</span> cell membrane and positively/<span class="hlt">negatively</span> <span class="hlt">charged</span> HAP nanoparticles. The neutral HAP nanoparticles could not penetrate cell membrane due to the larger size. MTT assay and LDH assay results indicated that as compared with the polystyrene control, greater cell viability and cell proliferation were measured on MC3T3-E1 cells treated with the three kinds of the HAP nanoparticles (neutral, positive, and untreated), among which positively <span class="hlt">charged</span> HAP nanoparticles shows strongest improvement for cell viability and cell proliferation. In summary, the surface <span class="hlt">charge</span> of HAP nanoparticles can be modified to influence the cellular uptake of HAP</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26379082','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26379082"><span>Molecular simulation study of feruloyl esterase adsorption on <span class="hlt">charged</span> surfaces: effects of surface <span class="hlt">charge</span> density and ionic strength.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Liu, Jie; Peng, Chunwang; Yu, Gaobo; Zhou, Jian</p> <p>2015-10-06</p> <p>The surrounding conditions, such as surface <span class="hlt">charge</span> density and ionic strength, play an important role in enzyme adsorption. The adsorption of a nonmodular type-A feruloyl esterase from Aspergillus niger (AnFaeA) on <span class="hlt">charged</span> surfaces was investigated by parallel tempering Monte Carlo (PTMC) and all-atom molecular dynamics (AAMD) simulations at different surface <span class="hlt">charge</span> densities (±0.05 and ±0.16 C·m(-2)) and ionic strengths (0.007 and 0.154 M). The adsorption energy, orientation, and conformational changes were analyzed. Simulation results show that whether AnFaeA can adsorb onto a <span class="hlt">charged</span> surface is mainly controlled by electrostatic interactions between AnFaeA and the <span class="hlt">charged</span> surface. The electrostatic interactions between AnFaeA and <span class="hlt">charged</span> surfaces are weakened when the ionic strength increases. The positively <span class="hlt">charged</span> surface at low surface <span class="hlt">charge</span> density and high ionic strength conditions can maximize the utilization of the immobilized AnFaeA. The counterion layer plays a key role in the adsorption of AnFaeA on the <span class="hlt">negatively</span> <span class="hlt">charged</span> COOH-SAM. The native conformation of AnFaeA is well preserved under all of these conditions. The results of this work can be used for the controlled immobilization of AnFaeA.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013JGRD..11810313H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013JGRD..11810313H"><span><span class="hlt">Charge</span> rearrangement deduced from nearby electric field measurements of an intracloud flash with K‒changes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hager, William W.; Feng, Wei</p> <p>2013-09-01</p> <p>An intracloud flash near Langmuir Laboratory is analyzed to determine the net rearrangement of <span class="hlt">charge</span>. The analysis employed data from a balloon borne electric field sensor, or Esonde, that was within a few hundred meters of the lightning channel, data from a similar Esonde on a mountain about 6.4 km from the balloon, and data from the New Mexico Institute of Mining and Technology Lightning Mapping Array (LMA). The recovery of the <span class="hlt">charge</span> transport required the solution of Poisson's equation over the mountainous terrain surrounding Langmuir Laboratory and the solution of a vastly under‒determined system of equations. The <span class="hlt">charge</span> movement is analyzed using a new smooth <span class="hlt">charge</span> transport model that incorporates constraints in the least squares fitting process through the use of penalty terms to smooth the <span class="hlt">charge</span> movement and prevent data overfitting. The electric field measurements were consistent with about 26% of the <span class="hlt">negative</span> <span class="hlt">charge</span> being transported to the end of the channel, 36% deposited along the channel in the positive region, 8% deposited near the start of the channel in the positive region, and 30% deposited in another positive region several kilometers beneath the main channel. The transport of <span class="hlt">negative</span> <span class="hlt">charge</span> to a lower positive region occurred during the K‒processes when some <span class="hlt">negative</span> <span class="hlt">charge</span> was also deposited along the main channel in the upper positive region. Hence, the <span class="hlt">charge</span> transport process during the K‒processes amounted to a tripolar <span class="hlt">charge</span> rearrangement where the <span class="hlt">charge</span> from the <span class="hlt">negative</span> region was transported to two distinct positive regions, the positive region along the main channel and a lower positive region beneath the main channel. High altitude, widely scattered LMA sources beyond the end of the main channel could indicate the existence of streamers which transported the end‒of‒channel <span class="hlt">charge</span> into the surrounding volume. Although the LMA showed the development of two upper channels, the <span class="hlt">charge</span> transport analysis showed that</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JPCM...30f4002U','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JPCM...30f4002U"><span>The effects of ion adsorption on the potential of zero <span class="hlt">charge</span> and the differential capacitance of <span class="hlt">charged</span> aqueous interfaces</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Uematsu, Yuki; Netz, Roland R.; Bonthuis, Douwe Jan</p> <p>2018-02-01</p> <p>Using a box profile approximation for the non-electrostatic surface adsorption potentials of anions and cations, we calculate the differential capacitance of aqueous electrolyte interfaces from a numerical solution of the Poisson-Boltzmann equation, including steric interactions between the ions and an inhomogeneous dielectric profile. Preferential adsorption of the positive (<span class="hlt">negative</span>) ion shifts the minimum of the differential capacitance to positive (<span class="hlt">negative</span>) surface potential values. The trends are similar for the potential of zero <span class="hlt">charge</span>; however, the potential of zero <span class="hlt">charge</span> does not correspond to the minimum of the differential capacitance in the case of asymmetric ion adsorption, contrary to the assumption commonly used to determine the potential of zero <span class="hlt">charge</span>. Our model can be used to obtain more accurate estimates of ion adsorption properties from differential capacitance or electrocapillary measurements. Asymmetric ion adsorption also affects the relative heights of the characteristic maxima in the differential capacitance curves as a function of the surface potential, but even for strong adsorption potentials the effect is small, making it difficult to reliably determine the adsorption properties from the peak heights.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23477295','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23477295"><span>Analysis of the kinetics of P+ HA- recombination in membrane-embedded wild-type and mutant Rhodobacter sphaeroides reaction centers between 298 and 77 K indicates that the adjacent <span class="hlt">negatively</span> <span class="hlt">charged</span> QA ubiquinone modulates the free energy of P+ HA- and may influence the rate of the protein dielectric response.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Gibasiewicz, Krzysztof; Pajzderska, Maria; Dobek, Andrzej; Brettel, Klaus; Jones, Michael R</p> <p>2013-09-26</p> <p>Time-resolved spectroscopic studies of recombination of the P(+)HA(-) radical pair in photosynthetic reaction centers (RCs) from Rhodobacter sphaeroides give an opportunity to study protein dynamics triggered by light and occurring over the lifetime of P(+)HA(-). The state P(+)HA(-) is formed after the ultrafast light-induced electron transfer from the primary donor pair of bacteriochlorophylls (P) to the acceptor bacteriopheophytin (HA). In order to increase the lifetime of this state, and thus increase the temporal window for the examination of protein dynamics, it is possible to block forward electron transfer from HA(-) to the secondary electron acceptor QA. In this contribution, the dynamics of P(+)HA(-) recombination were compared at a range of temperatures from 77 K to room temperature, electron transfer from HA(-) to QA being blocked either by prereduction of QA or by genetic removal of QA. The observed P(+)HA(-) <span class="hlt">charge</span> recombination was significantly slower in the QA-deficient RCs, and in both types of complexes, lowering the temperature from RT to 77 K led to a slowing of <span class="hlt">charge</span> recombination. The effects are explained in the frame of a model in which <span class="hlt">charge</span> recombination occurs via competing pathways, one of which is thermally activated and includes transient formation of a higher-energy state, P(+)BA(-). An internal electrostatic field supplied by the <span class="hlt">negative</span> <span class="hlt">charge</span> on QA increases the free energy levels of the state P(+)HA(-), thus decreasing its energetic distance to the state P(+)BA(-). In <span class="hlt">addition</span>, the dielectric response of the protein environment to the appearance of the state P(+)HA(-) is accelerated from ∼50-100 ns in the QA-deficient mutant RCs to ∼1-16 ns in WT RCs with a <span class="hlt">negatively</span> <span class="hlt">charged</span> QA(-). In both cases, the temperature dependence of the protein dynamics is weak.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/16185409','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/16185409"><span>[Clinical study and pathological examination on the treatment of deep partial thickness burn wound with <span class="hlt">negative</span> <span class="hlt">charge</span> aerosol].</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Li, Tian-zeng; Xu, Ying-bin; Hu, Xiao-gen; Shen, Rui; Peng, Xiao-dong; Wu, Wei-jiang; Luo, Lan; Dai, Xin-ming; Zou, Yong-tong; Qi, Shao-hai; Wu, Li-ping; Xie, Ju-lin; Deng, Xiao-xin; Chen, E; Zhang, Hui-Zhen</p> <p>2005-08-01</p> <p>To investigate the effect of <span class="hlt">negative</span> <span class="hlt">charge</span> aerosol (NCA) on the treatment of burn wound. Patients with superficial or deep partial thickness burn only were enrolled in the study, and they were randomly divided into trial group (T, including 180 cases of superficial thickness burn and 100 cases of deep partial thickness burn), control group (C, including 30 cases with superficial thickness burn and 30 with deep partial thickness burn), and self control group (SC, including 10 cases with superficial thickness burn and 10 with deep partial thickness burn). The patients in T and SC groups were treated with NCA for 1.5 hours, 1-2 times a day, from 6 postburn hour (PBH) to 2 postburn day (PBD), while those in C group received conventional treatment. For those in SC group, some of the wounds were covered with sterile schissel, while other wounds without schissel covering. The general changes in the wounds during NCA treatment were observed, and bacterial culture before and after NCA treatment was performed. The healing time was recorded and the blood biochemical parameters were determined. Rat model with deep partial thickness scald was established, and the rats were also divided into T and C groups, and received treatment as in human. Tissue samples were harvested from the wounds of rats in the 2 groups before and 1, 2, 3 weeks after treatment for pathological examination. There was no infection and little exudation in the patients in T group. No bacteria were found in the wound before and after NCA treatment. The healing time of the wounds of patients with superficial and deep partial thickness burn in T group was 6.3 +/- 1.6 d and 15.1 +/- 3.1 d, respectively, which was obviously shorter than those in C group (11.3 +/- 1.4 d and 21.2 +/- 1.4 d, P < 0.01). In SC group, the healing time of those with sterile schissel coverage was also significantly shorter than those without covering (P < 0.01). There was no obvious change in the liver and kidney functions and blood</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AIPA....8d7301A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AIPA....8d7301A"><span>Using magnetic <span class="hlt">charge</span> to understand soft-magnetic materials</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Arrott, Anthony S.; Templeton, Terry L.</p> <p>2018-04-01</p> <p>This is an overview of what the Landau-Lifshitz-Gilbert equations are doing in soft-magnetic materials with dimensions large compared to the exchange length. The surface magnetic <span class="hlt">charges</span> try to cancel applied magnetic fields inside the soft magnetic material. The exchange energy tries to reach a minimum while meeting the boundary conditions set by the magnetic <span class="hlt">charges</span> by using magnetization patterns that have a curl but no divergence. It can almost do this, but it still pays to add some divergence to further lower the exchange energy. There are then both positively and <span class="hlt">negatively</span> <span class="hlt">charged</span> regions in the bulk. The unlike <span class="hlt">charges</span> attract one another, but do not annihilate because they are paid for by the reduction in exchange energy. The micromagnetics of soft magnetic materials is about how those <span class="hlt">charges</span> rearrange themselves. The topology of magnetic <span class="hlt">charge</span> distributions presents challenges for mathematicians. No one guessed that they like to form helical patterns of extended multiples of <span class="hlt">charge</span> density.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFM.V12A..07H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFM.V12A..07H"><span>Advances in <span class="hlt">Charge</span>-Compensation in Secondary Ion Mass Spectrometry (SIMS)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hervig, R. L.; Chen, J.; Schauer, S.; Stanley, B. D.; Moore, G. M.; Roggensack, K.</p> <p>2012-12-01</p> <p>In secondary ion mass spectrometry (SIMS), a sample is bombarded by a <span class="hlt">charged</span> particle beam (the primary ion) and sputtered positive or <span class="hlt">negative</span> secondary ions are analyzed in a mass spectrometer. When the target is not conducting (like many geological materials), sample <span class="hlt">charging</span> can result in variable deflection of secondary ions away from the mass spectrometer and a low, unstable, or absent signal. Applying a thin conducting coat (e.g., C, Au) to polished samples is required, and if the primary ion beam is <span class="hlt">negatively-charged</span>, the build-up of <span class="hlt">negative</span> <span class="hlt">charge</span> can be alleviated by secondary electrons draining to the conducting coat at the edge of the crater (if a positive potential is applied to the sample for the collection of positive secondary ions) or accelerated away from the crater (if a <span class="hlt">negative</span> potential is applied for <span class="hlt">negative</span> ion study). Unless the sputtered crater in the conducting coat becomes too large, sample <span class="hlt">charging</span> can be kept at a controllable level, and high-quality trace element analyses and isotope ratios have been obtained using this technique over the past 3+ decades. When a positive primary beam is used, the resulting build-up of positive <span class="hlt">charge</span> in the sample requires an electron gun to deliver sufficient <span class="hlt">negative</span> <span class="hlt">charge</span> to the sputtered crater. While there are many examples of successful analyses using this approach, the purpose of this presentation is to describe a very simple technique for aligning the electron gun on Cameca nf and 1270/80 SIMS instruments. This method allows reproducible analyses of insulating phases with a Cs+ primary beam and detection of <span class="hlt">negative</span> secondary ions. Normally, the filament voltage on the E-gun is the same as the sample voltage; thus electrons do not strike the sample except when a positive <span class="hlt">charge</span> has built up (e.g., in the analysis crater!). In this method, we decrease the sample voltage by 3 or more kV, so that the impact energy of the electrons is sufficient to induce a cathodoluminescent (CL) image on an</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=243259','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=243259"><span>Concentration of poliovirus from tap water using positively <span class="hlt">charged</span> microporous filters.</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Sobsey, M D; Jones, B L</p> <p>1979-01-01</p> <p>Microporous filters that are more electropositive than the <span class="hlt">negatively</span> <span class="hlt">charged</span> filters currently used for virus concentrations from water by filter adsorption-elution methods were evaluated for poliovirus recovery from tap water. Zeta Plus filters composed of diatomaceous earth-cellulose-"<span class="hlt">charge</span>-modified" resin mixtures and having a net positive <span class="hlt">charge</span> of up to pH 5 to 6 efficiently adsorbed poliovirus from tap water at ambient pH levels 7.0 to 7.5 without added multivalent cation salts. The adsorbed virus were eluted with glycine-NaOH, pH 9.5 to 11.5. Electropositive asbestos-cellulose filters efficiently adsorbed poliovirus from tap water without added multivalent cation salts between pH 3.5 and 9.0, and the absorbed viruses could be eluted with 3% beef extract, pH 9, but not with pH 9.5 to 11.5 glycine-NaOH. Under water quality conditions in which poliovirus recoveries from large volumes of water were less than 5% with conventional <span class="hlt">negatively</span> <span class="hlt">charged</span> filters and standard methods, recoveries with Zeta Plus filters averaged 64 and 22.5% for one- and two-stage concentration procedures, respectively. Electropositive filters appear to offer distinct advantages over conventional <span class="hlt">negatively</span> <span class="hlt">charged</span> filters for concentrating enteric viruses from water, and their behavior tends to confirm the importance of electrostatic forces in virus recovery from water by microporous filter adsorption-elution methods. PMID:36844</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23413220','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23413220"><span>Direct analysis of samples under ambient condition by high-voltage-assisted laser desorption ionization mass spectrometry in both positive and <span class="hlt">negative</span> ion mode.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ren, Xinxin; Liu, Jia; Zhang, Chengsen; Luo, Hai</p> <p>2013-03-15</p> <p>With the rapid development of ambient mass spectrometry, the hybrid laser-based ambient ionization methods which can generate multiply <span class="hlt">charged</span> ions of large biomolecules and also characterize small molecules with good signal-to-noise in both positive and <span class="hlt">negative</span> ion modes are of particular interest. An ambient ionization method termed high-voltage-assisted laser desorption ionization (HALDI) is developed, in which a 1064 nm laser is used to desorb various liquid samples from the sample target biased at a high potential without the need for an organic matrix. The pre-<span class="hlt">charged</span> liquid samples are desorbed by the laser to form small <span class="hlt">charged</span> droplets which may undergo an electrospray-like ionization process to produce multiply <span class="hlt">charged</span> ions of large biomolecules. Various samples including proteins, oligonucleotides (ODNs), drugs, whole milk and chicken eggs have been analyzed by HALDI-MS in both positive and <span class="hlt">negative</span> ion mode with little or no sample preparation. In <span class="hlt">addition</span>, HALDI can generate intense signals with better signal-to-noise in <span class="hlt">negative</span> ion mode than laser desorption spay post-ionization (LDSPI) from the same samples, such as ODNs and some carboxylic-group-containing small drug molecules. HALDI-MS can directly analyze a variety of liquid samples including proteins, ODNs, pharmaceuticals and biological fluids in both positive and <span class="hlt">negative</span> ion mode without the use of an organic matrix. This technique may be further developed into a useful tool for rapid analysis in many different fields such as pharmaceutical, food, and biological sciences. Copyright © 2013 John Wiley & Sons, Ltd.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29263979','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29263979"><span>Hybrid Simulations of Positively and <span class="hlt">Negatively</span> <span class="hlt">Charged</span> Pickup Ions and Cyclotron Wave Generation at Europa.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Desai, R T; Cowee, M M; Wei, H; Fu, X; Gary, S P; Volwerk, M; Coates, A J</p> <p>2017-10-01</p> <p>In the vicinity of Europa, Galileo observed bursty Alfvén-cyclotron wave power at the gyrofrequencies of a number of species including K + , O 2+, Na + , and Cl + , indicating the localized pickup of these species. <span class="hlt">Additional</span> evidence for the presence of chlorine was the occurrence of both left-hand (LH) and right-hand (RH) polarized transverse wave power near the Cl + gyrofrequency, thought to be due to the pickup of both Cl + and the easily formed chlorine anion, Cl - . To test this hypothesis, we use one-dimensional hybrid (kinetic ion, massless fluid electron) simulations for both positive and <span class="hlt">negative</span> pickup ions and self-consistently reproduce the growth of both LH and RH Alfvén-cyclotron waves in agreement with linear theory. We show how the simultaneous generation of LH and RH waves can result in nongyrotropic ion distributions and increased wave amplitudes, and how even trace quantities of <span class="hlt">negative</span> pickup ions are able to generate an observable RH signal. Through comparing simulated and observed wave amplitudes, we are able to place the first constraints on the densities of Chlorine pickup ions in localized regions at Europa.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007JAP...101h1713B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007JAP...101h1713B"><span>Spin properties of <span class="hlt">charged</span> Mn-doped quantum dota)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Besombes, L.; Léger, Y.; Maingault, L.; Mariette, H.</p> <p>2007-04-01</p> <p>The optical properties of individual quantum dots doped with a single Mn atom and <span class="hlt">charged</span> with a single carrier are analyzed. The emission of the neutral, <span class="hlt">negatively</span> and positively <span class="hlt">charged</span> excitons coupled with a single magnetic atom (Mn) are observed in the same individual quantum dot. The spectrum of the <span class="hlt">charged</span> excitons in interaction with the Mn atom shows a rich pattern attributed to a strong anisotropy of the hole-Mn exchange interaction slightly perturbed by a small valence-band mixing. The anisotropy in the exchange interaction between a single magnetic atom and a single hole is revealed by comparing the emission of a <span class="hlt">charged</span> Mn-doped quantum dot in longitudinal and transverse magnetic field.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/40205568-negatively-charged-excitons-photoluminescence-asymmetric-quantum-wells','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/40205568-negatively-charged-excitons-photoluminescence-asymmetric-quantum-wells"><span><span class="hlt">Negatively</span> <span class="hlt">charged</span> excitons and photoluminescence in asymmetric quantum wells</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Szlufarska, Izabela; Wojs, Arkadiusz; Quinn, John J.</p> <p>2001-02-15</p> <p>We study photoluminescence (PL) of <span class="hlt">charged</span> excitons (X{sup -}) in narrow asymmetric quantum wells in high magnetic fields B. The binding of all X{sup -} states strongly depends on the separation {delta} of electron and hole layers. The most sensitive is the ''bright'' singlet, whose binding energy decreases quickly with increasing {delta} even at relatively small B. As a result, the value of B at which the singlet-triplet crossing occurs in the X{sup -} spectrum also depends on {delta}, and decreases from 35 T in a symmetric 10 nm GaAs well to 16 T for {delta}=0.5 nm. Since the criticalmore » values of {delta} at which different X{sup -} states unbind are surprisingly small compared to the well width, the observation of strongly bound X{sup -} states in an experimental PL spectrum implies virtually no layer displacement in the sample. This casts doubt on the interpretation of PL spectra of heterojunctions in terms of X{sup -} recombination.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1364315','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1364315"><span>Interaction of the Antimicrobial Peptide Aurein 1.2 and <span class="hlt">Charged</span> Lipid Bilayer</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Rai, Durgesh K.; Qian, Shuo</p> <p></p> <p>Aurein 1.2 is a potent antimicrobial peptide secreted by frog Litoria aurea. As a short membrane-active peptide with only 13 amino acids in sequence, it has been found to be residing on the surface of lipid bilayer and permeabilizing bacterial membranes at high concentration. However, the detail at the molecular level is largely unknown. Here in this study, we investigated the action of Aurein 1.2 in <span class="hlt">charged</span> lipid bilayers composed of DMPC/DMPG. Oriented Circular Dichroism results showed that the peptide was on the surface of lipid bilayer regardless of the <span class="hlt">charged</span> lipid ratio. Only at a very high peptide-to-lipid ratiomore » (~1/10), the peptide became perpendicular to the bilayer, however no pore was detected by neutron in-plane scattering. To further understand how it interacted with <span class="hlt">charged</span> lipid bilayers, we employed Small Angle Neutron Scattering to probe lipid distribution across bilayer leaflets in lipid vesicles. The results showed that Aurein 1.2 interacted strongly with <span class="hlt">negatively</span> <span class="hlt">charged</span> DMPG, causing strong asymmetry in lipid bilayer. At high concentration, while the vesicles were intact, we found <span class="hlt">additional</span> structure feature on the bilayer. Finally, our study provides a glimpse into how Aurein 1.2 disturbs anionic lipid-containing membranes without pore formation.« less</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li class="active"><span>14</span></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_14 --> <div id="page_15" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li class="active"><span>15</span></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="281"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1364315-interaction-antimicrobial-peptide-aurein-charged-lipid-bilayer','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1364315-interaction-antimicrobial-peptide-aurein-charged-lipid-bilayer"><span>Interaction of the Antimicrobial Peptide Aurein 1.2 and <span class="hlt">Charged</span> Lipid Bilayer</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Rai, Durgesh K.; Qian, Shuo</p> <p>2017-06-16</p> <p>Aurein 1.2 is a potent antimicrobial peptide secreted by frog Litoria aurea. As a short membrane-active peptide with only 13 amino acids in sequence, it has been found to be residing on the surface of lipid bilayer and permeabilizing bacterial membranes at high concentration. However, the detail at the molecular level is largely unknown. Here in this study, we investigated the action of Aurein 1.2 in <span class="hlt">charged</span> lipid bilayers composed of DMPC/DMPG. Oriented Circular Dichroism results showed that the peptide was on the surface of lipid bilayer regardless of the <span class="hlt">charged</span> lipid ratio. Only at a very high peptide-to-lipid ratiomore » (~1/10), the peptide became perpendicular to the bilayer, however no pore was detected by neutron in-plane scattering. To further understand how it interacted with <span class="hlt">charged</span> lipid bilayers, we employed Small Angle Neutron Scattering to probe lipid distribution across bilayer leaflets in lipid vesicles. The results showed that Aurein 1.2 interacted strongly with <span class="hlt">negatively</span> <span class="hlt">charged</span> DMPG, causing strong asymmetry in lipid bilayer. At high concentration, while the vesicles were intact, we found <span class="hlt">additional</span> structure feature on the bilayer. Finally, our study provides a glimpse into how Aurein 1.2 disturbs anionic lipid-containing membranes without pore formation.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/15783594','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/15783594"><span>Optical pumping of the electronic and nuclear spin of single <span class="hlt">charge</span>-tunable quantum dots.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Bracker, A S; Stinaff, E A; Gammon, D; Ware, M E; Tischler, J G; Shabaev, A; Efros, Al L; Park, D; Gershoni, D; Korenev, V L; Merkulov, I A</p> <p>2005-02-04</p> <p>We present a comprehensive examination of optical pumping of spins in individual GaAs quantum dots as we change the net <span class="hlt">charge</span> from positive to neutral to <span class="hlt">negative</span> with a <span class="hlt">charge</span>-tunable heterostructure. <span class="hlt">Negative</span> photoluminescence polarization memory is enhanced by optical pumping of ground state electron spins, which we prove with the first measurements of the Hanle effect on an individual quantum dot. We use the Overhauser effect in a high longitudinal magnetic field to demonstrate efficient optical pumping of nuclear spins for all three <span class="hlt">charge</span> states of the quantum dot.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005PhRvL..94d7402B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005PhRvL..94d7402B"><span>Optical Pumping of the Electronic and Nuclear Spin of Single <span class="hlt">Charge</span>-Tunable Quantum Dots</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bracker, A. S.; Stinaff, E. A.; Gammon, D.; Ware, M. E.; Tischler, J. G.; Shabaev, A.; Efros, Al. L.; Park, D.; Gershoni, D.; Korenev, V. L.; Merkulov, I. A.</p> <p>2005-02-01</p> <p>We present a comprehensive examination of optical pumping of spins in individual GaAs quantum dots as we change the net <span class="hlt">charge</span> from positive to neutral to <span class="hlt">negative</span> with a <span class="hlt">charge</span>-tunable heterostructure. <span class="hlt">Negative</span> photoluminescence polarization memory is enhanced by optical pumping of ground state electron spins, which we prove with the first measurements of the Hanle effect on an individual quantum dot. We use the Overhauser effect in a high longitudinal magnetic field to demonstrate efficient optical pumping of nuclear spins for all three <span class="hlt">charge</span> states of the quantum dot.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19930061215&hterms=renyi&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Drenyi','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19930061215&hterms=renyi&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Drenyi"><span>Comment on 'The effect of liquid water on thunderstorm <span class="hlt">charging</span>' by C.P.R. Saunders et al</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Williams, Earle; Zhang, Renyi</p> <p>1993-01-01</p> <p>This paper is a comment on the claims made in the paper by Saunders et al. (1991), which reports on a laboratory simulation of ice particle <span class="hlt">charging</span> in thunderstorms, concerning the microphysical condition of riming ice particles and the conditions for sublimation and <span class="hlt">negative</span> <span class="hlt">charging</span> in thunderclouds. It is argued that the interpretation of Saunders is contrary to the findings of Williams et al. (1991), which support the hypothesis that sublimating graupel <span class="hlt">charge</span> <span class="hlt">negatively</span> (in collision with smaller ice particles) and graupel in deposition <span class="hlt">charge</span> positively. Based on microphysical calculations as well as observations in thunderclouds, it is concluded that, while sublimation of the rimer surface and <span class="hlt">negative</span> <span class="hlt">charging</span> do not appear to account for the laboratory observations reported by Saunders et al., these authors do not have sufficient evidence for rejecting the sublimation hypothesis presented by Williams et al. (1991) for thunderstorms.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/867839','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/867839"><span>High brilliance <span class="hlt">negative</span> ion and neutral beam source</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Compton, Robert N.</p> <p>1991-01-01</p> <p>A high brilliance mass selected (Z-selected) <span class="hlt">negative</span> ion and neutral beam source having good energy resolution. The source is based upon laser resonance ionization of atoms or molecules in a small gaseous medium followed by <span class="hlt">charge</span> exchange through an alkali oven. The source is capable of producing microampere beams of an extremely wide variety of <span class="hlt">negative</span> ions, and milliampere beams when operated in the pulsed mode.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22493872-attraction-likely-charged-nano-sized-grains-dust-electron-plasmas','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22493872-attraction-likely-charged-nano-sized-grains-dust-electron-plasmas"><span>Attraction of likely <span class="hlt">charged</span> nano-sized grains in dust-electron plasmas</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Vishnyakov, Vladimir I., E-mail: eksvar@ukr.net</p> <p>2016-01-15</p> <p>Dust-electron plasma, which contains only the dust grains and electrons, emitted by them, is studied. Assumption of almost uniform spatial electrons distribution, which deviates from the uniformity only near the dust grains, leads to the grain <span class="hlt">charge</span> division into two parts: first part is the individual for each grain “visible” <span class="hlt">charge</span> and the second part is the common <span class="hlt">charge</span> of the neutralized background. The visible grain <span class="hlt">charge</span> can be both <span class="hlt">negative</span> and positive, while the total grain <span class="hlt">charge</span> is only positive. The attraction of likely <span class="hlt">charged</span> grains is possible, because the grain interaction is determined by the visible <span class="hlt">charges</span>. Themore » equilibrium state between attraction and repulsion of grains is demonstrated.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140003213','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140003213"><span>Solar Array and Auroral <span class="hlt">Charging</span> Studies of DMSP Spacecraft</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Matias, Kelwin</p> <p>2013-01-01</p> <p>The SSJ electrostatic analyzers and the SSIES plasma instruments on the DMSP spacecraft in low Earth polar orbit can be used to conduct case studies of auroral and solar array <span class="hlt">charging</span>. We will use a program written in the Interactive Data Language (IDL) to evaluate questionable <span class="hlt">charging</span> events in the SSJ records by comparing <span class="hlt">charging</span> signatures in SSJ and SSIES data. In <span class="hlt">addition</span>, we will assemble a number of case studies of solar array <span class="hlt">charging</span> showing the signatures from the SSJ data and compare to the SSIES <span class="hlt">charging</span> signatures. In <span class="hlt">addition</span> we will use Satellite Tool Kit (STK) to propagate orbits, obtain solar intensity, and use to verify onset of <span class="hlt">charging</span> with sunrise.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20100040613','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20100040613"><span>Assessment and Control of Spacecraft <span class="hlt">Charging</span> Risks on the International Space Station</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Koontz, Steve; Edeen, Marybeth; Spetch, William; Dalton, Penni; Keening, Thomas</p> <p>2003-01-01</p> <p>Electrical interactions between the F2 region ionospheric plasma and the 160V photovoltaic (PV) electrical power system on the International Space Station (ISS) can produce floating potentials (FP) on the ISS conducting structure of greater magnitude than are usually observed on spacecraft in low-Earth orbit. Flight through the geomagnetic field also causes magnetic induction <span class="hlt">charging</span> of ISS conducting structure. <span class="hlt">Charging</span> processes resulting from interaction of ISS with auroral electrons may also contribute to <span class="hlt">charging</span> albeit rarely. The magnitude and frequency of occurrence of possibly hazardous <span class="hlt">charging</span> events depends on the ISS assembly stage (six more 160V PV arrays will be added to ISS), ISS flight configuration, ISS position (latitude and longitude), and the natural variability in the ionospheric flight environment. At present, ISS is equipped with two plasma contactors designed to control ISS FP to within 40 volts of the ambient F2 plasma. The <span class="hlt">negative</span>-polarity grounding scheme utilized in the ISS 160V power system leads, naturally, to <span class="hlt">negative</span> values of ISS FP. A <span class="hlt">negative</span> ISS structural FP leads to application of electrostatic fields across the dielectrics that separate conducting structure from the ambient F2 plasma, thereby enabling dielectric breakdown and arcing. Degradation of some thermal control coatings and noise in electrical systems can result. Continued review and evaluation of the putative <span class="hlt">charging</span> hazards, as required by the ISS Program Office, revealed that ISS <span class="hlt">charging</span> could produce a risk of electric shock to the ISS crew during extra vehicular activity. ISS <span class="hlt">charging</span> risks are being evaluated in ongoing ISS <span class="hlt">charging</span> measurements and analysis campaigns. The results of ISS <span class="hlt">charging</span> measurements are combined with a recently developed detailed model of the ISS <span class="hlt">charging</span> process and an extensive analysis of historical ionospheric variability data, to assess ISS <span class="hlt">charging</span> risks using Probabilistic Risk Assessment (PRA) methods. The PRA analysis</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014PhRvB..89s5123M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014PhRvB..89s5123M"><span>Coulombic <span class="hlt">charge</span> ice</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>McClarty, P. A.; O'Brien, A.; Pollmann, F.</p> <p>2014-05-01</p> <p>We consider a classical model of <span class="hlt">charges</span> ±q on a pyrochlore lattice in the presence of long-range Coulomb interactions. This model first appeared in the early literature on <span class="hlt">charge</span> order in magnetite [P. W. Anderson, Phys. Rev. 102, 1008 (1956), 10.1103/PhysRev.102.1008]. In the limit where the interactions become short ranged, the model has a ground state with an extensive entropy and dipolar <span class="hlt">charge-charge</span> correlations. When long-range interactions are introduced, the exact degeneracy is broken. We study the thermodynamics of the model and show the presence of a correlated <span class="hlt">charge</span> liquid within a temperature window in which the physics is well described as a liquid of screened <span class="hlt">charged</span> defects. The structure factor in this phase, which has smeared pinch points at the reciprocal lattice points, may be used to detect <span class="hlt">charge</span> ice experimentally. In <span class="hlt">addition</span>, the model exhibits fractionally <span class="hlt">charged</span> excitations ±q/2 which are shown to interact via a 1/r potential. At lower temperatures, the model exhibits a transition to a long-range ordered phase. We are able to treat the Coulombic <span class="hlt">charge</span> ice model and the dipolar spin ice model on an equal footing by mapping both to a constrained <span class="hlt">charge</span> model on the diamond lattice. We find that states of the two ice models are related by a staggering field which is reflected in the energetics of these two models. From this perspective, we can understand the origin of the spin ice and <span class="hlt">charge</span> ice ground states as coming from a dipolar model on a diamond lattice. We study the properties of <span class="hlt">charge</span> ice in an external electric field, finding that the correlated liquid is robust to the presence of a field in contrast to the case of spin ice in a magnetic field. Finally, we comment on the transport properties of Coulombic <span class="hlt">charge</span> ice in the correlated liquid phase.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016Nanos...8.7695G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016Nanos...8.7695G"><span>Metal nanoparticles triggered persistent <span class="hlt">negative</span> photoconductivity in silk protein hydrogels</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gogurla, Narendar; Sinha, Arun K.; Naskar, Deboki; Kundu, Subhas C.; Ray, Samit K.</p> <p>2016-03-01</p> <p>Silk protein is a natural biopolymer with intriguing properties, which are attractive for next generation bio-integrated electronic and photonic devices. Here, we demonstrate the <span class="hlt">negative</span> photoconductive response of Bombyx mori silk protein fibroin hydrogels, triggered by Au nanoparticles. The room temperature electrical conductivity of Au-silk hydrogels is found to be enhanced with the incorporation of Au nanoparticles over the control sample, due to the increased <span class="hlt">charge</span> transporting networks within the hydrogel. Au-silk lateral photoconductor devices show a unique <span class="hlt">negative</span> photoconductive response under an illumination of 325 nm, with excitation energy higher than the characteristic metal plasmon resonance band. The enhanced photoconductance yield in the hydrogels over the silk protein is attributed to the photo-oxidation of amino groups in the β-pleated sheets of the silk around the Au nanoparticles followed by the breaking of <span class="hlt">charge</span> transport networks. The Au-silk nanocomposite does not show any photoresponse under visible illumination because of the localization of excited <span class="hlt">charges</span> in Au nanoparticles. The <span class="hlt">negative</span> photoconductive response of hybrid Au-silk under UV illumination may pave the way towards the utilization of silk for future bio-photonic devices using metal nanoparticle platforms.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23532939','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23532939"><span>Stabilization of enzymes in ionic liquids via modification of enzyme <span class="hlt">charge</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Nordwald, Erik M; Kaar, Joel L</p> <p>2013-09-01</p> <p>Due to the propensity of ionic liquids (ILs) to inactivate enzymes, the development of strategies to improve enzyme utility in these solvents is critical to fully exploit ILs for biocatalysis. We have developed a strategy to broadly improve enzyme utility in ILs based on elucidating the effect of <span class="hlt">charge</span> modifications on the function of enzymes in IL environments. Results of stability studies in aqueous-IL mixtures indicated a clear connection between the ratio of enzyme-containing positive-to-<span class="hlt">negative</span> sites and enzyme stability in ILs. Stability studies of the effect of [BMIM][Cl] and [EMIM][EtSO4 ] on chymotrypsin specifically found an optimum ratio of positively-<span class="hlt">charged</span> amine-to-<span class="hlt">negatively-charged</span> acid groups (0.39). At this ratio, the half-life of chymotrypsin was increased 1.6- and 4.3-fold relative to wild-type chymotrypsin in [BMIM][Cl] and [EMIM][EtSO4 ], respectively. The half-lives of lipase and papain were similarly increased as much as 4.0 and 2.4-fold, respectively, in [BMIM][Cl] by modifying the ratio of positive-to-<span class="hlt">negative</span> sites of each enzyme. More generally, the results of stability studies found that modifications that reduce the ratio of enzyme-containing positive-to-<span class="hlt">negative</span> sites improve enzyme stability in ILs. Understanding the impact of <span class="hlt">charge</span> modification on enzyme stability in ILs may ultimately be exploited to rationally engineer enzymes for improved function in IL environments. Copyright © 2013 Wiley Periodicals, Inc.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29283252','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29283252"><span><span class="hlt">Negative</span> Differential Conductance in Polyporphyrin Oligomers with Nonlinear Backbones.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kuang, Guowen; Chen, Shi Zhang; Yan, Linghao; Chen, Ke Qiu; Shang, Xuesong; Liu, Pei Nian; Lin, Nian</p> <p>2018-01-17</p> <p>We study <span class="hlt">negative</span> differential conductance (NDC) effects in polyporphyrin oligomers with nonlinear backbones. Using a low-temperature scanning tunneling microscope, we selectively controlled the <span class="hlt">charge</span> transport path in single oligomer wires. We observed robust NDC when <span class="hlt">charge</span> passed through a T-shape junction, bistable NDC when <span class="hlt">charge</span> passed through a 90° kink and no NDC when <span class="hlt">charge</span> passed through a 120° kink. Aided by density functional theory with nonequilibrium Green's functions simulations, we attributed this backbone-dependent NDC to bias-modulated hybridization of the electrode states with the resonant transport molecular orbital. We argue this mechanism is generic in molecular systems, which opens a new route of designing molecular NDC devices.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AIPA....8b5209C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AIPA....8b5209C"><span>Modulating the line shape of magnetoconductance by varying the <span class="hlt">charge</span> injection in polymer light-emitting diodes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chitraningrum, Nidya; Chu, Ting-Yi; Huang, Ping-Tsung; Wen, Ten-Chin; Guo, Tzung-Fang</p> <p>2018-02-01</p> <p>We fabricate the phenyl-substituted poly(p-phenylene vinylene) copolymer (super yellow, SY-PPV)-based polymer light-emitting diodes (PLEDs) with different device architectures to modulate the injection of opposite <span class="hlt">charge</span> carriers and investigate the corresponding magnetoconductance (MC) responses. At the first glance, we find that all PLEDs exhibit the positive MC responses. By applying the mathematical analysis to fit the curves with two empirical equations of a non-Lorentzian and a Lorentzian function, we are able to extract the hidden <span class="hlt">negative</span> MC component from the positive MC curve. We attribute the growth of the <span class="hlt">negative</span> MC component to the reduced interaction of the triplet excitons with <span class="hlt">charges</span> to generate the free <span class="hlt">charge</span> carriers as modulated by the applied magnetic field, known as the triplet exciton-<span class="hlt">charge</span> reaction, by analyzing MC responses for PLEDs of the <span class="hlt">charge</span>-unbalanced and hole-blocking device configurations. The <span class="hlt">negative</span> MC component causes the broadening of the line shape in MC curves.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3945335','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3945335"><span><span class="hlt">Charge</span> Segregation and Low Hydrophobicity Are Key Features of Ribosomal Proteins from Different Organisms*</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Fedyukina, Daria V.; Jennaro, Theodore S.; Cavagnero, Silvia</p> <p>2014-01-01</p> <p>Ribosomes are large and highly <span class="hlt">charged</span> macromolecular complexes consisting of RNA and proteins. Here, we address the electrostatic and nonpolar properties of ribosomal proteins that are important for ribosome assembly and interaction with other cellular components and may influence protein folding on the ribosome. We examined 50 S ribosomal subunits from 10 species and found a clear distinction between the net <span class="hlt">charge</span> of ribosomal proteins from halophilic and non-halophilic organisms. We found that ∼67% ribosomal proteins from halophiles are <span class="hlt">negatively</span> <span class="hlt">charged</span>, whereas only up to ∼15% of ribosomal proteins from non-halophiles share this property. Conversely, hydrophobicity tends to be lower for ribosomal proteins from halophiles than for the corresponding proteins from non-halophiles. Importantly, the surface electrostatic potential of ribosomal proteins from all organisms, especially halophiles, has distinct positive and <span class="hlt">negative</span> regions across all the examined species. Positively and <span class="hlt">negatively</span> <span class="hlt">charged</span> residues of ribosomal proteins tend to be clustered in buried and solvent-exposed regions, respectively. Hence, the majority of ribosomal proteins is characterized by a significant degree of intramolecular <span class="hlt">charge</span> segregation, regardless of the organism of origin. This key property enables the ribosome to accommodate proteins within its complex scaffold regardless of their overall net <span class="hlt">charge</span>. PMID:24398678</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4307797','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4307797"><span>Inversion of membrane surface <span class="hlt">charge</span> by trivalent cations probed with a cation-selective channel</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Gurnev, Philip A.; Bezrukov, Sergey M.</p> <p>2014-01-01</p> <p>We demonstrate that the cation-selective channel formed by gramicidin A can be used as a reliable sensor for studying the multivalent ion accumulation at the surfaces of <span class="hlt">charged</span> lipid membranes and the “<span class="hlt">charge</span> inversion” phenomenon. In asymmetrically <span class="hlt">charged</span> membranes with the individual leaflets formed from pure <span class="hlt">negative</span> and positive lipids bathed by 0.1 M CsCl solutions the channel exhibits current rectification which is comparable to that of a typical n/p semiconductor diode. We show that even at these highly asymmetrical conditions the channel conductance can be satisfactorily described by the electrodiffusion equation in the constant field approximation but, due to predictable limitations, only when the applied voltages do not exceed 50 mV. Analysis of the changes in the voltage-dependent channel conductance upon <span class="hlt">addition</span> of trivalent cations allows us to gauge their interactions with the membrane surface. The inversion of the sign of the effective surface <span class="hlt">charge</span> takes place at the concentrations which correlate with the cation size. Specifically, these concentrations are close to 0.05 mM for lanthanum, 0.25 mM for hexaamminecobalt, and 4 mM for spermidine. PMID:23088396</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23088396','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23088396"><span>Inversion of membrane surface <span class="hlt">charge</span> by trivalent cations probed with a cation-selective channel.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Gurnev, Philip A; Bezrukov, Sergey M</p> <p>2012-11-13</p> <p>We demonstrate that the cation-selective channel formed by gramicidin A can be used as a reliable sensor for studying the multivalent ion accumulation at the surfaces of <span class="hlt">charged</span> lipid membranes and the "<span class="hlt">charge</span> inversion" phenomenon. In asymmetrically <span class="hlt">charged</span> membranes with the individual leaflets formed from pure <span class="hlt">negative</span> and positive lipids bathed by 0.1 M CsCl solutions the channel exhibits current rectification, which is comparable to that of a typical n/p semiconductor diode. We show that even at these highly asymmetrical conditions the channel conductance can be satisfactorily described by the electrodiffusion equation in the constant field approximation but, due to predictable limitations, only when the applied voltages do not exceed 50 mV. Analysis of the changes in the voltage-dependent channel conductance upon <span class="hlt">addition</span> of trivalent cations allows us to gauge their interactions with the membrane surface. The inversion of the sign of the effective surface <span class="hlt">charge</span> takes place at the concentrations, which correlate with the cation size. Specifically, these concentrations are close to 0.05 mM for lanthanum, 0.25 mM for hexaamminecobalt, and 4 mM for spermidine.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002EGSGA..27.5139A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002EGSGA..27.5139A"><span>Spacecraft <span class="hlt">Charging</span> Hazards In Low-earth Orbit</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Anderson, P. C.</p> <p></p> <p>The space environment in low-Earth orbit (LEO) has until recently been considered quite benign to high levels of spacecraft <span class="hlt">charging</span>. However, it has been found that the DMSP spacecraft at 840 km can <span class="hlt">charge</span> to very large <span class="hlt">negative</span> voltages (up to - 2000 V) when encountering intense precipitating electron events (auroral arcs) while traversing the auroral zone. The occurrence frequency of <span class="hlt">charging</span> events, defined as when the spacecraft <span class="hlt">charged</span> to levels exceeding 100 V <span class="hlt">negative</span>, was highly correlated with the 11-year solar cycle with the largest number of events occurring during solar minimum. This was due to the requirement that the background thermal plasma den- sity be low, at most 104 cm-2. During solar maximum, the plasma density is typically well above that level due to the solar EUV ionizing radiation, and although the oc- currence frequency of auroral arcs is considerably greater than at solar minimum, the occurrence of high-level <span class="hlt">charging</span> is minimal. Indeed, of the over 1200 events found during the most recent solar cycle, none occurred during the last solar maximum. This has implications to a number of LEO satellite programs, including the International Space Station (ISS). The plasma density in the ISS orbit, at a much lower altitude than DMSP, is well above that at 840 km and rarely below 104 cm-2. However, in the wake of the ISS, the plasma density can be 2 orders of magnitude or more lower than the background density and thus conditions are ripe for significant <span class="hlt">charging</span> effects. With an inclination of 51.6 degrees, the ISS does enter the auroral zone, particularly during geomagnetic storms and substorms when the auroral boundary can penetrate to very low latitudes. This has significant implications for EVA operations in the ISS wake.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005PhyB..362..199V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005PhyB..362..199V"><span>Influence of composition on phase occurrence during <span class="hlt">charge</span> process of AB 5+x Ni-MH <span class="hlt">negative</span> electrode materials</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vivet, S.; Latroche, M.; Chabre, Y.; Joubert, J.-M.; Knosp, B.; Percheron-Guégan, A.</p> <p>2005-05-01</p> <p>Multi-substituted LaNi 5-type alloys (AB 5+x) are widely used as <span class="hlt">negative</span> electrode materials in commercial Ni-MH batteries. Cobalt substitution on Ni sites allows to enhance battery cycle life by reducing alloy pulverization induced by hydrogen cycling. This improvement is attributed to the occurrence of a three-phase process (α, β and γ) during electrochemical hydrogen loading. In order to better understand the effect of the composition on the phase occurrence and to reduce the rate of costly cobalt, an in situ neutron diffraction study has been performed at room temperature during electrochemical <span class="hlt">charge</span> of two different electrode materials MmNi 4.07Mn 0.63Al 0.2M 0.4 with M=Fe and Mn and B/A=5.3. These cobalt free compounds show cycle life comparable to that of commercial materials. The results show that three phases are also observed for these samples. The γ-phase content depends on M and is higher for M=Fe than for M=Mn. These results are related to the improved cycle lives and to the alloy pulverization process.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1339417','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1339417"><span>The effect of <span class="hlt">charging</span> rate on the graphite electrode of commercial lithium-ion cells: A post-mortem study</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Somerville, L.; Bareno, J.; Trask, S.</p> <p></p> <p>Increased <span class="hlt">charging</span> rates <span class="hlt">negatively</span> affect the lifetime of lithium-ion cells by increasing cell resistance and reducing capacity. This work is a post-mortem study of 18650 cells subjected to <span class="hlt">charge</span> rates of 0.7-, 2-, 4-, and 6-C. For cells <span class="hlt">charged</span> at 0.7-C to 4-C, this performance degradation is primarily related to surface film thickness with no observable change in surface film chemical composition. However, at <span class="hlt">charge</span> rates of 6-C, the chemical composition of the surface film changes significantly, suggesting that this change is the reason for the sharper increase in cell resistance compared to the lower <span class="hlt">charge</span> rates. In <span class="hlt">addition</span>, wemore » found that surface film formation was not uniform across the electrode. Surface film was thicker and chemically different along the central band of the electrode “jelly roll”. This result is most likely attributable to an increase in temperature that results from non-uniform electrode wetting during manufacture. As a result, this non-uniform change further resulted in active material delamination from the current collector owing to chemical changes to the binder for the cell <span class="hlt">charged</span> at 6-C.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1339417-effect-charging-rate-graphite-electrode-commercial-lithium-ion-cells-post-mortem-study','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1339417-effect-charging-rate-graphite-electrode-commercial-lithium-ion-cells-post-mortem-study"><span>The effect of <span class="hlt">charging</span> rate on the graphite electrode of commercial lithium-ion cells: A post-mortem study</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Somerville, L.; Bareno, J.; Trask, S.; ...</p> <p>2016-10-22</p> <p>Increased <span class="hlt">charging</span> rates <span class="hlt">negatively</span> affect the lifetime of lithium-ion cells by increasing cell resistance and reducing capacity. This work is a post-mortem study of 18650 cells subjected to <span class="hlt">charge</span> rates of 0.7-, 2-, 4-, and 6-C. For cells <span class="hlt">charged</span> at 0.7-C to 4-C, this performance degradation is primarily related to surface film thickness with no observable change in surface film chemical composition. However, at <span class="hlt">charge</span> rates of 6-C, the chemical composition of the surface film changes significantly, suggesting that this change is the reason for the sharper increase in cell resistance compared to the lower <span class="hlt">charge</span> rates. In <span class="hlt">addition</span>, wemore » found that surface film formation was not uniform across the electrode. Surface film was thicker and chemically different along the central band of the electrode “jelly roll”. This result is most likely attributable to an increase in temperature that results from non-uniform electrode wetting during manufacture. As a result, this non-uniform change further resulted in active material delamination from the current collector owing to chemical changes to the binder for the cell <span class="hlt">charged</span> at 6-C.« less</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li class="active"><span>15</span></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_15 --> <div id="page_16" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li class="active"><span>16</span></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="301"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18569691','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18569691"><span>Memory for media: investigation of false memories for <span class="hlt">negatively</span> and positively <span class="hlt">charged</span> public events.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Porter, Stephen; Taylor, Kristian; Ten Brinke, Leanne</p> <p>2008-01-01</p> <p>Despite a large body of false memory research, little has addressed the potential influence of an event's emotional content on susceptibility to false recollections. The Paradoxical <span class="hlt">Negative</span> Emotion (PNE) hypothesis predicts that <span class="hlt">negative</span> emotion generally facilitates memory but also heightens susceptibility to false memories. Participants were asked whether they could recall 20 "widely publicised" public events (half fictitious) ranging in emotional valence, with or without visual cues. Participants recalled a greater number of true <span class="hlt">negative</span> events (M=3.31/5) than true positive (M=2.61/5) events. Nearly everyone (95%) came to recall at least one false event (M=2.15 false events recalled). Further, more than twice as many participants recalled any false <span class="hlt">negative</span> (90%) compared to false positive (41.7%) events. <span class="hlt">Negative</span> events, in general, were associated with more detailed memories and false <span class="hlt">negative</span> event memories were more detailed than false positive event memories. Higher dissociation scores were associated with false recollections of <span class="hlt">negative</span> events, specifically.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110016853','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110016853"><span><span class="hlt">Charge</span>-Dissipative Electrical Cables</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kolasinski, John R.; Wollack, Edward J.</p> <p>2004-01-01</p> <p>Electrical cables that dissipate spurious static electric <span class="hlt">charges</span>, in <span class="hlt">addition</span> to performing their main functions of conducting signals, have been developed. These cables are intended for use in trapped-ion or ionizing-radiation environments, in which electric <span class="hlt">charges</span> tend to accumulate within, and on the surfaces of, dielectric layers of cables. If the <span class="hlt">charging</span> rate exceeds the dissipation rate, <span class="hlt">charges</span> can accumulate in excessive amounts, giving rise to high-current discharges that can damage electronic circuitry and/or systems connected to it. The basic idea of design and operation of <span class="hlt">charge</span>-dissipative electrical cables is to drain spurious <span class="hlt">charges</span> to ground by use of lossy (slightly electrically conductive) dielectric layers, possibly in conjunction with drain wires and/or drain shields (see figure). In typical cases, the drain wires and/or drain shields could be electrically grounded via the connector assemblies at the ends of the cables, in any of the conventional techniques for grounding signal conductors and signal shields. In some cases, signal shields could double as drain shields.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018NJPh...20b3002L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018NJPh...20b3002L"><span><span class="hlt">Charged</span> dopants in neutral supercells through substitutional donor (acceptor): nitrogen donor <span class="hlt">charging</span> of the nitrogen-vacancy center in diamond</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Löfgren, Robin; Pawar, Ravinder; Öberg, Sven; Larsson, J. Andreas</p> <p>2018-02-01</p> <p><span class="hlt">Charged</span> defects are traditionally computed by adding (subtracting) electrons for <span class="hlt">negative</span> (positive) impurities. When using periodic boundary conditions this results in artificially <span class="hlt">charged</span> supercells that also require a compensating background <span class="hlt">charge</span> of the opposite sign, which makes slab supercells problematic because of an arbitrary dependence on the vacuum thickness. In this work, we test the method of using neutral supercells through the use of a substitutional electron donor (acceptor) to describe <span class="hlt">charged</span> systems. We use density functional theory (DFT) to compare the effects of <span class="hlt">charging</span> the well-studied NV-center in diamond by a substitutional donor nitrogen. We investigate the influence of the donor-N on the NV-center properties as a function of the distance between them, and find that they converge toward those obtained when adding an electron. We analyze the spin density and conclude that the donor-N has a zero magnetic moment, and thus, will not be seen in electron spin resonance. We validate our DFT energies through comparison to GW simulations. <span class="hlt">Charging</span> the NV-center with a substitutional donor-N enables accurate calculations of slabs, without the ambiguity of using <span class="hlt">charged</span> supercells. Implantation of donor-N atoms opens up the possibility to engineer NV-centers with the desired <span class="hlt">charge</span> state for future ICT and sensor applications.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4751258','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4751258"><span>Effects of <span class="hlt">Charged</span> Particles on Human Tumor Cells</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Held, Kathryn D.; Kawamura, Hidemasa; Kaminuma, Takuya; Paz, Athena Evalour S.; Yoshida, Yukari; Liu, Qi; Willers, Henning; Takahashi, Akihisa</p> <p>2016-01-01</p> <p>The use of <span class="hlt">charged</span> particle therapy in cancer treatment is growing rapidly, in large part because the exquisite dose localization of <span class="hlt">charged</span> particles allows for higher radiation doses to be given to tumor tissue while normal tissues are exposed to lower doses and decreased volumes of normal tissues are irradiated. In <span class="hlt">addition</span>, <span class="hlt">charged</span> particles heavier than protons have substantial potential clinical advantages because of their <span class="hlt">additional</span> biological effects, including greater cell killing effectiveness, decreased radiation resistance of hypoxic cells in tumors, and reduced cell cycle dependence of radiation response. These biological advantages depend on many factors, such as endpoint, cell or tissue type, dose, dose rate or fractionation, <span class="hlt">charged</span> particle type and energy, and oxygen concentration. This review summarizes the unique biological advantages of <span class="hlt">charged</span> particle therapy and highlights recent research and areas of particular research needs, such as quantification of relative biological effectiveness (RBE) for various tumor types and radiation qualities, role of genetic background of tumor cells in determining response to <span class="hlt">charged</span> particles, sensitivity of cancer stem-like cells to <span class="hlt">charged</span> particles, role of <span class="hlt">charged</span> particles in tumors with hypoxic fractions, and importance of fractionation, including use of hypofractionation, with <span class="hlt">charged</span> particles. PMID:26904502</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26327272','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26327272"><span>DNA Immobilization and Hybridization Detection by the Intrinsic Molecular <span class="hlt">Charge</span> Using Capacitive Field-Effect Sensors Modified with a <span class="hlt">Charged</span> Weak Polyelectrolyte Layer.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Bronder, Thomas S; Poghossian, Arshak; Scheja, Sabrina; Wu, Chunsheng; Keusgen, Michael; Mewes, Dieter; Schöning, Michael J</p> <p>2015-09-16</p> <p>Miniaturized setup, compatibility with advanced micro- and nanotechnologies, and ability to detect biomolecules by their intrinsic molecular <span class="hlt">charge</span> favor the semiconductor field-effect platform as one of the most attractive approaches for the development of label-free DNA chips. In this work, a capacitive field-effect EIS (electrolyte-insulator-semiconductor) sensor covered with a layer-by-layer prepared, positively <span class="hlt">charged</span> weak polyelectrolyte layer of PAH (poly(allylamine hydrochloride)) was used for the label-free electrical detection of DNA (deoxyribonucleic acid) immobilization and hybridization. The <span class="hlt">negatively</span> <span class="hlt">charged</span> probe single-stranded DNA (ssDNA) molecules were electrostatically adsorbed onto the positively <span class="hlt">charged</span> PAH layer, resulting in a preferentially flat orientation of the ssDNA molecules within the Debye length, thus yielding a reduced <span class="hlt">charge</span>-screening effect and a higher sensor signal. Each sensor-surface modification step (PAH adsorption, probe ssDNA immobilization, hybridization with complementary target DNA (cDNA), reducing an unspecific adsorption by a blocking agent, incubation with noncomplementary DNA (ncDNA) solution) was monitored by means of capacitance-voltage and constant-capacitance measurements. In <span class="hlt">addition</span>, the surface morphology of the PAH layer was studied by atomic force microscopy and contact-angle measurements. High hybridization signals of 34 and 43 mV were recorded in low-ionic strength solutions of 10 and 1 mM, respectively. In contrast, a small signal of 4 mV was recorded in the case of unspecific adsorption of fully mismatched ncDNA. The density of probe ssDNA and dsDNA molecules as well as the hybridization efficiency was estimated using the experimentally measured DNA immobilization and hybridization signals and a simplified double-layer capacitor model. The results of field-effect experiments were supported by fluorescence measurements, verifying the DNA-immobilization and hybridization event.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhRvD..95d4002F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhRvD..95d4002F"><span>Conserved <span class="hlt">charges</span> of the extended Bondi-Metzner-Sachs algebra</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Flanagan, Éanna É.; Nichols, David A.</p> <p>2017-02-01</p> <p>Isolated objects in asymptotically flat spacetimes in general relativity are characterized by their conserved <span class="hlt">charges</span> associated with the Bondi-Metzner-Sachs (BMS) group. These <span class="hlt">charges</span> include total energy, linear momentum, intrinsic angular momentum and center-of-mass location, and, in <span class="hlt">addition</span>, an infinite number of supermomentum <span class="hlt">charges</span> associated with supertranslations. Recently, it has been suggested that the BMS symmetry algebra should be enlarged to include an infinite number of <span class="hlt">additional</span> symmetries known as super-rotations. We show that the corresponding <span class="hlt">charges</span> are finite and well defined, and can be divided into electric parity "super center-of-mass" <span class="hlt">charges</span> and magnetic parity "superspin" <span class="hlt">charges</span>. The supermomentum <span class="hlt">charges</span> are associated with ordinary gravitational-wave memory, and the super center-of-mass <span class="hlt">charges</span> are associated with total (ordinary plus null) gravitational-wave memory, in the terminology of Bieri and Garfinkle. Superspin <span class="hlt">charges</span> are associated with the ordinary piece of spin memory. Some of these <span class="hlt">charges</span> can give rise to black hole hair, as described by Strominger and Zhiboedov. We clarify how this hair evades the no-hair theorems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25641162','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25641162"><span>Molecular dynamics investigation of the ionic liquid/enzyme interface: application to engineering enzyme surface <span class="hlt">charge</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Burney, Patrick R; Nordwald, Erik M; Hickman, Katie; Kaar, Joel L; Pfaendtner, Jim</p> <p>2015-04-01</p> <p>Molecular simulations of the enzymes Candida rugosa lipase and Bos taurus α-chymotrypsin in aqueous ionic liquids 1-butyl-3-methylimidazolium chloride and 1-ethyl-3-methylimidazolium ethyl sulfate were used to study the change in enzyme-solvent interactions induced by modification of the enzyme surface <span class="hlt">charge</span>. The enzymes were altered by randomly mutating lysine surface residues to glutamate, effectively decreasing the net surface <span class="hlt">charge</span> by two for each mutation. These mutations resemble succinylation of the enzyme by chemical modification, which has been shown to enhance the stability of both enzymes in ILs. After establishing that the enzymes were stable on the simulated time scales, we focused the analysis on the organization of the ionic liquid substituents about the enzyme surface. Calculated solvent <span class="hlt">charge</span> densities show that for both enzymes and in both solvents that changing positively <span class="hlt">charged</span> residues to <span class="hlt">negative</span> <span class="hlt">charge</span> does indeed increase the <span class="hlt">charge</span> density of the solvent near the enzyme surface. The radial distribution of IL constituents with respect to the enzyme reveals decreased interactions with the anion are prevalent in the modified systems when compared to the wild type, which is largely accompanied by an increase in cation contact. <span class="hlt">Additionally</span>, the radial dependence of the <span class="hlt">charge</span> density and ion distribution indicates that the effect of altering enzyme <span class="hlt">charge</span> is confined to short range (≤1 nm) ordering of the IL. Ultimately, these results, which are consistent with that from prior experiments, provide molecular insight into the effect of enzyme surface <span class="hlt">charge</span> on enzyme stability in ILs. © 2015 Wiley Periodicals, Inc.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22408371-analytic-expression-sheath-criterion-magnetized-plasmas-multi-charged-ion-species','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22408371-analytic-expression-sheath-criterion-magnetized-plasmas-multi-charged-ion-species"><span>An analytic expression for the sheath criterion in magnetized plasmas with multi-<span class="hlt">charged</span> ion species</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Hatami, M. M., E-mail: m-hatami@kntu.ac.ir</p> <p>2015-04-15</p> <p>The generalized Bohm criterion in magnetized multi-component plasmas consisting of multi-<span class="hlt">charged</span> positive and <span class="hlt">negative</span> ion species and electrons is analytically investigated by using the hydrodynamic model. It is assumed that the electrons and <span class="hlt">negative</span> ion density distributions are the Boltzmann distribution with different temperatures and the positive ions enter into the sheath region obliquely. Our results show that the positive and <span class="hlt">negative</span> ion temperatures, the orientation of the applied magnetic field and the <span class="hlt">charge</span> number of positive and <span class="hlt">negative</span> ions strongly affect the Bohm criterion in these multi-component plasmas. To determine the validity of our derived generalized Bohm criterion, itmore » reduced to some familiar physical condition and it is shown that monotonically reduction of the positive ion density distribution leading to the sheath formation occurs only when entrance velocity of ion into the sheath satisfies the obtained Bohm criterion. Also, as a practical application of the obtained Bohm criterion, effects of the ionic temperature and concentration as well as magnetic field on the behavior of the <span class="hlt">charged</span> particle density distributions and so the sheath thickness of a magnetized plasma consisting of electrons and singly <span class="hlt">charged</span> positive and <span class="hlt">negative</span> ion species are studied numerically.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.1583D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.1583D"><span>Positive and <span class="hlt">negative</span> ion outflow at Rhea as observed by Cassini</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Desai, Ravindra; Jones, Geraint; Regoli, Leonardo; Cowee, Misa; Coates, Andrew; Kataria, Dhiren</p> <p>2017-04-01</p> <p>Rhea is Saturn's largest icy moon and hosts an ethereal oxygen and carbon-dioxide atmosphere as was detected when Cassini observed positive and <span class="hlt">negative</span> pickup ions outflowing from the moon and an extended neutral exosphere. These pickup ions can form current systems which, with the resulting jxB force, act to slow-down the incident magneto-plasma and cause field-line draping. As well as impacting the plasma interaction, the composition and density of picked up ions provide key diagnostics of the moon's sputter-induced atmosphere and surface. During the first Cassini-Rhea encounter (R1), the Cassini Plasma Spectrometer (CAPS) observed positively and <span class="hlt">negatively</span> <span class="hlt">charged</span> pickup ions before and after passing through the moon's plasma wake respectively, in agreement with their anticipated cycloidal trajectories. On the subsequent more distant wake encounter (R1.5) however, only positively <span class="hlt">charged</span> pickup ions were observed, indicating high loss rates of the <span class="hlt">negative</span> ions in Saturn's magnetosphere. Here, using an updated model of Cassini's Electron Spectrometer response function, we are able to estimate the outward flux of <span class="hlt">negatively</span> <span class="hlt">charged</span> pickup ions, the first time such a plasma population has been constrained. Using test-particle simulations we trace both the positive and <span class="hlt">negative</span> particles back to Rhea's exobase to better understand their production and loss processes and the implications for Rhea's sputter-induced exosphere. We also look to examine whether the calculated ion densities could generate ion cyclotron wave activity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016NatCo...712660J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016NatCo...712660J"><span>Optical patterning of trapped <span class="hlt">charge</span> in nitrogen-doped diamond</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jayakumar, Harishankar; Henshaw, Jacob; Dhomkar, Siddharth; Pagliero, Daniela; Laraoui, Abdelghani; Manson, Neil B.; Albu, Remus; Doherty, Marcus W.; Meriles, Carlos A.</p> <p>2016-08-01</p> <p>The nitrogen-vacancy (NV) centre in diamond is emerging as a promising platform for solid-state quantum information processing and nanoscale metrology. Of interest in these applications is the manipulation of the NV <span class="hlt">charge</span>, which can be attained by optical excitation. Here, we use two-colour optical microscopy to investigate the dynamics of NV photo-ionization, <span class="hlt">charge</span> diffusion and trapping in type-1b diamond. We combine fixed-point laser excitation and scanning fluorescence imaging to locally alter the concentration of <span class="hlt">negatively</span> <span class="hlt">charged</span> NVs, and to subsequently probe the corresponding redistribution of <span class="hlt">charge</span>. We uncover the formation of spatial patterns of trapped <span class="hlt">charge</span>, which we qualitatively reproduce via a model of the interplay between photo-excited carriers and atomic defects. Further, by using the NV as a probe, we map the relative fraction of positively <span class="hlt">charged</span> nitrogen on localized optical excitation. These observations may prove important to transporting quantum information between NVs or to developing three-dimensional, <span class="hlt">charge</span>-based memories.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27573190','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27573190"><span>Optical patterning of trapped <span class="hlt">charge</span> in nitrogen-doped diamond.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Jayakumar, Harishankar; Henshaw, Jacob; Dhomkar, Siddharth; Pagliero, Daniela; Laraoui, Abdelghani; Manson, Neil B; Albu, Remus; Doherty, Marcus W; Meriles, Carlos A</p> <p>2016-08-30</p> <p>The nitrogen-vacancy (NV) centre in diamond is emerging as a promising platform for solid-state quantum information processing and nanoscale metrology. Of interest in these applications is the manipulation of the NV <span class="hlt">charge</span>, which can be attained by optical excitation. Here, we use two-colour optical microscopy to investigate the dynamics of NV photo-ionization, <span class="hlt">charge</span> diffusion and trapping in type-1b diamond. We combine fixed-point laser excitation and scanning fluorescence imaging to locally alter the concentration of <span class="hlt">negatively</span> <span class="hlt">charged</span> NVs, and to subsequently probe the corresponding redistribution of <span class="hlt">charge</span>. We uncover the formation of spatial patterns of trapped <span class="hlt">charge</span>, which we qualitatively reproduce via a model of the interplay between photo-excited carriers and atomic defects. Further, by using the NV as a probe, we map the relative fraction of positively <span class="hlt">charged</span> nitrogen on localized optical excitation. These observations may prove important to transporting quantum information between NVs or to developing three-dimensional, <span class="hlt">charge</span>-based memories.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5013603','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5013603"><span>Optical patterning of trapped <span class="hlt">charge</span> in nitrogen-doped diamond</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Jayakumar, Harishankar; Henshaw, Jacob; Dhomkar, Siddharth; Pagliero, Daniela; Laraoui, Abdelghani; Manson, Neil B.; Albu, Remus; Doherty, Marcus W.; Meriles, Carlos A.</p> <p>2016-01-01</p> <p>The nitrogen-vacancy (NV) centre in diamond is emerging as a promising platform for solid-state quantum information processing and nanoscale metrology. Of interest in these applications is the manipulation of the NV <span class="hlt">charge</span>, which can be attained by optical excitation. Here, we use two-colour optical microscopy to investigate the dynamics of NV photo-ionization, <span class="hlt">charge</span> diffusion and trapping in type-1b diamond. We combine fixed-point laser excitation and scanning fluorescence imaging to locally alter the concentration of <span class="hlt">negatively</span> <span class="hlt">charged</span> NVs, and to subsequently probe the corresponding redistribution of <span class="hlt">charge</span>. We uncover the formation of spatial patterns of trapped <span class="hlt">charge</span>, which we qualitatively reproduce via a model of the interplay between photo-excited carriers and atomic defects. Further, by using the NV as a probe, we map the relative fraction of positively <span class="hlt">charged</span> nitrogen on localized optical excitation. These observations may prove important to transporting quantum information between NVs or to developing three-dimensional, <span class="hlt">charge</span>-based memories. PMID:27573190</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012PhDT.......358B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012PhDT.......358B"><span>The role of interfacial water layer in atmospherically relevant <span class="hlt">charge</span> separation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bhattacharyya, Indrani</p> <p></p> <p><span class="hlt">Charge</span> separation at interfaces is important in various atmospheric processes, such as thunderstorms, lightning, and sand storms. It also plays a key role in several industrial processes, including ink-jet printing and electrostatic separation. Surprisingly, little is known about the underlying physics of these <span class="hlt">charging</span> phenomena. Since thin films of water are ubiquitous, they may play a role in these <span class="hlt">charge</span> separation processes. This talk will focus on the experimental investigation of the role of a water adlayer in interfacial <span class="hlt">charging</span>, with relevance to meteorologically important phenomena, such as atmospheric <span class="hlt">charging</span> due to wave actions on oceans and sand storms. An ocean wave generates thousands of bubbles, which upon bursting produce numerous large jet droplets and small film droplets that are <span class="hlt">charged</span>. In the 1960s, Blanchard showed that the jet droplets are positively <span class="hlt">charged</span>. However, the <span class="hlt">charge</span> on the film droplets was not known. We designed an experiment to exclusively measure the <span class="hlt">charge</span> on film droplets generated by bubble bursting on pure water and aqueous salt solution surfaces. We measured their <span class="hlt">charge</span> to be <span class="hlt">negative</span> and proposed a model where a slight excess of hydroxide ions in the interfacial water layer is responsible for generating these <span class="hlt">negatively</span> <span class="hlt">charged</span> droplets. The findings from this research led to a better understanding of the ionic disposition at the air-water interface. Sand particles in a wind-blown sand layer, or 'saltation' layer, become <span class="hlt">charged</span> due to collisions, so much so, that it can cause lightning. Silica, being hydrophilic, is coated with a water layer even under low-humidity conditions. To investigate the importance of this water adlayer in <span class="hlt">charging</span> the silica surfaces, we performed experiments to measure the <span class="hlt">charge</span> on silica surfaces due to contact and collision processes. In case of contact <span class="hlt">charging</span>, the maximum <span class="hlt">charge</span> separation occurred at an optimum relative humidity. On the contrary, in collisional <span class="hlt">charging</span> process, no</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2682175','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2682175"><span>Ruminative self-focus, <span class="hlt">negative</span> life events, and <span class="hlt">negative</span> affect</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Moberly, Nicholas J.; Watkins, Edward R.</p> <p>2008-01-01</p> <p>Ruminative thinking is believed to exacerbate the psychological distress that follows stressful life events. An experience-sampling study was conducted in which participants recorded <span class="hlt">negative</span> life events, ruminative self-focus, and <span class="hlt">negative</span> affect eight times daily over one week. Occasions when participants reported a <span class="hlt">negative</span> event were marked by higher levels of <span class="hlt">negative</span> affect. <span class="hlt">Additionally</span>, <span class="hlt">negative</span> events were prospectively associated with higher levels of <span class="hlt">negative</span> affect at the next sampling occasion, and this relationship was partially mediated by momentary ruminative self-focus. Depressive symptoms were associated with more frequent <span class="hlt">negative</span> events, but not with increased reactivity to <span class="hlt">negative</span> events. Trait rumination was associated with reports of more severe <span class="hlt">negative</span> events and increased reactivity to <span class="hlt">negative</span> events. These results suggest that the extent to which a person engages in ruminative self-focus after everyday stressors is an important determinant of the degree of distress experienced after such events. Further, dispositional measures of rumination predict mood reactivity to everyday stressors in a non-clinical sample. PMID:18684437</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/921596-variable-charge-soils-mineralogy-chemistry','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/921596-variable-charge-soils-mineralogy-chemistry"><span>Variable <span class="hlt">Charge</span> Soils: Mineralogy and Chemistry</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Qafoku, Nik; Van Ranst, Eric; Noble, Andrew</p> <p>2003-11-01</p> <p>Soils rich in particles with amphoteric surface properties in the Oxisols, Ultisols, Alfisols, Spodosols and Andisols orders (1) are considered variable <span class="hlt">charge</span> soils (2). The term “variable charge” is used to describe organic and inorganic soil constituents with reactive surface groups whose <span class="hlt">charge</span> varies with pH, ionic concentration and composition of the soil solution. Such groups are the surface carboxyl, phenolic and amino functional groups of organic materials in soils, and surface hydroxyl groups of Fe and Al oxides, allophane and imogolite. The hydroxyl surface groups are also present on edges of some phyllosilicate minerals such as kaolinite, mica, andmore » hydroxyl-interlayered vermiculite. The variable <span class="hlt">charge</span> is developed on the surface groups as a result of adsorption or desorption of ions that are constituents of the solid phase, i.e., H+, and the adsorption or desorption of solid-unlike ions that are not constituents of the solid. Highly weathered soils usually undergo isoeletric weathering and reach a “zero net charge” stage during their development. They have a slightly acidic to acidic soil solution pH, which is close to either point of zero net <span class="hlt">charge</span> (PZNC) (3) or point of zero salt effect (PZSE) (3). They are characterized by high abundances of minerals with a point of zero net proton <span class="hlt">charge</span> (PZNPC) (3) at neutral and slightly basic pHs; the most important being Fe and Al oxides and allophane. Under acidic conditions, the surfaces of these minerals are net positively <span class="hlt">charged</span>. In contrast, the surfaces of permanent <span class="hlt">charge</span> phyllosilicates are <span class="hlt">negatively</span> <span class="hlt">charged</span> regardless of ambient conditions. Variable <span class="hlt">charge</span> soils therefore, are heterogeneous <span class="hlt">charge</span> systems. The coexistence and interactions of oppositely <span class="hlt">charged</span> surfaces or particles confers a different pattern of physical and chemical behavior on the soil, relatively to a homogeneously <span class="hlt">charged</span> system of temperate regions. In some variable <span class="hlt">charge</span> soils (Oxisols and some Ultisols</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21639994','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21639994"><span>Combinatorial effects of <span class="hlt">charge</span> characteristics and hydrophobicity of silk fibroin on the sorption and release of <span class="hlt">charged</span> dyes.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wongpanit, Panya; Rujiravanit, Ratana</p> <p>2012-01-01</p> <p>The present study was designed to examine the influence of the <span class="hlt">charge</span> characteristics of silk fibroin on the sorption and release of <span class="hlt">charged</span> dyes by varying the pH values of the sorption and release media as well as types of <span class="hlt">charged</span> dyes. <span class="hlt">Negatively</span> <span class="hlt">charged</span> dyes (phenol red and chromotrope 2R) and positively <span class="hlt">charged</span> dyes (crystal violet and indoine blue) were used as the model compounds. Silk fibroin films were prepared by using a solution casting technique. The prepared films were then treated with an aqueous methanol solution or annealed with water to control their conformation. The sorption behavior of the model compounds made by the methanol-treated and water-annealed silk fibroin films was investigated. Compared to the water- annealed silk fibroin films, a higher hydrophobicity of the methanol-treated silk fibroin films caused a higher sorption of the hydrophobic dyes. The dye molecules had a fairly high affinity to the silk fibroin film, even though the dye and the matrix possessed the same <span class="hlt">charge</span>. However, in the presence of two <span class="hlt">charged</span> groups in a single dye molecule, the electrostatic repulsion become more dominant. Stronger interaction was observed when the <span class="hlt">charges</span> of the film and the dye were opposite. The results of dye sorption and release experiments showed that the degree of synergism or competition between electrostatic and hydrophobic interactions directly depended on the <span class="hlt">charges</span> and chemical structure of the dye molecules and the environmental pH conditions of the existing silk fibroin film.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21278462','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21278462"><span>Influence of natural organic matter on equilibrium adsorption of neutral and <span class="hlt">charged</span> pharmaceuticals onto activated carbon.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>de Ridder, D J; Verliefde, A R D; Heijman, S G J; Verberk, J Q J C; Rietveld, L C; van der Aa, L T J; Amy, G L; van Dijk, J C</p> <p>2011-01-01</p> <p>Natural organic matter (NOM) can influence pharmaceutical adsorption onto granular activated carbon (GAC) by direct adsorption competition and pore blocking. However, in the literature there is limited information on which of these mechanisms is more important and how this is related to NOM and pharmaceutical properties. Adsorption batch experiments were carried out in ultrapure, waste- and surface water and fresh and NOM preloaded GAC was used. Twenty-one pharmaceuticals were selected with varying hydrophobicity and with neutral, <span class="hlt">negative</span> or positive <span class="hlt">charge</span>. The influence of NOM competition and pore blocking could not be separated. However, while reduction in surface area was similar for both preloaded GACs, up to 50% lower pharmaceutical removal was observed on wastewater preloaded GAC. This was attributed to higher hydrophobicity of wastewater NOM, indicating that NOM competition may influence pharmaceutical removal more than pore blocking. Preloaded GAC was <span class="hlt">negatively</span> <span class="hlt">charged</span>, which influenced removal of <span class="hlt">charged</span> pharmaceuticals significantly. At a GAC dose of 6.7 mg/L, <span class="hlt">negatively</span> <span class="hlt">charged</span> pharmaceuticals were removed for 0-58%, while removal of positively <span class="hlt">charged</span> pharmaceuticals was between 32-98%. <span class="hlt">Charge</span> effects were more pronounced in ultrapure water, as it contained no ions to shield the surface <span class="hlt">charge</span>. Solutes with higher log D could compete better with NOM, resulting in higher removal.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24463476','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24463476"><span>Effects of different blasting materials on <span class="hlt">charge</span> generation and decay on titanium surface after sandblasting.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Guo, Cecilia Yan; Hong Tang, Alexander Tin; Hon Tsoi, James Kit; Matinlinna, Jukka Pekka</p> <p>2014-04-01</p> <p>It has been reported that sandblasting titanium with alumina (Al2O3) powder could generate a <span class="hlt">negative</span> electric <span class="hlt">charge</span> on titanium surface. This has been proven to promote osteoblast activities and possibly osseointegration. The purpose of this pilot study was to investigate the effects of different blasting materials, in terms of the grit sizes and electro-<span class="hlt">negativity</span>, on the generation of a <span class="hlt">negative</span> <span class="hlt">charge</span> on the titanium surface. The aim was also to make use of these results to deduct the underlying mechanism of <span class="hlt">charge</span> generation by sandblasting. Together 60 c.p. 2 titanium plates were machine-cut and polished for sandblasting, and divided into 6 groups with 10 plates in each. Every plate in the study groups was sandblasted with one of the following 6 powder materials: 110µm Al2O3 grits, 50µm Al2O3 grits, 150-300µm glass beads, 45-75µm glass beads, 250µm Al powder and 44µm Al powder. The static voltage on the surface of every titanium plate was measured immediately after sandblasting. The static voltages of the titanium plates were recorded and processed using statistical analysis. The results suggested that only sandblasting with 45-75µm glass beads generated a positive <span class="hlt">charge</span> on titanium, while using all other blasting materials lead to a <span class="hlt">negative</span> <span class="hlt">charge</span>. Furthermore, blasting grits of the same powder material but of different sizes might lead to different amount and polarity of the <span class="hlt">charges</span>. This triboelectric effect is likely to be the main mechanism for <span class="hlt">charge</span> generation through sandblasting. Copyright © 2014 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=47481&Lab=ORD&keyword=corona&actType=&TIMSType=+&TIMSSubTypeID=&DEID=&epaNumber=&ntisID=&archiveStatus=Both&ombCat=Any&dateBeginCreated=&dateEndCreated=&dateBeginPublishedPresented=&dateEndPublishedPresented=&dateBeginUpdated=&dateEndUpdated=&dateBeginCompleted=&dateEndCompleted=&personID=&role=Any&journalID=&publisherID=&sortBy=revisionDate&count=50','EPA-EIMS'); return false;" href="https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=47481&Lab=ORD&keyword=corona&actType=&TIMSType=+&TIMSSubTypeID=&DEID=&epaNumber=&ntisID=&archiveStatus=Both&ombCat=Any&dateBeginCreated=&dateEndCreated=&dateBeginPublishedPresented=&dateEndPublishedPresented=&dateBeginUpdated=&dateEndUpdated=&dateBeginCompleted=&dateEndCompleted=&personID=&role=Any&journalID=&publisherID=&sortBy=revisionDate&count=50"><span><span class="hlt">CHARGE</span> MEASUREMENTS OF PARTICLES EXITING ELECTROSTATIC PRECIPITATORS</span></a></p> <p><a target="_blank" href="http://oaspub.epa.gov/eims/query.page">EPA Science Inventory</a></p> <p></p> <p></p> <p>The report gives results of an investigation of particle <span class="hlt">charging</span> in positive and <span class="hlt">negative</span> corona discharge as a function of temperature from 38 to 343C in order to establish, especially at hot-side electrostatic precipitator (ESP) temperatures, the relative effectiveness of the ...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003JPS...117..260R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003JPS...117..260R"><span>Correlation between <span class="hlt">charge</span> input and cycle life of MgNi electrode for Ni-MH batteries</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ruggeri, Stéphane; Roué, Lionel</p> <p></p> <p>Amorphous MgNi material has been prepared by mechanically alloying magnesium and nickel powders for 10 h. Its cycle life as a <span class="hlt">negative</span> electrode for nickel-metal hydride (Ni-MH) batteries has been studied with <span class="hlt">charge</span> inputs varying from 0 to 600 mAh/g. For <span class="hlt">charge</span> inputs lower than 400 mAh/g, the first cycle discharge capacity is superior to the <span class="hlt">charge</span> input capacity. This surplus discharge capacity can be associated with the alloy oxidation to Mg(OH) 2 and Ni(OH) 2. For <span class="hlt">charge</span> inputs higher than 400 mAh/g, the initial discharge capacity becomes inferior to the <span class="hlt">charge</span> input capacity due to the progressive decrease of the <span class="hlt">charge</span> efficiency related to the hydrogen evolution side reaction. From the second <span class="hlt">charge</span>/discharge cycle, no <span class="hlt">additional</span> discharge capacity appears and no discharge capacity degradation occurs for <span class="hlt">charge</span> inputs inferior or equal to 233 mAh/g. In contrast, for higher <span class="hlt">charge</span> input values, an important decay in the discharge capacity appears, which is accentuated with increasing <span class="hlt">charge</span> input. The thresholds <span class="hlt">charge</span> input of 233 mAh/g corresponds to an amount of hydrogen absorbed into the alloy of 0.8 wt.% (MgNiH 0.7). For higher absorbed hydrogen amounts, it is assumed that extended electrode pulverization occurs, which breaks the passive surface layer of Mg(OH) 2 formed during the first <span class="hlt">charge</span>/discharge cycle. This creates unprotected fresh MgNi surfaces and consequently, leads to electrode capacity degradation. The stability of the MgNi electrode for absorbed hydrogen content lower than 0.8 wt.% may be related to its amorphous character, which favors a gradual volume expansion upon hydrogen absorption in contrast to crystalline compounds characterized by an abrupt α-to-β lattice expansion.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li class="active"><span>16</span></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_16 --> <div id="page_17" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li class="active"><span>17</span></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="321"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25051121','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25051121"><span>Analysis of microscopic parameters of surface <span class="hlt">charging</span> in polymer caused by defocused electron beam irradiation.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Liu, Jing; Zhang, Hai-Bo</p> <p>2014-12-01</p> <p>The relationship between microscopic parameters and polymer <span class="hlt">charging</span> caused by defocused electron beam irradiation is investigated using a dynamic scattering-transport model. The dynamic <span class="hlt">charging</span> process of an irradiated polymer using a defocused 30 keV electron beam is conducted. In this study, the space <span class="hlt">charge</span> distribution with a 30 keV non-penetrating e-beam is <span class="hlt">negative</span> and supported by some existing experimental data. The internal potential is <span class="hlt">negative</span>, but relatively high near the surface, and it decreases to a maximum <span class="hlt">negative</span> value at z=6 μm and finally tend to 0 at the bottom of film. The leakage current and the surface potential behave similarly, and the secondary electron and leakage currents follow the <span class="hlt">charging</span> equilibrium condition. The surface potential decreases with increasing beam current density, trap concentration, capture cross section, film thickness and electron-hole recombination rate, but with decreasing electron mobility and electron energy. The total <span class="hlt">charge</span> density increases with increasing beam current density, trap concentration, capture cross section, film thickness and electron-hole recombination rate, but with decreasing electron mobility and electron energy. This study shows a comprehensive analysis of microscopic factors of surface <span class="hlt">charging</span> characteristics in an electron-based surface microscopy and analysis. Copyright © 2014 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19800062721&hterms=laboratory+Roche&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dlaboratory%2BRoche','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19800062721&hterms=laboratory+Roche&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dlaboratory%2BRoche"><span>A three-dimensional spacecraft-<span class="hlt">charging</span> computer code</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Rubin, A. G.; Katz, I.; Mandell, M.; Schnuelle, G.; Steen, P.; Parks, D.; Cassidy, J.; Roche, J.</p> <p>1980-01-01</p> <p>A computer code is described which simulates the interaction of the space environment with a satellite at geosynchronous altitude. Employing finite elements, a three-dimensional satellite model has been constructed with more than 1000 surface cells and 15 different surface materials. Free space around the satellite is modeled by nesting grids within grids. Applications of this NASA Spacecraft <span class="hlt">Charging</span> Analyzer Program (NASCAP) code to the study of a satellite photosheath and the differential <span class="hlt">charging</span> of the SCATHA (satellite <span class="hlt">charging</span> at high altitudes) satellite in eclipse and in sunlight are discussed. In order to understand detector response when the satellite is <span class="hlt">charged</span>, the code is used to trace the trajectories of particles reaching the SCATHA detectors. Particle trajectories from positive and <span class="hlt">negative</span> emitters on SCATHA also are traced to determine the location of returning particles, to estimate the escaping flux, and to simulate active control of satellite potentials.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140006451','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140006451"><span>DMSP Auroral <span class="hlt">Charging</span> at Solar Cycle 24 Maximum</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Chandler, M.; Parker, L. Neergaard; Minow, J. I.</p> <p>2013-01-01</p> <p>It has been well established that polar orbiting satellites can experience mild to severe auroral <span class="hlt">charging</span> levels (on the order of a few hundred volts to few kilovolts <span class="hlt">negative</span> frame potentials) during solar minimum conditions. These same studies have shown a strong reduction in <span class="hlt">charging</span> during the rising and declining phases of the past few solar cycles with a nearly complete suppression of auroral <span class="hlt">charging</span> at solar maximum. Recently, we have observed examples of high level <span class="hlt">charging</span> during the recent approach to Solar Cycle 24 solar maximum conditions not unlike those reported by Frooninckx and Sojka. These observations demonstrate that spacecraft operations during solar maximum cannot be considered safe from auroral <span class="hlt">charging</span> when solar activity is low. We present a survey of auroral <span class="hlt">charging</span> events experienced by the Defense Meteorological Satellite Program (DMSP) F16 satellite during Solar Cycle 24 maximum conditions. We summarize the auroral energetic particle environment and the conditions necessary for <span class="hlt">charging</span> to occur in this environment, we describe how the lower than normal solar activity levels for Solar Cycle 24 maximum conditions are conducive to <span class="hlt">charging</span> in polar orbits, and we show examples of the more extreme <span class="hlt">charging</span> events, sometimes exceeding 1 kV, during this time period.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140006417','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140006417"><span>DMSP Auroral <span class="hlt">Charging</span> at Solar Cycle 24 Maximum</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Chandler, Michael; Parker, Linda Neergaard; Minow, Joseph I.</p> <p>2013-01-01</p> <p>It has been well established that polar orbiting satellites can experience mild to severe auroral <span class="hlt">charging</span> levels (on the order of a few hundred volts to few kilovolts <span class="hlt">negative</span> frame potentials) during solar minimum conditions (Frooninckx and Sojka, 1992; Anderson and Koons, 1996; Anderson, 2012). These same studies have shown a strong reduction in <span class="hlt">charging</span> during the rising and declining phases of the past few solar cycles with a nearly complete suppression of auroral <span class="hlt">charging</span> at solar maximum. Recently, we have observed examples of high level <span class="hlt">charging</span> during the recent approach to Solar Cycle 24 solar maximum conditions not unlike those reported by Frooninckx and Sojka (1992). These observations demonstrate that spacecraft operations during solar maximum cannot be considered safe from auroral <span class="hlt">charging</span> when solar activity is low. We present a survey of auroral <span class="hlt">charging</span> events experienced by the Defense Meteorological Satellite Program (DMSP) F16 satellite during Solar Cycle 24 maximum conditions. We summarize the auroral energetic particle environment and the conditions necessary for <span class="hlt">charging</span> to occur in this environment, we describe how the lower than normal solar activity levels for Solar Cycle 24 maximum conditions are conducive to <span class="hlt">charging</span> in polar orbits, and we show examples of the more extreme <span class="hlt">charging</span> events, sometimes exceeding 1 kV, during this time period.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18363694','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18363694"><span>Concurrent application of <span class="hlt">charge</span> using a novel circuit prevents heat-related coagulum formation during radiofrequency ablation.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lim, Bernard; Venkatachalam, Kalpathi L; Jahangir, Arshad; Johnson, Susan B; Asirvatham, Samuel J</p> <p>2008-08-01</p> <p>Thromboembolism resulting from coagulum formation on the catheter and electrode surfaces is a serious complication with radiofrequency ablation procedures for heart rhythm disorders. Why coagulum occurs despite therapeutic heparinization is unclear. In this report, we demonstrate a novel approach to minimize coagulum formation based on the electromolecular characteristics of fibrinogen. Atomic force microscopy was used to establish that fibrinogen deposited on surfaces underwent conformational changes that resulted in spontaneous clot formation. We then immersed ablation catheters that were uncharged, <span class="hlt">negatively</span>, or positively <span class="hlt">charged</span> in heparinized blood for 30 minutes and noted the extent of clot formation. In separate experiments, ablation catheters were sutured to the ventricle of an excised porcine heart immersed in whole, heparinized blood and radiofrequency ablation performed for 5 minutes with and without <span class="hlt">charge</span> delivered to the catheter tips. Electron microscopy of the catheter tips showed surface coverage of fibrin clot of the catheter to be 33.8% for <span class="hlt">negatively</span> <span class="hlt">charged</span> catheters, compared with 84.7% (P = 0.01) in noncharged catheters. There was no significant difference in surface coverage of fibrin clot between positively <span class="hlt">charged</span> catheters (93.8%) and noncharged catheters (84.7%, P = ns). In contrast, the thickness of surface clot coverage for positively <span class="hlt">charged</span> catheters was 87.5%, compared with 28.45% (P= 0.03) for noncharged catheters and 11.25% (P = 0.03) for <span class="hlt">negatively</span> <span class="hlt">charged</span> catheters, compared with noncharged catheters. We describe a novel method of placing <span class="hlt">negative</span> <span class="hlt">charge</span> on electrodes during ablation that reduced coagulum formation. This may decrease thromboembolism-related complications with radiofrequency ablation procedures.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/524601-characteristics-space-charge-formed-laminated-ldpe-eva-dielectric-under-dc-stress','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/524601-characteristics-space-charge-formed-laminated-ldpe-eva-dielectric-under-dc-stress"><span>Characteristics of space <span class="hlt">charge</span> formed in a laminated LDPE/EVA dielectric under DC stress</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Tanaka, Toshikatsu; Kisanuki, Osamu; Sakata, Masataka</p> <p>1996-12-31</p> <p>A laser-induced pressure pulse (LIPP) method was used for measuring the space <span class="hlt">charge</span> distribution of LDPE/EVA laminate dielectrics under dc stress. The constant voltage up to {+-}20 kV was applied to a side of the laminates of 0.5 mm thickness for 30 minutes. The other side is grounded. When the amount of space <span class="hlt">charge</span> was measured by LIPP, both sides were virtually grounded. Space <span class="hlt">charge</span> built up in or near the interface between LDPE and EVA was mainly investigated. Positive and <span class="hlt">negative</span> voltage was applied to the side of LDPE in the laminates. It was clarified that the space chargemore » was larger in case of LDPE <span class="hlt">negatively</span> biased than in case of LDPE positively biased. The density of the space <span class="hlt">charge</span> ranged around 1 nC/mm{sup 3}. The formation of interfacial space <span class="hlt">charge</span> is analyzed.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..MARH23003S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..MARH23003S"><span>The observation of <span class="hlt">negative</span> permittivity in stripe and bubble phases</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Smet, Jurgen</p> <p></p> <p>The physics of itinerant two-dimensional electrons is by and large governed by repulsive Coulomb forces. However, cases exist where the interplay of attractive and repulsive interaction components may instigate spontaneous symmetry lowering and clustering of <span class="hlt">charges</span> in geometric patterns such as bubbles and stripes, provided these interactions act on different length scales. The existence of these phases in higher Landau levels has so far been concluded from transport behavior. Here, we report surface acoustic wave experiments. They probe the permittivity at small wave vector. This technique offers true directionality, whereas in transport the current distribution is complex and strongly affected by the inhomogeneous density pattern. Outside the <span class="hlt">charge</span> density wave regime, the measured permittivity is always positive. However, <span class="hlt">negative</span> permittivity is observed in the bubble phase irrespective of the propagation direction. For the stripe phase the permittivity takes on both positive as well as <span class="hlt">negative</span> values depending on the propagation direction. This confirms the stripe phase to be a strongly anisotropic medium. The observation of <span class="hlt">negative</span> permittivity is considered an immediate consequence of the exchange related attractive interaction. It makes <span class="hlt">charge</span> clustering favorable in higher Landau levels where the repulsive direct Coulomb interaction acts on a longer length scale and is responsible for a <span class="hlt">negative</span> compressibility of the electronic system. This work has been carried out with B. Friess, K. von Klitzing (MPI-FKF), Y. Peng, F. von Oppen (FU Berlin), B. Rosenow (Uni Leipzig) and V. Umansky (Weizmann Institute of Science).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JPhD...51p5301L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JPhD...51p5301L"><span>A Monte Carlo modeling on <span class="hlt">charging</span> effect for structures with arbitrary geometries</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, C.; Mao, S. F.; Zou, Y. B.; Li, Yong Gang; Zhang, P.; Li, H. M.; Ding, Z. J.</p> <p>2018-04-01</p> <p>Insulating materials usually suffer <span class="hlt">charging</span> effects when irradiated by <span class="hlt">charged</span> particles. In this paper, we present a Monte Carlo study on the <span class="hlt">charging</span> effect caused by electron beam irradiation for sample structures with any complex geometry. When transporting in an insulating solid, electrons encounter elastic and inelastic scattering events; the Mott cross section and a Lorentz-type dielectric function are respectively employed to describe such scatterings. In <span class="hlt">addition</span>, the band gap and the electron–long optical phonon interaction are taken into account. The electronic excitation in inelastic scattering causes generation of electron–hole pairs; these <span class="hlt">negative</span> and positive <span class="hlt">charges</span> establish an inner electric field, which in turn induces the drift of <span class="hlt">charges</span> to be trapped by impurities, defects, vacancies etc in the solid, where the distributions of trapping sites are assumed to have uniform density. Under <span class="hlt">charging</span> conditions, the inner electric field distorts electron trajectories, and the surface electric potential dynamically alters secondary electron emission. We present, in this work, an iterative modeling method for a self-consistent calculation of electric potential; the method has advantages in treating any structure with arbitrary complex geometry, in comparison with the image <span class="hlt">charge</span> method—which is limited to a quite simple boundary geometry. Our modeling is based on: the combination of the finite triangle mesh method for an arbitrary geometry construction; a self-consistent method for the spatial potential calculation; and a full dynamic description for the motion of deposited <span class="hlt">charges</span>. Example calculations have been done to simulate secondary electron yield of SiO2 for a semi-infinite solid, the <span class="hlt">charging</span> for a heterostructure of SiO2 film grown on an Au substrate, and SEM imaging of a SiO2 line structure with rough surfaces and SiO2 nanoparticles with irregular shapes. The simulations have explored interesting interlaced <span class="hlt">charge</span> layer distribution</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JPhCS1013a2108F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JPhCS1013a2108F"><span>How to build institutionalization on students: a pilot experiment on a didactical design of <span class="hlt">addition</span> and subtraction involving <span class="hlt">negative</span> integers</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fuadiah, N. F.; Suryadi, D.; Turmudi</p> <p>2018-05-01</p> <p>This study focuses on the design of a didactical situation in <span class="hlt">addition</span> and subtraction involving <span class="hlt">negative</span> integers at the pilot experiment phase. As we know, <span class="hlt">negative</span> numbers become an obstacle for students in solving problems related to them. This study aims to create a didactical design that can assist students in understanding the <span class="hlt">addition</span> and subtraction. Another expected result in this way is that students are introduced to the characteristics of <span class="hlt">addition</span> and subtraction of integers. The design was implemented on 32 seventh grade students in one of the classes in a junior secondary school as the pilot experiment. Learning activities were observed thoroughly including the students’ responses that emerged during the learning activities. The written documentation of the students was also used to support the analysis in the learning activities. The results of the analysis showed that this method could help the students perform a large number of integer operations that could not be done with a number line. The teacher’s support as a didactical potential contract was still needed to encourage institutionalization processes. The results of the design analysis used as the basis of the revision are expected to be implemented by the teacher in the teaching experiment.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20150002526','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20150002526"><span>Spacecraft <span class="hlt">Charging</span> in Geostationary Transfer Orbit</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Parker, Linda Neergaard; Minow, Joseph I.</p> <p>2014-01-01</p> <p>The 700 km x 5.8 Re orbit of the two Van Allen Probes spacecraft provide a unique opportunity to investigate spacecraft <span class="hlt">charging</span> in geostationary transfer orbits. We use records from the Helium Oxygen Proton Electron (HOPE) plasma spectrometer to identify candidate surface <span class="hlt">charging</span> events based on the "ion line" <span class="hlt">charging</span> signature in the ion records. We summarize the energetic particle environment and the conditions necessary for <span class="hlt">charging</span> to occur in this environment. We discuss the altitude, duration, and magnitude of events observed in the Van Allen Probes from the beginning of the mission to present time. In <span class="hlt">addition</span>, we explore what information the dual satellites provide on the spatial and temporal variations in the <span class="hlt">charging</span> environments.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26640083','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26640083"><span><span class="hlt">Charge</span> Master: Friend or Foe?</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wan, Wenshuai; Itri, Jason</p> <p>2016-01-01</p> <p>Prices <span class="hlt">charged</span> for imaging services can be found in the <span class="hlt">charge</span> master, a catalog of retail list prices for medical goods and services. This article reviews the evolution of reimbursement in the United States and provides a balanced discussion of the factors that influence <span class="hlt">charge</span> master prices. Reduced payments to hospitals have pressured hospitals to generate <span class="hlt">additional</span> revenue by increasing <span class="hlt">charge</span> master prices. An unfortunate consequence is that those least able to pay for health care, the uninsured, are subjected to the highest <span class="hlt">charges</span>. Yet, differences in pricing also represent an opportunity for radiology practices, which provide imaging services that are larger in scope or superior in quality to promote product differentiation. Physicians, hospital executives, and policy makers need to work together to improve the existing reimbursement system to promote high-quality, low-cost imaging. Copyright © 2016 Mosby, Inc. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19810023727','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19810023727"><span>Two-dimensiosnal electron beam <span class="hlt">charging</span> model for polymer films. M.S. Thesis; [spacecraft <span class="hlt">charging</span>, geosynchronous satellites</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Reeves, R. D.; Balmain, K. G.</p> <p>1981-01-01</p> <p>A two dimensional model was developed to describe the <span class="hlt">charging</span> of thin polymer films exposed to a uniform mon-energetic electron beam. The study was motivated by observed anomalous behavior of geosynchronous satellites which was attributed to electrical discharges associated with the differential <span class="hlt">charging</span> of satellite surfaces of magnetospheric electrons. Electric fields both internal and external to the irradiated specimen were calculated at steady state in order to identify regions of high electrical stress. Particular emphasis was placed on evaluating the <span class="hlt">charging</span> characteristics near the material's edge. The model was used to identify and quantify the effects of some of the experimental parameters notably: beam energy; beam angle of incidence; beam current density; material thickness; and material width. Simulations of the following situations were also conducted: positive or <span class="hlt">negative</span> precharging over part of the surface; a central gap in the material; and a discontinuity in the material's thickness.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18423766','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18423766"><span>Increase of the pharmacological and pharmacokinetic efficacy of <span class="hlt">negatively</span> <span class="hlt">charged</span> polypeptide recombinant hirudin in rats via parenteral route by association with cationic liposomes.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Meng, Meng; Liu, Yu; Wang, Yi-Bo; Wang, Jian-Cheng; Zhang, Hua; Wang, Xue-Qing; Zhang, Xuan; Lu, Wan-Liang; Zhang, Qiang</p> <p>2008-06-04</p> <p>Two biodegradable cationic lipids, stearylamine and DC-Chol, were chosen to investigate the effect of cationic lipids on the in vitro and in vivo characteristics of hydrophilic proteins or peptides of low isoelectric point. Thrombin inhibitor recombinant hirudin variant-2 (rHV2) was selected as the model drug. The cationic lipids were found to achieve higher entrapment efficiency of rHV2 in liposomes than zwitterionic lipids. The positively <span class="hlt">charged</span> liposomes became less positive and relatively stable in serum after loading rHV2. The cationic liposomes induced sustained release of rHV2 in the presence of plasma, significantly prolonged the antithrombotic efficacy and plasma level of rHV2 after intravenous injection in rats in comparison with neutral lipid liposomes, especially for stearylamine group. Both clotting times correlated well with plasma rHV2 levels. No serious adverse events were observed and physical state of rats was satisfactory for all the formulations. Electrostatic interaction between <span class="hlt">negative</span> <span class="hlt">charge</span> of rHV2 and cationic liposomes was confirmed and it might affect all the characteristics of rHV2 loaded cationic vehicles. The findings suggest that cationic liposomes may be a potential sustained-release delivery system for parenteral administration of hydrophilic proteins or peptides with low isoelectric point to prolong efficacy and improve bioavailability.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007PhPl...14b4502K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007PhPl...14b4502K"><span>Role of electron temperature on <span class="hlt">charging</span> of dust grains</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kausik, S. S.; Chakraborty, M.; Saikia, B. K.</p> <p>2007-02-01</p> <p>Dust grains are produced by evaporation of silver in an experimental setup consisting of a dust chamber, a plasma chamber, and a deflection chamber. Due to differential pressure between the dust and plasma chambers, the dust grains move upward and after passing through plasma they become <span class="hlt">negatively</span> <span class="hlt">charged</span>. These <span class="hlt">charged</span> dust grains are then deflected by a dc field applied across a pair of deflector plates in the deflection chamber. Both from the amount of deflection and also from the floating potential, the number of <span class="hlt">charges</span> collected on the dust grains is calculated. As the gas pressure is changed, the plasma density and the electron temperature changes. Dust <span class="hlt">charge</span> is then calculated at each value of pressure from the deflection and floating potential. It is found that the electron temperature has a profound effect in the accumulation of <span class="hlt">charge</span> on dust grains.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1997JAP....82..845J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1997JAP....82..845J"><span>Space <span class="hlt">charge</span> effects on the current-voltage characteristics of gated field emitter arrays</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jensen, K. L.; Kodis, M. A.; Murphy, R. A.; Zaidman, E. G.</p> <p>1997-07-01</p> <p>Microfabricated field emitter arrays (FEAs) can provide the very high electron current densities required for rf amplifier applications, typically on the order of 100 A/cm2. Determining the dependence of emission current on gate voltage is important for the prediction of emitter performance for device applications. Field emitters use high applied fields to extract current, and therefore, unlike thermionic emitters, the current densities can exceed 103A/cm2 when averaged over an array. At such high current densities, space <span class="hlt">charge</span> effects (i.e., the influence of <span class="hlt">charge</span> between cathode and collector on emission) affect the emission process or initiate conditions which can lead to failure mechanisms for field emitters. A simple model of a field emitter will be used to calculate the one-dimensional space <span class="hlt">charge</span> effects on the emission characteristics by examining two components: <span class="hlt">charge</span> between the gate and anode, which leads to Child's law, and <span class="hlt">charge</span> within the FEA unit cell, which gives rise to a field suppression effect which can exist for a single field emitter. The predictions of the analytical model are compared with recent experimental measurements designed to assess space <span class="hlt">charge</span> effects and predict the onset of gate current. It is shown that <span class="hlt">negative</span> convexity on a Fowler-Nordheim plot of Ianode(Vgate) data can be explained in terms of field depression at the emitter tip in <span class="hlt">addition</span> to reflection of electrons by a virtual cathode created when the anode field is insufficient to extract all of the current; in particular, the effects present within the unit cell constitute a newly described effect.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015P%26SS..119..208M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015P%26SS..119..208M"><span>Modeling the total dust production of Enceladus from stochastic <span class="hlt">charge</span> equilibrium and simulations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Meier, Patrick; Motschmann, Uwe; Schmidt, Jürgen; Spahn, Frank; Hill, Thomas W.; Dong, Yaxue; Jones, Geraint H.; Kriegel, Hendrik</p> <p>2015-12-01</p> <p><span class="hlt">Negatively</span> and positively <span class="hlt">charged</span> nano-sized ice grains were detected in the Enceladus plume by the Cassini Plasma Spectrometer (CAPS). However, no data for uncharged grains, and thus for the total amount of dust, are available. In this paper we estimate this population of uncharged grains based on a model of stochastic <span class="hlt">charging</span> in thermodynamic equilibrium and on the assumption of quasi-neutrality in the plasma-dust system. This estimation is improved upon by combining simulations of the dust component of the plume and simulations for the plasma environment into one self-consistent model. Calibration of this model with CAPS data provides a total dust production rate of about 12 kg s-1, including larger dust grains up to a few microns in size. We find that the fraction of <span class="hlt">charged</span> grains dominates over that of the uncharged grains. Moreover, our model reproduces densities of both <span class="hlt">negatively</span> and positively <span class="hlt">charged</span> nanograins measured by Cassini CAPS. In Enceladus' plume ion densities up to ~104cm-3 are required by the self-consistent model, resulting in an electron depletion of about 50% in the plasma, because electrons are attached to the <span class="hlt">negatively</span> <span class="hlt">charged</span> nanograins. These ion densities correspond to effective ionization rates of about 10-7s-1, which are about two orders of magnitude higher than expected.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1340890-variable-charge-soils-mineralogy-chemistry','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1340890-variable-charge-soils-mineralogy-chemistry"><span>VARIABLE <span class="hlt">CHARGE</span> SOILS: MINERALOGY AND CHEMISTRY</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Van Ranst, Eric; Qafoku, Nikolla; Noble, Andrew</p> <p>2016-09-19</p> <p>Soils rich in particles with amphoteric surface properties in the Oxisols, Ultisols, Alfisols, Spodosols and Andisols orders (1) are considered to be variable <span class="hlt">charge</span> soils (2) (Table 1). The term “variable charge” is used to describe organic and inorganic soil constituents with reactive surface groups whose <span class="hlt">charge</span> varies with pH and ionic concentration and composition of the soil solution. Such groups are the surface carboxyl, phenolic and amino functional groups of organic materials in soils, and surface hydroxyl groups of Fe and Al oxides, allophane and imogolite. The hydroxyl surface groups are also present on edges of some phyllosilicate mineralsmore » such as kaolinite, mica, and hydroxyl-interlayered vermiculite. The variable <span class="hlt">charge</span> is developed on the surface groups as a result of adsorption or desorption of ions that are constituents of the solid phase, i.e., H+, and the adsorption or desorption of solid-unlike ions that are not constituents of the solid phase. Highly weathered soils and subsoils (e.g., Oxisols and some Ultisols, Alfisols and Andisols) may undergo isoelectric weathering and reach a “zero net charge” stage during their development. They usually have a slightly acidic to acidic soil solution pH, which is close to either the point of zero net <span class="hlt">charge</span> (PZNC) (3) or the point of zero salt effect (PZSE) (3). They are characterized by high abundances of minerals with a point of zero net proton <span class="hlt">charge</span> (PZNPC) (3) at neutral and slightly basic pHs; the most important being Fe and Al oxides and allophane. Under acidic conditions, the surfaces of these minerals are net positively <span class="hlt">charged</span>. In contrast, the surfaces of permanent <span class="hlt">charge</span> phyllosilicates are <span class="hlt">negatively</span> <span class="hlt">charged</span> regardless of ambient conditions. Variable <span class="hlt">charge</span> soils therefore, are heterogeneous <span class="hlt">charge</span> systems.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018InPhT..89...41W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018InPhT..89...41W"><span>Modeling of frequency-dependent <span class="hlt">negative</span> differential capacitance in InGaAs/InP photodiode</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, Yidong; Chen, Jun; Xu, Jintong; Li, Xiangyang</p> <p>2018-03-01</p> <p>The <span class="hlt">negative</span> differential capacitance (NDC) of p-i-n InGaAs/InP photodetector has been clearly observed, and the small signal model of frequency-dependent NDC is established, based on the accumulation and emission of electrons at the p-InP/i-InGaAs interface. The NDC phenomenon is contributed by the <span class="hlt">additional</span> capacitance (CT), which is caused by the <span class="hlt">charging</span>-discharging process in the p-InP/i-InGaAs interface. It is found that the NDC becomes more obvious with decreasing frequency, which is consistent with the conclusion of the experiment. It is proved that the probability of electron capture/escape in the p-i interface is affected by frequency. Therefore, the smaller frequency applied, the higher <span class="hlt">additional</span> capacitance is obtained.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20500092','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20500092"><span>Electrostatic <span class="hlt">charge</span> characteristics of jet nebulized aerosols.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kwok, Philip Chi Lip; Trietsch, Sebastiaan J; Kumon, Michiko; Chan, Hak-Kim</p> <p>2010-06-01</p> <p>Liquid droplets can be spontaneously <span class="hlt">charged</span> in the absence of applied electric fields by spraying. It has been shown by computational simulation that <span class="hlt">charges</span> may influence particle deposition in the airways. The electrostatic properties of jet nebulized aerosols and their potential effects on lung deposition have hardly been studied. A modified electrical low pressure impactor (ELPI) was employed to characterize the aerosol <span class="hlt">charges</span> generated from jet nebulized commercial products. The <span class="hlt">charge</span> and size measurements were conducted at 50% RH and 22 degrees C with a modified ELPI. Ventolin, Bricanyl, and Atrovent were nebulized using PARI LC Plus jet nebulizers coupled to a DeVilbiss Pulmo-Aide compressor. The aerosols were sampled in 30-sec durations. The drug deposits on the impactor stages were assayed chemically using high-performance liquid chromatography (HPLC). The <span class="hlt">charges</span> of nebulized deionized water, isotonic saline, and the three commercial products diluted with saline were also measured to analyze the contributions of the major nebule ingredients on <span class="hlt">charging</span>. No mass assays were performed on these runs. All three commercial nebules generated net <span class="hlt">negative</span> <span class="hlt">charges</span>. The magnitude of the <span class="hlt">charges</span> reduced over the period of nebulization. Ventolin and Bricanyl yielded similar <span class="hlt">charge</span> profiles. Highly variable <span class="hlt">charges</span> were produced from deionized water. On the other hand, nebulized saline reproducibly generated net positive <span class="hlt">charges</span>. Diluted commercial nebules showed <span class="hlt">charge</span> polarity inversion. The <span class="hlt">charge</span> profiles of diluted salbutamol and terbutaline solutions resembled those of saline, while the <span class="hlt">charges</span> from diluted ipratropium solutions fluctuated near neutrality. The <span class="hlt">charge</span> profiles were shown to be influenced by the concentration and physicochemical properties of the drugs, as well as the history of nebulization. The drugs may have unique isoelectric concentrations in saline at which the nebulized droplets would carry near-zero <span class="hlt">charges</span>. According to results from</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010JChPh.132f5101X','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010JChPh.132f5101X"><span>Parallel tempering Monte Carlo simulations of lysozyme orientation on <span class="hlt">charged</span> surfaces</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Xie, Yun; Zhou, Jian; Jiang, Shaoyi</p> <p>2010-02-01</p> <p>In this work, the parallel tempering Monte Carlo (PTMC) algorithm is applied to accurately and efficiently identify the global-minimum-energy orientation of a protein adsorbed on a surface in a single simulation. When applying the PTMC method to simulate lysozyme orientation on <span class="hlt">charged</span> surfaces, it is found that lysozyme could easily be adsorbed on <span class="hlt">negatively</span> <span class="hlt">charged</span> surfaces with "side-on" and "back-on" orientations. When driven by dominant electrostatic interactions, lysozyme tends to be adsorbed on <span class="hlt">negatively</span> <span class="hlt">charged</span> surfaces with the side-on orientation for which the active site of lysozyme faces sideways. The side-on orientation agrees well with the experimental results where the adsorbed orientation of lysozyme is determined by electrostatic interactions. As the contribution from van der Waals interactions gradually dominates, the back-on orientation becomes the preferred one. For this orientation, the active site of lysozyme faces outward, which conforms to the experimental results where the orientation of adsorbed lysozyme is co-determined by electrostatic interactions and van der Waals interactions. It is also found that despite of its net positive <span class="hlt">charge</span>, lysozyme could be adsorbed on positively <span class="hlt">charged</span> surfaces with both "end-on" and back-on orientations owing to the nonuniform <span class="hlt">charge</span> distribution over lysozyme surface and the screening effect from ions in solution. The PTMC simulation method provides a way to determine the preferred orientation of proteins on surfaces for biosensor and biomaterial applications.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li class="active"><span>17</span></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_17 --> <div id="page_18" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li class="active"><span>18</span></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="341"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20090014075&hterms=electrostatics&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Delectrostatics','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20090014075&hterms=electrostatics&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Delectrostatics"><span>Electrostatic <span class="hlt">Charging</span> of Lunar Dust by UV Photoelectric Emissions and Solar Wind Electrons</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Abbas, Mian M.; Tankosic, Dragana; Spann, James f.; LeClair, Andre C.; Dube, Michael J.</p> <p>2008-01-01</p> <p>The ubiquitous presence of dust in the lunar environment with its high adhesive characteristics has been recognized to be a major safety issue that must be addressed in view of its hazardous effects on robotic and human exploration of the Moon. The reported observations of a horizon glow and streamers at the lunar terminator during the Apollo missions are attributed to the sunlight scattered by the levitated lunar dust. The lunar surface and the dust grains are predominantly <span class="hlt">charged</span> positively by the incident UV solar radiation on the dayside and <span class="hlt">negatively</span> by the solar wind electrons on the night-side. The <span class="hlt">charged</span> dust grains are levitated and transported over long distances by the established electric fields. A quantitative understanding of the lunar dust phenomena requires development of global dust distribution models, based on an accurate knowledge of lunar dust <span class="hlt">charging</span> properties. Currently available data of lunar dust <span class="hlt">charging</span> is based on bulk materials, although it is well recognized that measurements on individual dust grains are expected to be substantially different from the bulk measurements. In this paper we present laboratory measurements of <span class="hlt">charging</span> properties of Apollo 11 & 17 dust grains by UV photoelectric emissions and by electron impact. These measurements indicate substantial differences of both qualitative and quantitative nature between dust <span class="hlt">charging</span> properties of individual micron/submicron sized dust grains and of bulk materials. In <span class="hlt">addition</span>, there are no viable theoretical models available as yet for calculation of dust <span class="hlt">charging</span> properties of individual dust grains for both photoelectric emissions and electron impact. It is thus of paramount importance to conduct comprehensive measurements for <span class="hlt">charging</span> properties of individual dust grains in order to develop realistic models of dust processes in the lunar atmosphere, and address the hazardous issues of dust on lunar robotic and human missions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20080015655','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20080015655"><span>Measurements of <span class="hlt">Charging</span> of Apollo 17 Lunar Dust Grains by Electron Impact</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Abbas, Mian M.; Tankosic, Dragana; Spann, James F.; Dube, Michael J.</p> <p>2008-01-01</p> <p>It is well known since the Apollo missions that the lunar surface is covered with a thick layer of micron size dust grains with unusually high adhesive characteristics. The dust grains observed to be levitated and transported on the lunar surface are believed to have a hazardous impact on the robotic and human missions to the Moon. The observed dust phenomena are attributed to the lunar dust being <span class="hlt">charged</span> positively during the day by UV photoelectric emissions, and <span class="hlt">negatively</span> during the night by the solar wind electrons. The current dust <span class="hlt">charging</span> and the levitation models, however, do not fully explain the observed phenomena, with the uncertainty of dust <span class="hlt">charging</span> processes and the equilibrium potentials of the individual dust grains. It is well recognized that the <span class="hlt">charging</span> properties of individual dust grains are substantially different from those determined from measurements made on bulk materials that are currently available. An experimental facility has been developed in the Dusty Plasma Laboratory at MSFC for investigating the <span class="hlt">charging</span> and optical properties of individual micron/sub-micron size positively or <span class="hlt">negatively</span> <span class="hlt">charged</span> dust grains by levitating them in an electrodynamic balance in simulated space environments. In this paper, we present the laboratory measurements on <span class="hlt">charging</span> of Apollo 17 individual lunar dust grains by a low energy electron beam. The <span class="hlt">charging</span> rates and the equilibrium potentials produced by direct electron impact and by secondary electron emission process are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1177112','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1177112"><span>Operating a redox flow battery with a <span class="hlt">negative</span> electrolyte imbalance</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Pham, Quoc; Chang, On; Durairaj, Sumitha</p> <p>2015-03-31</p> <p>Loss of flow battery electrode catalyst layers during self-discharge or <span class="hlt">charge</span> reversal may be prevented by establishing and maintaining a <span class="hlt">negative</span> electrolyte imbalance during at least parts of a flow battery's operation. <span class="hlt">Negative</span> imbalance may be established and/or maintained actively, passively or both. Actively establishing a <span class="hlt">negative</span> imbalance may involve detecting an imbalance that is less <span class="hlt">negative</span> than a desired threshold, and processing one or both electrolytes until the imbalance reaches a desired <span class="hlt">negative</span> level. <span class="hlt">Negative</span> imbalance may be effectively established and maintained passively within a cell by constructing a cell with a <span class="hlt">negative</span> electrode chamber that is larger than the cell's positive electrode chamber, thereby providing a larger quantity of <span class="hlt">negative</span> electrolyte for reaction with positive electrolyte.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JASMS..27..124R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JASMS..27..124R"><span>High-Resolution Ambient MS Imaging of <span class="hlt">Negative</span> Ions in Positive Ion Mode: Using Dicationic Reagents with the Single-Probe</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rao, Wei; Pan, Ning; Tian, Xiang; Yang, Zhibo</p> <p>2016-01-01</p> <p>We have used the Single-probe, a miniaturized sampling device utilizing in-situ surface microextraction for ambient mass spectrometry (MS) analysis, for the high resolution MS imaging (MSI) of <span class="hlt">negatively</span> <span class="hlt">charged</span> species in the positive ionization mode. Two dicationic compounds, 1,5-pentanediyl-bis(1-butylpyrrolidinium) difluoride [C5(bpyr)2F2] and 1,3-propanediyl-bis(tripropylphosphonium) difluoride [C3(triprp)2F2], were added into the sampling solvent to form 1+ <span class="hlt">charged</span> adducts with the <span class="hlt">negatively</span> <span class="hlt">charged</span> species extracted from tissues. We were able to detect 526 and 322 <span class="hlt">negatively</span> <span class="hlt">charged</span> species this way using [C5(bpyr)2F2] and [C3(triprp)2F2], respectively, including oleic acid, arachidonic acid, and several species of phosphatidic acid, phosphoethanolamine, phosphatidylserine, phosphatidylglycerol, phosphatidylinositol, and others. In conjunction with the identification of the non-adduct cations, we have tentatively identified a total number of 1200 and 828 metabolites from mouse brain sections using [C5(bpyr)2F2] and [C3(triprp)2F2], respectively, through high mass accuracy measurements (mass error <5 ppm); MS/MS analyses were also performed to verify the identity of selected species. In <span class="hlt">addition</span> to the high mass accuracy measurement, we were able to generate high spatial resolution (~17 μm) MS images of mouse brain sections. Our study demonstrated that utilization of dicationic compounds in the surface microextraction with the Single-probe device can perform high mass and spatial resolution ambient MSI measurements of broader types of compounds in tissues. Other reagents can be potentially used with the Single-probe device for a variety of reactive MSI studies to enable the analysis of species that are previously intractable.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1996PrSS...53..305B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1996PrSS...53..305B"><span>Volume shift and <span class="hlt">charge</span> instability of simple-metal clusters</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Brajczewska, M.; Vieira, A.; Fiolhais, C.; Perdew, J. P.</p> <p>1996-12-01</p> <p>Experiment indicates that small clusters show changes (mostly contractions) of the bond lengths with respect to bulk values. We use the stabilized jellium model to study the self-expansion and self-compression of spherical clusters (neutral or ionized) of simple metals. Results from Kohn - Sham density functional theory are presented for small clusters of Al and Na, including <span class="hlt">negatively-charged</span> ones. We also examine the stability of clusters with respect to <span class="hlt">charging</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1986stos.work...24R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1986stos.work...24R"><span>Vehicle <span class="hlt">Charging</span> And Potential (VCAP)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Roberts, B.</p> <p>1986-01-01</p> <p>The vehicle <span class="hlt">charging</span> and potential (VCAP) payload includes a small electron accelerator capable of operating in a pulsed mode with firing pulses ranging from 600 nanoseconds to 107 seconds (100 milliamps at 1000 volts), a spherical retarding potential analyzer - Langmuir probe, and <span class="hlt">charge</span> current probes. This instrumentation will support studies of beam plasma interactions and the electrical <span class="hlt">charging</span> of the spacecraft. Active experiments may also be performed to investigate the fundamental processes of artificial aurora and ionospheric perturbations. In <span class="hlt">addition</span>, by firing the beam up the geomagnetic field lines of force (away from the Earth) investigations of parallel electric field may be performed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1985tpss.procW....R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1985tpss.procW....R"><span>Vehicle <span class="hlt">Charging</span> And Potential (VCAP)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Roberts, W. T.</p> <p></p> <p>The vehicle <span class="hlt">charging</span> and potential (VCAP) payload includes a small electron accelerator capable of operating in a pulsed mode with firing pulses ranging from 600 nanoseconds to 107 seconds (100 milliamps at 1000 volts), a spherical retarding potential analyzer - Langmuir probe, and <span class="hlt">charge</span> current probes. This instrumentation will support studies of beam plasma interactions and the electrical <span class="hlt">charging</span> of the spacecraft. Active experiments may also be performed to investigate the fundamental processes of artificial aurora and ionospheric perturbations. In <span class="hlt">addition</span>, by firing the beam up the geomagnetic field lines of force (away from the Earth) investigations of parallel electric field may be performed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3762602','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3762602"><span>Protein <span class="hlt">Charge</span> and Mass Contribute to the Spatio-temporal Dynamics of Protein-Protein Interactions in a Minimal Proteome</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Xu, Yu; Wang, Hong; Nussinov, Ruth; Ma, Buyong</p> <p>2013-01-01</p> <p>We constructed and simulated a ‘minimal proteome’ model using Langevin dynamics. It contains 206 essential protein types which were compiled from the literature. For comparison, we generated six proteomes with randomized concentrations. We found that the net <span class="hlt">charges</span> and molecular weights of the proteins in the minimal genome are not random. The net <span class="hlt">charge</span> of a protein decreases linearly with molecular weight, with small proteins being mostly positively <span class="hlt">charged</span> and large proteins <span class="hlt">negatively</span> <span class="hlt">charged</span>. The protein copy numbers in the minimal genome have the tendency to maximize the number of protein-protein interactions in the network. <span class="hlt">Negatively</span> <span class="hlt">charged</span> proteins which tend to have larger sizes can provide large collision cross-section allowing them to interact with other proteins; on the other hand, the smaller positively <span class="hlt">charged</span> proteins could have higher diffusion speed and are more likely to collide with other proteins. Proteomes with random <span class="hlt">charge</span>/mass populations form less stable clusters than those with experimental protein copy numbers. Our study suggests that ‘proper’ populations of <span class="hlt">negatively</span> and positively <span class="hlt">charged</span> proteins are important for maintaining a protein-protein interaction network in a proteome. It is interesting to note that the minimal genome model based on the <span class="hlt">charge</span> and mass of E. Coli may have a larger protein-protein interaction network than that based on the lower organism M. pneumoniae. PMID:23420643</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JGRD..121.2188N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JGRD..121.2188N"><span>A unified engineering model of the first stroke in downward <span class="hlt">negative</span> lightning</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nag, Amitabh; Rakov, Vladimir A.</p> <p>2016-03-01</p> <p>Each stroke in a <span class="hlt">negative</span> cloud-to-ground lightning flash is composed of downward leader and upward return stroke processes, which are usually modeled individually. The first stroke leader is stepped and starts with preliminary breakdown (PB) which is often viewed as a separate process. We present the first unified engineering model for computing the electric field produced by a sequence of PB, stepped leader, and return stroke processes, serving to transport <span class="hlt">negative</span> <span class="hlt">charge</span> to ground. We assume that a <span class="hlt">negatively</span> <span class="hlt">charged</span> channel extends downward in a stepped fashion during both the PB and leader stages. Each step involves a current wave that propagates upward along the newly formed channel section. Once the leader attaches to ground, an upward propagating return stroke neutralizes the <span class="hlt">charge</span> deposited along the channel. Model-predicted electric fields are in reasonably good agreement with simultaneous measurements at both near (hundreds of meters, electrostatic field component is dominant) and far (tens of kilometers, radiation field component is dominant) distances from the lightning channel. Relations between the features of computed electric field waveforms and model input parameters are examined. It appears that peak currents associated with PB pulses are similar to return stroke peak currents, and the observed variation of electric radiation field peaks produced by leader steps at different heights above ground is influenced by the ground corona space <span class="hlt">charge</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005AGUFMSA13A0226B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005AGUFMSA13A0226B"><span>The <span class="hlt">Charged</span> Aerosol Release Experiment (CARE)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bernhardt, P. A.; Ganguli, G.; Lampe, M.; Scales, W. A.</p> <p>2005-12-01</p> <p>The physics of radar scatter from <span class="hlt">charged</span> particulates in the upper atmosphere will be studied with the <span class="hlt">Charged</span> Aerosol Release Experiment (CARE). In 2008, two rocket payloads are being designed for launch North America. The purpose of the CARE program is to identify the mechanisms for radar scatter from polar mesospheric clouds. Polar mesospheric summer echoes (PMSE) are observed at high latitudes when small concentrations of electrons (one-thousand per cubic cm) become attached to sub-micron dust particles. Radar in the VHF (30-300 MHz) frequency range have seen 30 dB enhancements in radar echoes coincident with formation of ice near 85 km altitude. Radar echoes from electrons in the vicinity of <span class="hlt">charged</span> dust have been observed for frequencies exceeding 1 GHz. Some fundamental questions that remain about the scatting process are: (1) What is the relative importance of turbulent scatter versus incoherent (i.e., Thompson) scatter from individual electrons? (2) What produces the inhomogeneous electron/dust plasma? (3) How is the radar scatter influenced by the density of background electrons, plasma instabilities and turbulence, and photo detachment of electrons from the particulates? These questions will be addressed when the CARE program releases 50 kg of dust particles in an expanding shell at about 300 km altitude. The dust will be manufactured by the chemical release payload to provide particulate sizes in the 10 to 1000 nm range. The expanding dust shell will collect electrons making dense, heavy particles the move the <span class="hlt">negative</span> <span class="hlt">charges</span> across magnetic field lines. Plasma turbulence and electron acceleration will be formed from the <span class="hlt">charge</span> separation between the magnetized oxygen ions in the background ionosphere and the streaming <span class="hlt">negatively</span> <span class="hlt">charged</span> dust. Simulations of this process provide estimates of plasma structure which can scatter radar. As the particulates settle through the lower thermosphere into the mesosphere, artificial mesospheric clouds will be</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012JAP...112k6103M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012JAP...112k6103M"><span>An oppositely <span class="hlt">charged</span> insect exclusion screen with gap-free multiple electric fields</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Matsuda, Yoshinori; Kakutani, Koji; Nonomura, Teruo; Kimbara, Junji; Kusakari, Shin-ichi; Osamura, Kazumi; Toyoda, Hideyoshi</p> <p>2012-12-01</p> <p>An electric field screen was constructed to examine insect attraction mechanisms in multiple electric fields generated inside the screen. The screen consisted of two parallel insulated conductor wires (ICWs) <span class="hlt">charged</span> with equal but opposite voltages and two separate grounded nets connected to each other and placed on each side of the ICW layer. Insects released inside the fields were <span class="hlt">charged</span> either positively or <span class="hlt">negatively</span> as a result of electricity flow from or to the insect, respectively. The force generated between the <span class="hlt">charged</span> insects and opposite ICW <span class="hlt">charges</span> was sufficient to capture all insects.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/864392','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/864392"><span>Electrochemical cell and <span class="hlt">negative</span> electrode therefor</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Kaun, Thomas D.</p> <p>1982-01-01</p> <p>A secondary electrochemical cell with the positive and <span class="hlt">negative</span> electrodes separated by a molten salt electrolyte with the <span class="hlt">negative</span> electrode comprising a particulate mixture of lithium-aluminum alloy and electrolyte and an <span class="hlt">additive</span> selected from graphitized carbon, Raney iron or mixtures thereof. The lithium-aluminum alloy is present in the range of from about 45 to about 80 percent by volume of the <span class="hlt">negative</span> electrode, and the electrolyte is present in an amount not less than about 10 percent by volume of the <span class="hlt">negative</span> electrode. The <span class="hlt">additive</span> of graphitized carbon is present in the range of from about 1 to about 10 percent by volume of the <span class="hlt">negative</span> electrode, and the Raney iron <span class="hlt">additive</span> is present in the range of from about 3 to about 10 percent by volume of the <span class="hlt">negative</span> electrode.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3708033','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3708033"><span>Structural Pituitary Abnormalities Associated With <span class="hlt">CHARGE</span> Syndrome</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Gregory, Louise C.; Gevers, Evelien F.; Baker, Joanne; Kasia, Tessa; Chong, Kling; Josifova, Dragana J.; Caimari, Maria; Bilan, Frederic; McCabe, Mark J.</p> <p>2013-01-01</p> <p>Introduction: <span class="hlt">CHARGE</span> syndrome is a multisystem disorder that, in <span class="hlt">addition</span> to Kallmann syndrome/isolated hypogonadotrophic hypogonadism, has been associated with anterior pituitary hypoplasia (APH). However, structural abnormalities such as an ectopic posterior pituitary (EPP) have not yet been described in such patients. Objective: The aims of the study were: 1) to describe the association between <span class="hlt">CHARGE</span> syndrome and a structurally abnormal pituitary gland; and 2) to investigate whether CHD7 variants, which are identified in 65% of <span class="hlt">CHARGE</span> patients, are common in septo-optic dysplasia /hypopituitarism. Methods: We describe 2 patients with features of <span class="hlt">CHARGE</span> and EPP. CHD7 was sequenced in these and other patients with septo-optic dysplasia/hypopituitarism. Results: EPP, APH, and GH, TSH, and probable LH/FSH deficiency were present in 1 patient, and EPP and APH with GH, TSH, LH/FSH, and ACTH deficiency were present in another patient, both of whom had features of <span class="hlt">CHARGE</span> syndrome. Both had variations in CHD7 that were novel and undetected in control cohorts or in the international database of <span class="hlt">CHARGE</span> patients, but were also present in their unaffected mothers. No CHD7 variants were detected in the patients with septo-optic dysplasia/hypopituitarism without <span class="hlt">additional</span> <span class="hlt">CHARGE</span> features. Conclusion: We report a novel association between <span class="hlt">CHARGE</span> syndrome and structural abnormalities of the pituitary gland in 2 patients with variations in CHD7 that are of unknown significance. However, CHD7 mutations are an uncommon cause of septo-optic dysplasia or hypopituitarism. Our data suggest the need for evaluation of pituitary function/anatomy in patients with <span class="hlt">CHARGE</span> syndrome. PMID:23526466</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvE..97e3207M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvE..97e3207M"><span>Discrete stochastic <span class="hlt">charging</span> of aggregate grains</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Matthews, Lorin S.; Shotorban, Babak; Hyde, Truell W.</p> <p>2018-05-01</p> <p>Dust particles immersed in a plasma environment become <span class="hlt">charged</span> through the collection of electrons and ions at random times, causing the dust <span class="hlt">charge</span> to fluctuate about an equilibrium value. Small grains (with radii less than 1 μm) or grains in a tenuous plasma environment are sensitive to single <span class="hlt">additions</span> of electrons or ions. Here we present a numerical model that allows examination of discrete stochastic <span class="hlt">charge</span> fluctuations on the surface of aggregate grains and determines the effect of these fluctuations on the dynamics of grain aggregation. We show that the mean and standard deviation of <span class="hlt">charge</span> on aggregate grains follow the same trends as those predicted for spheres having an equivalent radius, though aggregates exhibit larger variations from the predicted values. In some plasma environments, these <span class="hlt">charge</span> fluctuations occur on timescales which are relevant for dynamics of aggregate growth. Coupled dynamics and <span class="hlt">charging</span> models show that <span class="hlt">charge</span> fluctuations tend to produce aggregates which are much more linear or filamentary than aggregates formed in an environment where the <span class="hlt">charge</span> is stationary.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/16296167','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/16296167"><span>Apparent electric <span class="hlt">charge</span> of protein molecules. Human thyroxine - binding proteins.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Hocman, G; Sadlon, J</p> <p>1977-01-01</p> <p>1. By comparison of electrophoretic mobilities of two different <span class="hlt">charged</span> particles under the same conditions the net elementary electrostatic <span class="hlt">charge</span> of one particle could be calculated when the <span class="hlt">charge</span> of the other is known. 2. The electrophoretic mobility of human thyroxine - binding globulin does not depend upon the concentration of Tris - HCl buffer in the range 0.05 to 0.20 molar. The value of this mobility is 0.078 and 0.083 cm2 vol(-1) hour(-1) at pH 7.0 and 8.6, respectively. 3. The net elementary electrostatic <span class="hlt">charge</span> of the human thyroxine - binding globulin appears to be approximately 22 <span class="hlt">negative</span> elementary electrostatic units in mild alkaline solutions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28735157','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28735157"><span>Effects of adhesions of amorphous Fe and Al hydroxides on surface <span class="hlt">charge</span> and adsorption of K+ and Cd2+ on rice roots.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Liu, Zhao-Dong; Wang, Hai-Cui; Zhou, Qin; Xu, Ren-Kou</p> <p>2017-11-01</p> <p>Iron (Fe) and aluminum (Al) hydroxides in variable <span class="hlt">charge</span> soils attached to rice roots may affect surface-<span class="hlt">charge</span> properties and subsequently the adsorption and uptake of nutrients and toxic metals by the roots. Adhesion of amorphous Fe and Al hydroxides onto rice roots and their effects on zeta potential of roots and adsorption of potassium (K + ) and cadmium (Cd 2+ ) by roots were investigated. Rice roots adsorbed more Al hydroxide than Fe hydroxide because of the greater positive <span class="hlt">charge</span> on Al hydroxide. Adhesion of Fe and Al hydroxides decreased the <span class="hlt">negative</span> <span class="hlt">charge</span> on rice roots, and a greater effect of the Al hydroxide. Consequently, adhesion of Fe and Al hydroxides reduced the K + and Cd 2+ adsorption by rice roots. The results of attenuated total reflectance-Fourier transform infrared spectroscopy (ATR-FTIR) and desorption of K + and Cd 2+ from rice roots indicated that physical masking by Fe and Al hydroxides and diffuse-layer overlapping between the positively-<span class="hlt">charged</span> hydroxides and <span class="hlt">negatively-charged</span> roots were responsible for the reduction of <span class="hlt">negative</span> <span class="hlt">charge</span> on roots induced by adhesion of the hydroxides. Therefore, the interaction between Fe and Al hydroxides and rice roots reduced <span class="hlt">negative</span> <span class="hlt">charge</span> on roots and thus inhibited their adsorption of nutrient and toxic cations. Copyright © 2017 Elsevier Inc. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AIPA....3k2108A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AIPA....3k2108A"><span>Sub-diffusion and trapped dynamics of neutral and <span class="hlt">charged</span> probes in DNA-protein coacervates</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Arfin, Najmul; Yadav, Avinash Chand; Bohidar, H. B.</p> <p>2013-11-01</p> <p>The physical mechanism leading to the formation of large intermolecular DNA-protein complexes has been studied. Our study aims to explain the occurrence of fast coacervation dynamics at the <span class="hlt">charge</span> neutralization point, followed by the appearance of smaller complexes and slower coacervation dynamics as the complex experiences overcharging. Furthermore, the electrostatic potential and probe mobility was investigated to mimic the transport of DNA / DNA-protein complex in a DNA-protein complex coacervate medium [N. Arfin and H. B. Bohidar, J. Phys. Chem. B 116, 13192 (2012)] by assigning neutral, <span class="hlt">negative</span>, or positive <span class="hlt">charge</span> to the probe particle. The mobility of the neutral probe was maximal at low matrix concentrations and showed random walk behavior, while its mobility ceased at the jamming concentration of c = 0.6, showing sub-diffusion and trapped dynamics. The positively <span class="hlt">charged</span> probe showed sub-diffusive random walk followed by trapped dynamics, while the <span class="hlt">negatively</span> <span class="hlt">charged</span> probe showed trapping with occasional hopping dynamics at much lower concentrations. Sub-diffusion of the probe was observed in all cases under consideration, where the electrostatic interaction was used exclusively as the dominant force involved in the dynamics. For neutral and positive probes, the mean square displacement ⟨R2⟩ exhibits a scaling with time as ⟨R2⟩ ˜ tα, distinguishing random walk and trapped dynamics at α = 0.64 ± 0.04 at c = 0.12 and c = 0.6, respectively. In <span class="hlt">addition</span>, the same scaling factors with the exponent β = 0.64 ± 0.04 can be used to distinguish random walk and trapped dynamics for the neutral and positive probes using the relation between the number of distinct sites visited by the probe, S(t), which follows the scaling, S(t) ˜ tβ/ln (t). Our results established the occurrence of a hierarchy of diffusion dynamics experienced by a probe in a dense medium that is either <span class="hlt">charged</span> or neutral.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017CQGra..34j5008S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017CQGra..34j5008S"><span>Quasi-local conserved <span class="hlt">charges</span> in the Einstein-Maxwell theory</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Setare, M. R.; Adami, H.</p> <p>2017-05-01</p> <p>In this paper we consider the Einstein-Maxwell theory and define a combined transformation composed of diffeomorphism and U(1) gauge transformation. For generality, we assume that the generator χ of such transformation is field-dependent. We define the extended off-shell ADT current and then off-shell ADT <span class="hlt">charge</span> such that they are conserved off-shell for the asymptotically field-dependent symmetry generator χ. Then, we define the conserved <span class="hlt">charge</span> corresponding to the asymptotically field-dependent symmetry generator χ. We apply the presented method to find the conserved <span class="hlt">charges</span> of the asymptotically AdS3 spacetimes in the context of the Einstein-Maxwell theory in three dimensions. Although the usual proposal for the quasi local <span class="hlt">charges</span> provides divergent global <span class="hlt">charges</span> for the Einstein-Maxwell theory with <span class="hlt">negative</span> cosmological constant in three dimensions, here we avoid this problem by introducing proposed combined transformation χ</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2706807','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2706807"><span>A new biphasic osteoinductive calcium composite material with a <span class="hlt">negative</span> Zeta potential for bone augmentation</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Smeets, Ralf; Kolk, Andreas; Gerressen, Marcus; Driemel, Oliver; Maciejewski, Oliver; Hermanns-Sachweh, Benita; Riediger, Dieter; Stein, Jamal M</p> <p>2009-01-01</p> <p>The aim of the present study was to analyze the osteogenic potential of a biphasic calcium composite material (BCC) with a <span class="hlt">negative</span> surface <span class="hlt">charge</span> for maxillary sinus floor augmentation. In a 61 year old patient, the BCC material was used in a bilateral sinus floor augmentation procedure. Six months postoperative, a bone sample was taken from the augmented regions before two titanium implants were inserted at each side. We analyzed bone neoformation by histology, bone density by computed tomography, and measured the activity of voltage-activated calcium currents of osteoblasts and surface <span class="hlt">charge</span> effects. Control orthopantomograms were carried out five months after implant insertion. The BCC was biocompatible and replaced by new mineralized bone after being resorbed completely. The material demonstrated a <span class="hlt">negative</span> surface <span class="hlt">charge</span> (<span class="hlt">negative</span> Zeta potential) which was found to be favorable for bone regeneration and osseointegration of dental implants. PMID:19523239</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=physics+AND+glass&pg=2&id=EJ1148975','ERIC'); return false;" href="https://eric.ed.gov/?q=physics+AND+glass&pg=2&id=EJ1148975"><span>An Instrumental Method to Identify Electric <span class="hlt">Charge</span> Types with a Simple Device</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Isik, Hakan</p> <p>2015-01-01</p> <p>In this study, an easy and enjoyable activity to determine the type of electric <span class="hlt">charge</span> is presented, using a readymade electronic test screw. A four-way usage of the tester is explained with an electroscope. In the activity, ebonite and glass rods are <span class="hlt">negatively</span> and positively <span class="hlt">charged</span> by rubbing with paper sheets, respectively.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li class="active"><span>18</span></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_18 --> <div id="page_19" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li class="active"><span>19</span></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="361"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JPhD...50T5603Q','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JPhD...50T5603Q"><span>Surface <span class="hlt">charge</span> accumulation of solid insulator under nanosecond pulse in vacuum: 3D distribution features and mechanism</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Qi, Bo; Gao, Chunjia; Sun, Zelai; Li, Chengrong</p> <p>2017-11-01</p> <p>Surface <span class="hlt">charge</span> accumulation can incur changes in electric field distribution, involved in the electron propagation process, and result in a significant decrease in the surface flashover voltage. The existing 2D surface <span class="hlt">charge</span> measurement fails to meet the actual needs in real engineering applications that usually adopt the 45° conical frustum insulators. The present research developed a novel 3D measurement platform to capture surface <span class="hlt">charge</span> distribution on solid insulation under nanosecond pulse in a vacuum. The results indicate that all surface <span class="hlt">charges</span> are positive under a positive pulse and <span class="hlt">negative</span> under a <span class="hlt">negative</span> pulse. Surface <span class="hlt">charges</span> tend to accumulate more near the upper electrode. Surface <span class="hlt">charge</span> density increases significantly with the increase in pulse counts and amplitudes. Accumulation of surface <span class="hlt">charge</span> results in a certain decrease of flashover voltage. Taking consideration of the secondary electron emission for the surface <span class="hlt">charge</span> accumulation, four materials were obtained to demonstrate the effects on surface <span class="hlt">charge</span>. Combining the effect incurred by secondary electron emission and the weighty action taken by surface <span class="hlt">charge</span> accumulation on the flashover phenomena, the discharge mechanism along the insulator surface under nanosecond pulse voltage was proposed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..APR.X1022S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..APR.X1022S"><span><span class="hlt">Charge</span> Transport Properties in Disordered Organic Semiconductor as a Function of <span class="hlt">Charge</span> Density: Monte Carlo Simulation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shukri, Seyfan Kelil</p> <p>2017-01-01</p> <p>We have done Kinetic Monte Carlo (KMC) simulations to investigate the effect of <span class="hlt">charge</span> carrier density on the electrical conductivity and carrier mobility in disordered organic semiconductors using a lattice model. The density of state (DOS) of the system are considered to be Gaussian and exponential. Our simulations reveal that the mobility of the <span class="hlt">charge</span> carrier increases with <span class="hlt">charge</span> carrier density for both DOSs. In contrast, the mobility of <span class="hlt">charge</span> carriers decreases as the disorder increases. In <span class="hlt">addition</span> the shape of the DOS has a significance effect on the <span class="hlt">charge</span> transport properties as a function of density which are clearly seen. On the other hand, for the same distribution width and at low carrier density, the change occurred on the conductivity and mobility for a Gaussian DOS is more pronounced than that for the exponential DOS.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014JGRA..119.6190Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014JGRA..119.6190Y"><span>Random dust <span class="hlt">charge</span> fluctuations in the near-Enceladus plasma</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yaroshenko, V. V.; Lühr, H.</p> <p>2014-08-01</p> <p>Stochastic dust <span class="hlt">charge</span> fluctuations have been studied in the light of Cassini data on the near-Enceladus plasma environment. Estimates of fluctuation time scales showed that this process can be of importance for the grains emanating from the icy moon. The analytical modeling predicts that in the dust-loaded Enceladus plasma a majority of the grains acquires fluctuating <span class="hlt">negative</span> <span class="hlt">charges</span>, but there might appear a minority of positively <span class="hlt">charged</span> particles. The probability of this effect mostly depends on the ratio of the dust/plasma number densities. Our findings appear to be supported by the available Cassini Plasma Spectrometer measurements of the <span class="hlt">charged</span> grain distributions during E3 and E5 plume flybys. The theoretical results can also provide new insights into the intricate process of particle dynamics in the inner magnetosphere.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/6260685','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/biblio/6260685"><span>Noise reduction in <span class="hlt">negative</span>-ion quadrupole mass spectrometry</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Chastagner, P.</p> <p>1993-04-20</p> <p>A quadrupole mass spectrometer (QMS) system is described having an ion source, quadrupole mass filter, and ion collector/recorder system. A weak, transverse magnetic field and an electron collector are disposed between the quadrupole and ion collector. When operated in <span class="hlt">negative</span> ion mode, the ion source produces a beam of primarily <span class="hlt">negatively-charged</span> particles from a sample, including electrons as well as ions. The beam passes through the quadrupole and enters the magnetic field, where the electrons are deflected away from the beam path to the electron collector. The <span class="hlt">negative</span> ions pass undeflected to the ion collector where they are detected and recorded as a mass spectrum.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/868753','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/868753"><span>Noise reduction in <span class="hlt">negative</span>-ion quadrupole mass spectrometry</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Chastagner, Philippe</p> <p>1993-01-01</p> <p>A quadrupole mass spectrometer (QMS) system having an ion source, quadrupole mass filter, and ion collector/recorder system. A weak, transverse magnetic field and an electron collector are disposed between the quadrupole and ion collector. When operated in <span class="hlt">negative</span> ion mode, the ion source produces a beam of primarily <span class="hlt">negatively-charged</span> particles from a sample, including electrons as well as ions. The beam passes through the quadrupole and enters the magnetic field, where the electrons are deflected away from the beam path to the electron collector. The <span class="hlt">negative</span> ions pass undeflected to the ion collector where they are detected and recorded as a mass spectrum.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28915532','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28915532"><span>Formation mechanism of human serum albumin monolayers on positively <span class="hlt">charged</span> polymer microparticles.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Nattich-Rak, Małgorzata; Sadowska, Marta; Adamczyk, Zbigniew; Cieśla, Michał; Kąkol, Małgorzata</p> <p>2017-11-01</p> <p>Human serum albumin (HSA) adsorption on positively and <span class="hlt">negatively</span> <span class="hlt">charged</span> polystyrene microparticles was studied at various pHs and NaCl concentrations. Thorough electrophoretic mobility measurements were carried out that enabled to monitor in situ the progress of protein adsorption. The maximum coverage of irreversibly adsorbed HSA on microparticles was determined by different concentration depletion methods, one of them involving AFM imaging of residual molecules. An anomalous adsorption of HSA on the positive microparticles was observed at pH 3.5 where the maximum coverage attained 1.0mgm -2 for NaCl concentrations of 0.05M despite that the molecules were on average positively <span class="hlt">charged</span>. For comparison, the maximum coverage of HSA on <span class="hlt">negatively</span> <span class="hlt">charged</span> microparticles was equal to 1.3mgm -2 at this pH and NaCl concentration. At pH 7.4 the maximum coverage on positive microparticles was equal to 2.1mgm -2 for 0.05M NaCl concentration. On the other hand, for <span class="hlt">negative</span> microparticles, negligible adsorption of HSA was observed at pH 7.4 and 9.7. These experimental data were adequately interpreted in terms of the random sequential adsorption approach exploiting the bead model of the HSA molecule. Different orientations of adsorbed molecules, inert alia, the edge-on orientation prevailing for positively <span class="hlt">charged</span> microparticles at pH 7.4, were confirmed. This was explained in terms of a heterogeneous <span class="hlt">charge</span> distribution over the HSA molecule prevailing for a wide range of pHs. Copyright © 2017 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1984PhLB..140..137M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1984PhLB..140..137M"><span>Observation of coherent diffractive <span class="hlt">charged</span> current interactions of antineutrinos on neon nuclei</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Marage, P.; Aderholz, M.; Armenise, N.; Azemoon, T.; Barnham, K. W. J.; Bartley, J. H.; Baton, J. P.; Bertrand, D.; Brisson, V.; Bullock, F. W.; Calicchio, M.; Cooper, A. M.; Chwastowski, J.; Clayton, E. F.; Coghen, T.; Erriquez, O.; Fitch, P. J.; Gerbier, G.; Guy, J.; Hulth, P. O.; Jones, G. T.; Kasper, P.; Kochowski, C.; Leighton-Davies, S.; Middleton, R. P.; Mobayyen, M. M.; Morrison, D. R. O.; Neveu, M.; Nuzzo, S.; O'Neale, S. W.; Parker, M. A.; Petiau, P.; Ruggieri, F.; Sacton, J.; Sansum, R. A.; Simopoulou, E.; Talebzadeh, M.; Vallee, C.; Varvell, K.; Vayaki, A.; Venus, W.; Wells, J.; Wernhard, K. L.; Wittek, W.; Zevgolatakos, E.; WA59 Collaboration</p> <p>1984-05-01</p> <p>First observation is reported of semi-inclusive coherent diffractive <span class="hlt">charged</span> current interactions of antineutrinos on neon nuclei. A sharp peaking towards zero is observed in the | t| distribution of interactions for which the final state <span class="hlt">charge</span> is 0 and from which only one <span class="hlt">negative</span> hadron is emitted, unaccompanied by any evidence of nuclear fragmentation or reinteraction. This peak is correlated with high momentum of the outgoing <span class="hlt">charged</span> hadron and with small values of Q2 and x.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25839122','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25839122"><span>Surface <span class="hlt">charge</span> tunability as a powerful strategy to control electrostatic interaction for high efficiency silencing, using tailored oligopeptide-modified poly(beta-amino ester)s (PBAEs).</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Dosta, Pere; Segovia, Nathaly; Cascante, Anna; Ramos, Victor; Borrós, Salvador</p> <p>2015-07-01</p> <p>Here we present an extended family of pBAEs that incorporate terminal oligopeptide moieties synthesized from both positive and <span class="hlt">negative</span> amino acids. Polymer formulations of mixtures of <span class="hlt">negative</span> and positive oligopeptide-modified pBAEs are capable of condensing siRNA into discrete nanoparticles. We have demonstrated that efficient delivery of nucleic acids in a cell-type dependent manner can be achieved by careful control of the pBAE formulation. In <span class="hlt">addition</span>, our approach of adding differently <span class="hlt">charged</span> oligopeptides to the termini of poly(β-amino ester)s is of great interest for the design of tailored complexes having specific features, such as tuneable zeta potential. We anticipate that this surface <span class="hlt">charge</span> tunability may be a powerful strategy to control unwanted electrostatic interactions, while preserving high silencing efficiency and reduced toxicity. Copyright © 2015 Acta Materialia Inc. Published by Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/872937','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/872937"><span>Electrochemical storage cell containing a substituted anisole or di-anisole redox shuttle <span class="hlt">additive</span> for overcharge protection and suitable for use in liquid organic and solid polymer electrolytes</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Kerr, John B.; Tian, Minmin</p> <p>2000-01-01</p> <p>A electrochemical cell is described comprising an anode, a cathode, a solid polymer electrolyte, and a redox shuttle <span class="hlt">additive</span> to protect the cell against overcharging and a redox shuttle <span class="hlt">additive</span> to protect the cell against overcharging selected from the group consisting of: (a) a substituted anisole having the general formula (in an uncharged state): ##STR1## where R.sub.1 is selected from the group consisting of H, OCH.sub.3, OCH.sub.2 CH.sub.3, and OCH.sub.2 phenyl, and R.sub.2 is selected from the group consisting of OCH.sub.3, OCH.sub.2 CH.sub.3, OCH.sub.2 phenyl, and O.sup.- Li.sup.+ ; and (b) a di-anisole compound having the general formula (in an uncharged state): ##STR2## where R is selected from the group consisting of -OCH.sub.3 and -CH.sub.3, m is either 1 or 0, n is either 1 or 0, and X is selected from the group consisting of -OCH.sub.3 (methoxy) or its lithium salt --O.sup.- Li.sup.+. The lithium salt of the di-anisole is the preferred form of the redox shuttle <span class="hlt">additive</span> because the shuttle anion will then initially have a single <span class="hlt">negative</span> <span class="hlt">charge</span>, it loses two electrons when it is oxidized at the cathode, and then moves toward the anode as a single positively <span class="hlt">charged</span> species where it is then reduced to a single <span class="hlt">negatively</span> <span class="hlt">charged</span> species by gaining back two electrons.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=308486&Lab=NHEERL&keyword=algae&actType=&TIMSType=+&TIMSSubTypeID=&DEID=&epaNumber=&ntisID=&archiveStatus=Both&ombCat=Any&dateBeginCreated=&dateEndCreated=&dateBeginPublishedPresented=&dateEndPublishedPresented=&dateBeginUpdated=&dateEndUpdated=&dateBeginCompleted=&dateEndCompleted=&personID=&role=Any&journalID=&publisherID=&sortBy=revisionDate&count=50','EPA-EIMS'); return false;" href="https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=308486&Lab=NHEERL&keyword=algae&actType=&TIMSType=+&TIMSSubTypeID=&DEID=&epaNumber=&ntisID=&archiveStatus=Both&ombCat=Any&dateBeginCreated=&dateEndCreated=&dateBeginPublishedPresented=&dateEndPublishedPresented=&dateBeginUpdated=&dateEndUpdated=&dateBeginCompleted=&dateEndCompleted=&personID=&role=Any&journalID=&publisherID=&sortBy=revisionDate&count=50"><span>Ulva <span class="hlt">additions</span> alter soil biogeochemistry and <span class="hlt">negatively</span> impact Spartina alterniflora growth</span></a></p> <p><a target="_blank" href="http://oaspub.epa.gov/eims/query.page">EPA Science Inventory</a></p> <p></p> <p></p> <p>Decaying mats of Ulva can be washed into salt marshes by the tides as large wrack deposits, especially in eutrophic estuaries, where they can <span class="hlt">negatively</span> impact marsh vegetation. We report on a series of field and laboratory mesocosm experiments where we examined the effects of d...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29604827','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29604827"><span>Sequence <span class="hlt">charge</span> decoration dictates coil-globule transition in intrinsically disordered proteins.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Firman, Taylor; Ghosh, Kingshuk</p> <p>2018-03-28</p> <p>We present an analytical theory to compute conformations of heteropolymers-applicable to describe disordered proteins-as a function of temperature and <span class="hlt">charge</span> sequence. The theory describes coil-globule transition for a given protein sequence when temperature is varied and has been benchmarked against the all-atom Monte Carlo simulation (using CAMPARI) of intrinsically disordered proteins (IDPs). In <span class="hlt">addition</span>, the model quantitatively shows how subtle alterations of <span class="hlt">charge</span> placement in the primary sequence-while maintaining the same <span class="hlt">charge</span> composition-can lead to significant changes in conformation, even as drastic as a coil (swelled above a purely random coil) to globule (collapsed below a random coil) and vice versa. The theory provides insights on how to control (enhance or suppress) these changes by tuning the temperature (or solution condition) and <span class="hlt">charge</span> decoration. As an application, we predict the distribution of conformations (at room temperature) of all naturally occurring IDPs in the DisProt database and notice significant size variation even among IDPs with a similar composition of positive and <span class="hlt">negative</span> <span class="hlt">charges</span>. Based on this, we provide a new diagram-of-states delineating the sequence-conformation relation for proteins in the DisProt database. Next, we study the effect of post-translational modification, e.g., phosphorylation, on IDP conformations. Modifications as little as two-site phosphorylation can significantly alter the size of an IDP with everything else being constant (temperature, salt concentration, etc.). However, not all possible modification sites have the same effect on protein conformations; there are certain "hot spots" that can cause maximal change in conformation. The location of these "hot spots" in the parent sequence can readily be identified by using a sequence <span class="hlt">charge</span> decoration metric originally introduced by Sawle and Ghosh. The ability of our model to predict conformations (both expanded and collapsed states) of IDPs at a high</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JChPh.148l3305F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JChPh.148l3305F"><span>Sequence <span class="hlt">charge</span> decoration dictates coil-globule transition in intrinsically disordered proteins</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Firman, Taylor; Ghosh, Kingshuk</p> <p>2018-03-01</p> <p>We present an analytical theory to compute conformations of heteropolymers—applicable to describe disordered proteins—as a function of temperature and <span class="hlt">charge</span> sequence. The theory describes coil-globule transition for a given protein sequence when temperature is varied and has been benchmarked against the all-atom Monte Carlo simulation (using CAMPARI) of intrinsically disordered proteins (IDPs). In <span class="hlt">addition</span>, the model quantitatively shows how subtle alterations of <span class="hlt">charge</span> placement in the primary sequence—while maintaining the same <span class="hlt">charge</span> composition—can lead to significant changes in conformation, even as drastic as a coil (swelled above a purely random coil) to globule (collapsed below a random coil) and vice versa. The theory provides insights on how to control (enhance or suppress) these changes by tuning the temperature (or solution condition) and <span class="hlt">charge</span> decoration. As an application, we predict the distribution of conformations (at room temperature) of all naturally occurring IDPs in the DisProt database and notice significant size variation even among IDPs with a similar composition of positive and <span class="hlt">negative</span> <span class="hlt">charges</span>. Based on this, we provide a new diagram-of-states delineating the sequence-conformation relation for proteins in the DisProt database. Next, we study the effect of post-translational modification, e.g., phosphorylation, on IDP conformations. Modifications as little as two-site phosphorylation can significantly alter the size of an IDP with everything else being constant (temperature, salt concentration, etc.). However, not all possible modification sites have the same effect on protein conformations; there are certain "hot spots" that can cause maximal change in conformation. The location of these "hot spots" in the parent sequence can readily be identified by using a sequence <span class="hlt">charge</span> decoration metric originally introduced by Sawle and Ghosh. The ability of our model to predict conformations (both expanded and collapsed states) of IDPs at</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhPl...25a0702Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhPl...25a0702Y"><span>Reversed Hall effect and plasma conductivity in the presence of <span class="hlt">charged</span> impurities</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yaroshenko, V. V.; Lühr, H.</p> <p>2018-01-01</p> <p>The Hall conductivity of magnetized plasma can be strongly suppressed by the contribution of <span class="hlt">negatively</span> <span class="hlt">charged</span> particulates (referred further as "dust"). Once the <span class="hlt">charge</span> density accumulated by the dust exceeds a certain threshold, the Hall component becomes <span class="hlt">negative</span>, providing a reversal in the Hall current. Such an effect is unique for dust-loaded plasmas, and it can hardly be achieved in electronegative plasmas. Further growth of the dust density leads to an increase in both the absolute value of the Hall and Pedersen conductivities, while the field-aligned component is decreased. These modifications enhance the role of transverse electric currents and reduce the anisotropy of a magnetized plasma when loaded with <span class="hlt">charged</span> impurities. The findings provide an important basis for studying the generation of electric currents and transport phenomena in magnetized plasma systems containing small <span class="hlt">charged</span> particulates. They can be relevant for a wide range of applications from naturally occurring space plasmas in planetary magnetospheres and astrophysical objects to laboratory dusty plasmas (Magnetized Dusty Plasma Experiment) and to technological and fusion plasmas.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004JChPh.121..457G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004JChPh.121..457G"><span>Brownian dynamics simulations of simplified cytochrome c molecules in the presence of a <span class="hlt">charged</span> surface</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gorba, C.; Geyer, T.; Helms, V.</p> <p>2004-07-01</p> <p>Simulations were performed for up to 150 simplified spherical horse heart cytochrome c molecules in the presence of a <span class="hlt">charged</span> surface, which serves as an approximate model for a lipid membrane. Screened electrostatic and short-ranged attractive as well as repulsive van der Waals forces for interparticle and particle-membrane interactions are utilized in the simulations. At a distance from the membrane, where particle-membrane interactions are negligible, the simulation is coupled to a noninteraction continuum analogous to a heat bath [Geyer et al., J. Chem. Phys. 120, 4573 (2004)]. From the particles' density profiles perpendicular to the planar surface binding isotherms are derived and compared to experimental results [Heimburg et al. (1999)]. Using a <span class="hlt">negatively</span> <span class="hlt">charged</span> structureless membrane surface a saturation effect was found for relatively large particle concentrations. Since biological membranes often contain membrane proteins, we also studied the influence of <span class="hlt">additional</span> <span class="hlt">charges</span> on our model membrane mimicking bacterial reaction centers. We find that the onset of the saturation occurs for much lower concentrations and is sensitive to the detailed implementation. Therefore we suggest that local distortion of membrane planarity (undulation), or lipid demixing, or the presence of <span class="hlt">charged</span> integral membrane proteins create preferential binding sites on the membrane. Only then do we observe saturation at physiological concentrations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhTea..55..470M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhTea..55..470M"><span>Simple Pencil-and-Paper Notation for Representing Electrical <span class="hlt">Charge</span> States</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Morse, Robert A.</p> <p>2017-11-01</p> <p>In Benjamin Franklin's one fluid theory of electrification, ordinary unelectrified matter consisted of a matrix of matter suffused with a certain amount of "electrical fluid." Electrical effects were due to an excess or deficit of electrical fluid, hence the terms positive and <span class="hlt">negative</span>. Before the development of a modern view of the atom, diagrams showing <span class="hlt">charged</span> objects would simply have "+" or "-" signs to indicate the <span class="hlt">charged</span> state. As physicists we know how to interpret these diagrams and understand what they are telling us about the underlying atomic model of <span class="hlt">charging</span>. However, novice students may not readily make the connection between the atomic model, in which a <span class="hlt">charged</span> solid object either gains or loses electrons but does not gain or lose positive <span class="hlt">charges</span>. Furthermore, when isolated objects become <span class="hlt">charged</span>, the total number of electrons must be accounted for as <span class="hlt">charge</span> is a conserved quantity. To really understand the changes that occur in <span class="hlt">charging</span> by contact, conduction, or induction, it is useful for students to visually represent the processes in a way that emphasizes the atomicity of the processes, including the induced polarization of objects, and the requirement that <span class="hlt">charge</span> be conserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23982864','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23982864"><span>Transfer RNA: a dancer between <span class="hlt">charging</span> and mis-<span class="hlt">charging</span> for protein biosynthesis.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zhou, Xiaolong; Wang, Enduo</p> <p>2013-10-01</p> <p>Transfer RNA plays a fundamental role in the protein biosynthesis as an adaptor molecule by functioning as a biological link between the genetic nucleotide sequence in the mRNA and the amino acid sequence in the protein. To perform its role in protein biosynthesis, it has to be accurately recognized by aminoacyl-tRNA synthetases (aaRSs) to generate aminoacyl-tRNAs (aa-tRNAs). The correct pairing between an amino acid with its cognate tRNA is crucial for translational quality control. Production and utilization of mis-<span class="hlt">charged</span> tRNAs are usually detrimental for all the species, resulting in cellular dysfunctions. Correct aa-tRNAs formation is collectively controlled by aaRSs with distinct mechanisms and/or other trans-factors. However, in very limited instances, mis-<span class="hlt">charged</span> tRNAs are intermediate for specific pathways or essential components for the translational machinery. Here, from the point of accuracy in tRNA <span class="hlt">charging</span>, we review our understanding about the mechanism ensuring correct aa-tRNA generation. In <span class="hlt">addition</span>, some unique mis-<span class="hlt">charged</span> tRNA species necessary for the organism are also briefly described.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/3592324','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/3592324"><span>Interstitial distribution of <span class="hlt">charged</span> macromolecules in the dog lung: a kinetic model.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Parker, J C; Miniati, M; Pitt, R; Taylor, A E</p> <p>1987-01-01</p> <p>A mathematic model was constructed to investigate conflicting physiologic data concerning the <span class="hlt">charge</span> effect of continuous capillaries to macromolecules in the lung. We simulated the equilibration kinetics of lactate dehydrogenase (MR 4.2 nM) isozymes LDH 1 (pI = 5.0) and LDH 5 (pI = 7.9) between plasma and lymph using previously measured permeability coefficients, lung tissue distribution volumes (VA) and plasma concentrations (CP) in lung tissue. Our hypothesis is that the fixed anionic <span class="hlt">charges</span> in interstitium, basement membrane, and cell surfaces determine equilibration rather than <span class="hlt">charged</span> membrane effects at the capillary barrier, so the same capillary permeability coefficients were used for both isozymes. Capillary filtration rates and protein fluxes were calculated using conventional flux equations. Initial conditions at baseline and increased left atrial pressures (PLA) were those measured in animal studies. Simulated equilibration of isozymes over 30 h in the model at baseline capillary pressures accurately predicted the observed differences in lymph/plasma concentration ratios (CL/CP) between isotopes at 4 h and equilibration of these ratios at 24 h. Quantitative prediction of isozyme CL/CP ratios was also obtained at increased PLA. However, an <span class="hlt">additional</span> cation selective compartment representing the surface glycocalyx was required to accurately simulate the initial higher transcapillary clearances of cationic LDH 5. Thus experimental data supporting the <span class="hlt">negative</span> barrier, positive barrier, and no <span class="hlt">charge</span> barrier hypotheses were accurately reproduced by the model using only the observed differences in interstitial partitioning of isozymes without differences in capillary selectivity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19880001070','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19880001070"><span>The physics of <span class="hlt">charge</span> separation preceding lightning strokes in thunderclouds</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kyrala, Ali</p> <p>1987-01-01</p> <p>The physics of <span class="hlt">charge</span> separation preceding lightning strokes in thunderclouds is presented by three types of arguments: An explanation is given for the aggregation of electrical <span class="hlt">charges</span> of like sign overcoming Coulomb repulsion by attraction due to exchange interaction. The latter is well known in quantum mechanics from the theories of the nuclear bond and the covalent bond. A classical electrostatic model of <span class="hlt">charge</span> balls of segregated positive and <span class="hlt">negative</span> <span class="hlt">charges</span> in the thundercloud is presented. These <span class="hlt">charge</span> balls can only be maintained in temporarily stable locations by a containing vortex. Because they will be of different sizes and masses, they will stabilize at different altitudes when drag forces are included with the given electrostatic force. The question of how the <span class="hlt">charges</span> become concentrated again after lightning discharges is approached by means of the collisional Boltzmann transport equation to explain quasi-periodic recharging. It is shown that solutions cannot be separable in both position and time if they are to represent aggregation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29433313','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29433313"><span>Grain Boundaries Act as Solid Walls for <span class="hlt">Charge</span> Carrier Diffusion in Large Crystal MAPI Thin Films.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ciesielski, Richard; Schäfer, Frank; Hartmann, Nicolai F; Giesbrecht, Nadja; Bein, Thomas; Docampo, Pablo; Hartschuh, Achim</p> <p>2018-03-07</p> <p>Micro- and nanocrystalline methylammonium lead iodide (MAPI)-based thin-film solar cells today reach power conversion efficiencies of over 20%. We investigate the impact of grain boundaries on <span class="hlt">charge</span> carrier transport in large crystal MAPI thin films using time-resolved photoluminescence (PL) microscopy and numerical model calculations. Crystal sizes in the range of several tens of micrometers allow for the spatially and time resolved study of boundary effects. Whereas long-ranged diffusive <span class="hlt">charge</span> carrier transport is observed within single crystals, no detectable diffusive transport occurs across grain boundaries. The observed PL transients are found to crucially depend on the microscopic geometry of the crystal and the point of observation. In particular, spatially restricted diffusion of <span class="hlt">charge</span> carriers leads to slower PL decay near crystal edges as compared to the crystal center. In contrast to many reports in the literature, our experimental results show no quenching or <span class="hlt">additional</span> loss channels due to grain boundaries for the studied material, which thus do not <span class="hlt">negatively</span> affect the performance of the derived thin-film devices.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010JOpt...12l4008V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010JOpt...12l4008V"><span>Electric <span class="hlt">charging</span> influence in holograms of total internal reflection, recorded in a very thin chalcogenide film</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vlaeva, I.; Petkov, K.; Tasseva, J.; Todorov, R.; Yovcheva, T.; Sainov, S.</p> <p>2010-12-01</p> <p>We report the results of electric field influence on holographic recording in very thin chalcogenide glass films. The total internal reflection prism recording technique (Stetson's scheme) is applied for holographic recording. The main advantage of this scheme is the possibility of holographic recording in micro- and nanometer thick photosensitive materials. In the present work, 30 nm, 50 nm and 1.0 µm thick films are used. In the 1.0 µm thick film two slanted gratings are simultaneously recorded. In this recording geometry only one reconstructed beam is observed. The corona <span class="hlt">charging</span> influence on the diffraction efficiency of the recorded gratings is investigated. A <span class="hlt">negative</span> voltage of 5 kV is applied to the corona electrode (needle) prior to the holographic recording. The observed diffraction efficiency of <span class="hlt">charged</span> samples is always higher in comparison with uncharged samples. The reconstructed beam intensity is monitored with a red (635 nm) semiconductor laser. The possible reason is an <span class="hlt">additional</span> refractive index modulation due to the increase in polarization, caused by the electric <span class="hlt">charging</span>.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li class="active"><span>19</span></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_19 --> <div id="page_20" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li class="active"><span>20</span></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="381"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016APS..MARS45008D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016APS..MARS45008D"><span>Optical patterning of trapped <span class="hlt">charge</span> in nitrogen-doped diamond</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dhomkar, Siddharth; Jayakumar, Harishankar; Pagliero, Daniela; Laraoui, Abdelghani; Albu, Remus; Manson, Neil; Doherty, Marcus; Henshaw, Jacob; Meriles, Carlos</p> <p></p> <p>The nitrogen-vacancy (NV) center in diamond is emerging as a promising platform for solid-state quantum information processing and nanoscale metrology. Of interest in these applications is the manipulation of the NV <span class="hlt">charge</span> state, which can be attained by optical illumination. Here we use two-color optical microscopy to investigate the dynamics of NV photo-ionization, <span class="hlt">charge</span> diffusion, and trapping in type-1b diamond. We combine fixed-point laser excitation and scanning fluorescence imaging to locally alter the concentration of <span class="hlt">negatively</span> <span class="hlt">charged</span> NVs and to subsequently probe the corresponding redistribution of <span class="hlt">charge</span>. We uncover the formation of various spatial patterns of trapped <span class="hlt">charge</span>, which we semi-quantitatively reproduce via a model of the interplay between photo-excited carriers and atomic defects in the diamond lattice. Further, by using the NV as a local probe, we map the relative fraction of positively <span class="hlt">charged</span> nitrogen upon localized optical excitation. These observations may prove important to various technologies, including the transport of quantum information between remote NVs and the development of three-dimensional, <span class="hlt">charge</span>-based memories. We acknowledge support from the National Science Foundation through Grant NSF-1314205.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhRvE..96b2401L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhRvE..96b2401L"><span>Impact of a nonuniform <span class="hlt">charge</span> distribution on virus assembly</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, Siyu; Erdemci-Tandogan, Gonca; Wagner, Jef; van der Schoot, Paul; Zandi, Roya</p> <p>2017-08-01</p> <p>Many spherical viruses encapsulate their genomes in protein shells with icosahedral symmetry. This process is spontaneous and driven by electrostatic interactions between positive domains on the virus coat proteins and the <span class="hlt">negative</span> genomes. We model the effect of the nonuniform icosahedral <span class="hlt">charge</span> distribution from the protein shell instead using a mean-field theory. We find that this nonuniform <span class="hlt">charge</span> distribution strongly affects the optimal genome length and that it can explain the experimentally observed phenomenon of overcharging of virus and viruslike particles.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26937766','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26937766"><span>A Commercial Conducting Polymer as Both Binder and Conductive <span class="hlt">Additive</span> for Silicon Nanoparticle-Based Lithium-Ion Battery <span class="hlt">Negative</span> Electrodes.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Higgins, Thomas M; Park, Sang-Hoon; King, Paul J; Zhang, Chuanfang John; McEvoy, Niall; Berner, Nina C; Daly, Dermot; Shmeliov, Aleksey; Khan, Umar; Duesberg, Georg; Nicolosi, Valeria; Coleman, Jonathan N</p> <p>2016-03-22</p> <p>This work describes silicon nanoparticle-based lithium-ion battery <span class="hlt">negative</span> electrodes where multiple nonactive electrode <span class="hlt">additives</span> (usually carbon black and an inert polymer binder) are replaced with a single conductive binder, in this case, the conducting polymer PSS. While enabling the production of well-mixed slurry-cast electrodes with high silicon content (up to 95 wt %), this combination eliminates the well-known occurrence of capacity losses due to physical separation of the silicon and traditional inorganic conductive <span class="hlt">additives</span> during repeated lithiation/delithiation processes. Using an in situ secondary doping treatment of the PSS with small quantities of formic acid, electrodes containing 80 wt % SiNPs can be prepared with electrical conductivity as high as 4.2 S/cm. Even at the relatively high areal loading of 1 mg/cm(2), this system demonstrated a first cycle lithiation capacity of 3685 mA·h/g (based on the SiNP mass) and a first cycle efficiency of ∼78%. After 100 repeated cycles at 1 A/g this electrode was still able to store an impressive 1950 mA·h/g normalized to Si mass (∼75% capacity retention), corresponding to 1542 mA·h/g when the capacity is normalized by the total electrode mass. At the maximum electrode thickness studied (∼1.5 mg/cm(2)), a high areal capacity of 3 mA·h/cm(2) was achieved. Importantly, these electrodes are based on commercially available components and are produced by the standard slurry coating methods required for large-scale electrode production. Hence, the results presented here are highly relevant for the realization of commercial LiB <span class="hlt">negative</span> electrodes that surpass the performance of current graphite-based <span class="hlt">negative</span> electrode systems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4621264','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4621264"><span>Miniature Dual-Corona Ionizer for Bipolar <span class="hlt">Charging</span> of Aerosol</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Qi, Chaolong; Kulkarni, Pramod</p> <p>2015-01-01</p> <p>A corona-based bipolar charger has been developed for use in compact, field-portable mobility size spectrometers. The charger employs an aerosol flow cavity exposed to two corona ionizers producing ions of opposite polarity. Each corona ionizer houses two electrodes in parallel needle-mesh configuration and is operated at the same magnitude of corona current. Experimental measurement of detailed <span class="hlt">charge</span> distribution of near-monodisperse particles of different diameter in the submicrometer size range showed that the charger is capable of producing well-defined, consistent bipolar <span class="hlt">charge</span> distributions for flow rates up to 1.5 L/min and aerosol concentration up to 107 per cm3. For particles with preexisting <span class="hlt">charge</span> of +1, 0, and −1, the measured <span class="hlt">charge</span> distributions agreed well with the theoretical distributions within the range of experimental and theoretical uncertainties. The transmission efficiency of the charger was measured to be 80% for 10 nm particles (at 0.3 L/min and 5 μA corona current) and increased with increasing diameter beyond this size. Measurement of uncharged fractions at various combinations of positive and <span class="hlt">negative</span> corona currents showed the charger performance to be insensitive to fluctuations in corona current. Ion concentrations under positive and <span class="hlt">negative</span> unipolar operation were estimated to be 8.2 × 107 and 3.37 × 108 cm−3 for positive and <span class="hlt">negative</span> ions; the n·t product value under positive corona operation was independently estimated to be 8.5 × 105 s/cm3. The ion concentration estimates indicate the charger to be capable of “neutralizing” typical atmospheric and industrial aerosols in most measurement applications. The miniature size, simple and robust operation makes the charger suitable for portable mobility spectrometers. PMID:26512158</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26512158','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26512158"><span>Miniature Dual-Corona Ionizer for Bipolar <span class="hlt">Charging</span> of Aerosol.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Qi, Chaolong; Kulkarni, Pramod</p> <p>2013-01-01</p> <p>A corona-based bipolar charger has been developed for use in compact, field-portable mobility size spectrometers. The charger employs an aerosol flow cavity exposed to two corona ionizers producing ions of opposite polarity. Each corona ionizer houses two electrodes in parallel needle-mesh configuration and is operated at the same magnitude of corona current. Experimental measurement of detailed <span class="hlt">charge</span> distribution of near-monodisperse particles of different diameter in the submicrometer size range showed that the charger is capable of producing well-defined, consistent bipolar <span class="hlt">charge</span> distributions for flow rates up to 1.5 L/min and aerosol concentration up to 10 7 per cm 3 . For particles with preexisting <span class="hlt">charge</span> of +1, 0, and -1, the measured <span class="hlt">charge</span> distributions agreed well with the theoretical distributions within the range of experimental and theoretical uncertainties. The transmission efficiency of the charger was measured to be 80% for 10 nm particles (at 0.3 L/min and 5 μ A corona current) and increased with increasing diameter beyond this size. Measurement of uncharged fractions at various combinations of positive and <span class="hlt">negative</span> corona currents showed the charger performance to be insensitive to fluctuations in corona current. Ion concentrations under positive and <span class="hlt">negative</span> unipolar operation were estimated to be 8.2 × 10 7 and 3.37 × 10 8 cm -3 for positive and <span class="hlt">negative</span> ions; the n · t product value under positive corona operation was independently estimated to be 8.5 × 10 5 s/cm 3 . The ion concentration estimates indicate the charger to be capable of "neutralizing" typical atmospheric and industrial aerosols in most measurement applications. The miniature size, simple and robust operation makes the charger suitable for portable mobility spectrometers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ApPhL.111e3503L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ApPhL.111e3503L"><span>Insight into the split and asymmetry of <span class="hlt">charge</span> distribution in biased M-structure superlattice</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liu, Lu; Bi, Han; Zhao, Yunhao; Zhao, Xuebing; Han, Xi; Wang, Guowei; Xu, Yingqiang; Li, Yuesheng; Che, Renchao</p> <p>2017-07-01</p> <p>The <span class="hlt">charge</span> distribution in real space of an insertion variant based on an InAs/GaSb superlattice for an infrared detector is illustrated by in situ electron microscopy. The localization split of positive <span class="hlt">charge</span> can be directly observed in the InAs/GaSb/AlSb/GaSb superlattice (M-structure) rather than in the InAs/GaSb superlattice. With the applied bias increasing from 0 to 4.5 V, the double peaks of positive <span class="hlt">charge</span> density become asymmetrical gradually, with the peak integral ratio ranging from 1.13 to 2.54. Simultaneously, the <span class="hlt">negative</span> <span class="hlt">charges</span> move along the direction of the <span class="hlt">negative</span> electric field. Without inserting the AlSb layer, the <span class="hlt">charge</span> inversion occurs in both the hole wells and the electron wells of the InAs/GaSb superlattice under high bias. Such a discrepancy between the M-structure superlattice and the traditional superlattice suggests an effective reduction of tunneling probability of the M-structure design. Our result is of great help to understand the carrier immigration mechanism of the superlattice-based infrared detector.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19790035065&hterms=uv+laser&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Duv%2Blaser','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19790035065&hterms=uv+laser&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Duv%2Blaser"><span>Gain measurements of the Ca-Xe <span class="hlt">charge</span> exchange system. [for UV lasers</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Michels, C. J.; Chubb, D. L.</p> <p>1978-01-01</p> <p><span class="hlt">Charge</span>-exchange-pumped Ca(+) was studied for possible positive laser gain at 370.6 and 315.9 nm using an Xe MPD arc as the Xe(+) source. The present paper describes the MPD arc, the calcium injection system, the diagnostics for gain, and spontaneous emission measurements and results. No positive gain measurements were observed. A small Xe-Ca <span class="hlt">charge</span> exchange cross section compared to He-metal laser systems <span class="hlt">charge</span> exchange cross sections is the most probable reason why the result was <span class="hlt">negative</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3123086','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3123086"><span><span class="hlt">Charge</span> Requirements for Proton Gradient-driven Translocation of Anthrax Toxin*</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Brown, Michael J.; Thoren, Katie L.; Krantz, Bryan A.</p> <p>2011-01-01</p> <p>Anthrax lethal toxin is used as a model system to study protein translocation. The toxin is composed of a translocase channel, called protective antigen (PA), and an enzyme, called lethal factor (LF). A proton gradient (ΔpH) can drive LF unfolding and translocation through PA channels; however, the mechanism of ΔpH-mediated force generation, substrate unfolding, and establishment of directionality are poorly understood. One recent hypothesis suggests that the ΔpH may act through changes in the protonation state of residues in the substrate. Here we report the <span class="hlt">charge</span> requirements of LF's amino-terminal binding domain (LFN) using planar lipid bilayer electrophysiology. We found that acidic residues are required in LFN to utilize a proton gradient for translocation. Constructs lacking <span class="hlt">negative</span> <span class="hlt">charges</span> in the unstructured presequence of LFN translocate independently of the ΔpH driving force. Acidic residues markedly increase the rate of ΔpH-driven translocation, and the presequence is optimized in its natural acidic residue content for efficient ΔpH-driven unfolding and translocation. We discuss a ΔpH-driven <span class="hlt">charge</span> state Brownian ratchet mechanism for translocation, where glutamic and aspartic acid residues in the substrate are the “molecular teeth” of the ratchet. Our Brownian ratchet model includes a mechanism for unfolding and a novel role for positive <span class="hlt">charges</span>, which we propose chaperone <span class="hlt">negative</span> <span class="hlt">charges</span> through the PA channel during ΔpH translocation. PMID:21507946</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26932111','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26932111"><span>Overview of the <span class="hlt">negative</span> ion based neutral beam injectors for ITER.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Schunke, B; Boilson, D; Chareyre, J; Choi, C-H; Decamps, H; El-Ouazzani, A; Geli, F; Graceffa, J; Hemsworth, R; Kushwah, M; Roux, K; Shah, D; Singh, M; Svensson, L; Urbani, M</p> <p>2016-02-01</p> <p>The ITER baseline foresees 2 Heating Neutral Beams (HNB's) based on 1 MeV 40 A D(-) <span class="hlt">negative</span> ion accelerators, each capable of delivering 16.7 MW of deuterium atoms to the DT plasma, with an optional 3rd HNB injector foreseen as a possible upgrade. In <span class="hlt">addition</span>, a dedicated diagnostic neutral beam will be injecting ≈22 A of H(0) at 100 keV as the probe beam for <span class="hlt">charge</span> exchange recombination spectroscopy. The integration of the injectors into the ITER plant is nearly finished necessitating only refinements. A large number of components have passed the final design stage, manufacturing has started, and the essential test beds-for the prototype route chosen-will soon be ready to start.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013CeMDA.115..281M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013CeMDA.115..281M"><span>Dust motions in quasi-statically <span class="hlt">charged</span> binary asteroid systems</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Maruskin, Jared M.; Bellerose, Julie; Wong, Macken; Mitchell, Lara; Richardson, David; Mathews, Douglas; Nguyen, Tri; Ganeshalingam, Usha; Ma, Gina</p> <p>2013-03-01</p> <p>In this paper, we discuss dust motion and investigate possible mass transfer of <span class="hlt">charged</span> particles in a binary asteroid system, in which the asteroids are electrically <span class="hlt">charged</span> due to solar radiation. The surface potential of the asteroids is assumed to be a piecewise function, with positive potential on the sunlit half and <span class="hlt">negative</span> potential on the shadow half. We derive the nonautonomous equations of motion for <span class="hlt">charged</span> particles and an analytic representation for their lofting conditions. Particle trajectories and temporary relative equilibria are examined in relation to their moving forbidden regions, a concept we define and discuss. Finally, we use a Monte Carlo simulation for a case study on mass transfer and loss rates between the asteroids.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20690607','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20690607"><span>Surface-<span class="hlt">charge</span>-dependent cell localization and cytotoxicity of cerium oxide nanoparticles.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Asati, Atul; Santra, Santimukul; Kaittanis, Charalambos; Perez, J Manuel</p> <p>2010-09-28</p> <p>Cerium oxide nanoparticles (nanoceria) have shown great potential as antioxidant and radioprotective agents for applications in cancer therapy. Recently, various polymer-coated nanoceria preparations have been developed to improve their aqueous solubility and allow for surface functionalization of these nanoparticles. However, the interaction of polymer-coated nanoceria with cells, their uptake mechanism, and subcellular localization are poorly understood. Herein, we engineered polymer-coated cerium oxide nanoparticles with different surface <span class="hlt">charges</span> (positive, <span class="hlt">negative</span>, and neutral) and studied their internalization and toxicity in normal and cancer cell lines. The results showed that nanoceria with a positive or neutral <span class="hlt">charge</span> enters most of the cell lines studied, while nanoceria with a <span class="hlt">negative</span> <span class="hlt">charge</span> internalizes mostly in the cancer cell lines. Moreover, upon entry into the cells, nanoceria is localized to different cell compartments (e.g., cytoplasm and lysosomes) depending on the nanoparticle's surface <span class="hlt">charge</span>. The internalization and subcellular localization of nanoceria plays a key role in the nanoparticles' cytotoxicity profile, exhibiting significant toxicity when they localize in the lysosomes of the cancer cells. In contrast, minimal toxicity is observed when they localize into the cytoplasm or do not enter the cells. Taken together, these results indicate that the differential surface-<span class="hlt">charge</span>-dependent localization of nanoceria in normal and cancer cells plays a critical role in the nanoparticles' toxicity profile.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013RuPhJ..56..878G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013RuPhJ..56..878G"><span><span class="hlt">Negative</span> <span class="hlt">Charged</span> Pion Production on a Deuteron by Quasi-Real Photons</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gauzshtein, V. V.; Dusaev, R. R.; Loginov, A. Yu.; Nikolenko, D. M.; Sidorov, A. A.; Stibunov, V. N.</p> <p>2013-12-01</p> <p>Experimental differential cross sections of photoproduction of <span class="hlt">negative</span> pions on a deuteron have been obtained as functions of the polar angle of emission of π- mesons. A comparison is made of the measured cross sections with the results of calculations in a model that takes account the interaction in the final state of the reaction.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008AGUFMAE11A0288Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008AGUFMAE11A0288Y"><span>Evidence of <span class="hlt">negative</span> leaders which precede fast rise ICC pulses of upward</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yoshida, S.; Akita, M.; Morimoto, T.; Ushio, T.; Kawasaki, Z.; Wang, D.; Takagi, N.</p> <p>2008-12-01</p> <p>During winter thunderstorm season in Japan, a lightning observation campaign was conducted with using a VHF broadband digital interferometer (DITF), a capacitive antenna, and Rogowski coils to study the <span class="hlt">charge</span> transfer mechanism associated with ICC pulses of upward lightning. All the detection systems recorded one upward <span class="hlt">negative</span> lightning stroke hitting a lightning protection tower. The upward lightning consists of only the Initial Stage (IS) with one upward positive leader and six ICC pulses. The six ICC pulses are sub-classified clearly into two types according to current pulse shapes. The type 1 ICC pulses have a higher geometric mean (GM) current peak of 17 kA and a shorter GM 10-90% risetime of 8.9 μs, while the type 2 ICC pulses have a lower GM current peak of 0.34 kA and longer GM 10-90% risetime of 55 μs. The type 1 ICC pulses have the preceding <span class="hlt">negative</span> leaders connecting to the channel of the continuing current, while the type 2 ICC pulses have no clear preceding <span class="hlt">negative</span> leader. These <span class="hlt">negative</span> leaders prior to the type 1 ICC pulses probably caused the current increases of the ICC pulses, which means that the <span class="hlt">negative</span> leaders created the channels for the ICC pulses. The height of the space <span class="hlt">charge</span> transferred by one of the type 1 ICC pulses was estimated about 700 m above sea level at most. This observation result is the first evidence to show explicitly the existence of the <span class="hlt">negative</span> leaders prior to the fast rise ICC pulse. Furthermore, the result shows that space <span class="hlt">charge</span> could exist at a low attitude such as 700 m above sea level. This fact is one of the reasons why upward lightning occurs even from rather low structures during winter thunderstorm season in Japan.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvD..97e5003M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvD..97e5003M"><span>Probing new <span class="hlt">charged</span> scalars with neutrino trident production</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Magill, Gabriel; Plestid, Ryan</p> <p>2018-03-01</p> <p>We investigate the possibility of using neutrino trident production to probe leptophilic <span class="hlt">charged</span> scalars at future high intensity neutrino experiments. We show that under specific assumptions, this production process can provide competitive sensitivity for generic <span class="hlt">charged</span> scalars as compared to common existing bounds. We also investigate how the recently proposed mixed-flavor production—where the two oppositely <span class="hlt">charged</span> leptons in the final state need not be muon flavored—can give a 20%-50% increase in sensitivity for certain configurations of new physics couplings as compared to traditional trident modes. We then categorize all renormalizable leptophilic scalar extensions based on their representation under SU (2 )×U (1 ), and discuss the Higgs triplet and Zee-Babu models as explicit UV realizations. We find that the inclusion of <span class="hlt">additional</span> doubly <span class="hlt">charged</span> scalars and the need to reproduce neutrino masses make trident production uncompetitive with current bounds for these specific UV completions. Our work represents the first application of neutrino trident production to study <span class="hlt">charged</span> scalars. <span class="hlt">Additionally</span>, it is the first application of mixed-flavor trident production to study physics beyond the standard model more generally.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AIPC.1971d0020D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AIPC.1971d0020D"><span>Electric vehicle <span class="hlt">charging</span> station quantity forecasting model</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dong, Yingshuai</p> <p>2018-06-01</p> <p>For both environmental and economic reasons, there is global interest in reducing the use of fossil fuels, including gasoline for cars. Whether motivated by the environment or by the economics, consumers are starting to migrate to electric vehicles. Tesla currently offers two types of <span class="hlt">charging</span> stations: (1) destination <span class="hlt">charging</span> designed for <span class="hlt">charging</span> for several hours at a time or even overnight; and (2) supercharging designed for longer road trips to provide up to 170 miles of range in as little as 30 minutes of <span class="hlt">charging</span>. These stations are in <span class="hlt">addition</span> to at-home <span class="hlt">charging</span> used by many Tesla owners who have a personal garage or a driveway with power. Based on private car survey data from the NHTS in the United States, this article predicts the number of <span class="hlt">charging</span> stations required if everyone is using an electric passenger car across the United States.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22777854','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22777854"><span>Electrostatic interactions play an essential role in the binding of oleic acid with α-lactalbumin in the HAMLET-like complex: a study using <span class="hlt">charge</span>-specific chemical modifications.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Xie, Yongjing; Min, Soyoung; Harte, Níal P; Kirk, Hannah; O'Brien, John E; Voorheis, H Paul; Svanborg, Catharina; Hun Mok, K</p> <p>2013-01-01</p> <p>Human α-lactalbumin made lethal to tumor cells (HAMLET) and its analogs are partially unfolded protein-oleic acid (OA) complexes that exhibit selective tumoricidal activity normally absent in the native protein itself. To understand the nature of the interaction between protein and OA moieties, <span class="hlt">charge</span>-specific chemical modifications of lysine side chains involving citraconylation, acetylation, and guanidination were employed and the biophysical and biological properties were probed. Upon converting the original positively-<span class="hlt">charged</span> lysine residues to <span class="hlt">negatively-charged</span> citraconyl or neutral acetyl groups, the binding of OA to protein was eliminated, as were any cytotoxic activities towards osteosarcoma cells. Retention of the positive <span class="hlt">charges</span> by converting lysine residues to homoarginine groups (guanidination); however, yielded unchanged binding of OA to protein and identical tumoricidal activity to that displayed by the wild-type α-lactalbumin-oleic acid complex. With the <span class="hlt">addition</span> of OA, the wild-type and guanidinated α-lactalbumin proteins underwent substantial conformational changes, such as partial unfolding, loss of tertiary structure, but retention of secondary structure. In contrast, no significant conformational changes were observed in the citraconylated and acetylated α-lactalbumins, most likely because of the absence of OA binding. These results suggest that electrostatic interactions between the positively-<span class="hlt">charged</span> basic groups on α-lactalbumin and the <span class="hlt">negatively-charged</span> carboxylate groups on OA molecules play an essential role in the binding of OA to α-lactalbumin and that these interactions appear to be as important as hydrophobic interactions. Copyright © 2012 Wiley Periodicals, Inc.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ApSS..428..870N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ApSS..428..870N"><span>Tridodecylamine, an efficient <span class="hlt">charge</span> control agent in non-polar media for electrophoretic inks application</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Noel, Amélie; Mirbel, Déborah; Cloutet, Eric; Fleury, Guillaume; Schatz, Christophe; Navarro, Christophe; Hadziioannou, Georges; CyrilBrochon</p> <p>2018-01-01</p> <p>In order to obtain efficient electrophoretic inks, Tridodecylamine (Dod3N), has been studied as <span class="hlt">charge</span> control agent (CCA) in a non-polar paraffin solvent (Isopar G) for various inorganic pigments (TiO2 and Fe2O3). All hydrophobic mineral oxides, i.e. treated with octyltrimethoxysilane (C8) or dodecyltrimethoxysilane (C12), were found to be <span class="hlt">negatively</span> <span class="hlt">charged</span> in presence of Dod3N. The electrophoretic mobilities of inorganic pigments seemed to be strongly dependent of their isoelectric point (IEP) and also of the concentration of dod3N with an optimum range between 10 and 20 mM depending on the pigments. Finally, an electrophoretic ink constituted of hydrophobic mineral oxides in presence of Dod3N was tested in a device. Its efficiency as <span class="hlt">charge</span> control agent to <span class="hlt">negatively</span> <span class="hlt">charge</span> hydrophobic particles was confirmed through good optical properties and fast response time (220 ms at 200 kV m-1).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010PhDT........82V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010PhDT........82V"><span>Oppositely <span class="hlt">charged</span> colloids out of equilibrium</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vissers, T.</p> <p>2010-11-01</p> <p>Colloids are particles with a size in the range of a few nanometers up to several micrometers. Similar to atomic and molecular systems, they can form gases, liquids, solids, gels and glasses. Colloids can be used as model systems because, unlike molecules, they are sufficiently large to be studied directly with light microscopy and move sufficiently slow to study their dynamics. In this thesis, we study binary systems of polymethylmethacrylate (PMMA) colloidal particles suspended in low-polar solvent mixtures. Since the ions can still partially dissociate, a surface <span class="hlt">charge</span> builds up which causes electrostatic interactions between the colloids. By carefully tuning the conditions inside the suspension, we make two kinds of particles oppositely <span class="hlt">charged</span>. To study our samples, we use Confocal Laser Scanning Microscopy (CLSM). The positively and <span class="hlt">negatively</span> <span class="hlt">charged</span> particles can be distinguished by a different fluorescent dye. Colloids constantly experience a random motion resulting from random kicks of surrounding solvent molecules. When the attractions between the oppositely <span class="hlt">charged</span> particles are weak, the particles can attach and detach many times and explore a lot of possible configurations and the system can reach thermodynamic equilibrium. For example, colloidal ‘ionic’ crystals consisting of thousands to millions of particles can form under the right conditions. When the attractions are strong, the system can become kinetically trapped inside a gel-like state. We observe that when the interactions change again, crystals can even emerge again from this gel-like phase. By using local order parameters, we quantitatively study the crystallization of colloidal particles and identify growth defects inside the crystals. We also study the effect of gravity on the growth of ionic crystals by using a rotating stage. We find that sedimentation can completely inhibit crystal growth and plays an important role in crystallization from the gel-like state. The surface</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23534618','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23534618"><span>Effect of surface <span class="hlt">charge</span> density on the affinity of oxide nanoparticles for the vapor-water interface.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Brown, Matthew A; Duyckaerts, Nicolas; Redondo, Amaia Beloqui; Jordan, Inga; Nolting, Frithjof; Kleibert, Armin; Ammann, Markus; Wörner, Hans Jakob; van Bokhoven, Jeroen A; Abbas, Zareen</p> <p>2013-04-23</p> <p>Using in-situ X-ray photoelectron spectroscopy at the vapor-water interface, the affinity of nanometer-sized silica colloids to adsorb at the interface is shown to depend on colloid surface <span class="hlt">charge</span> density. In aqueous suspensions at pH 10 corrected Debye-Hückel theory for surface complexation calculations predict that smaller silica colloids have increased <span class="hlt">negative</span> surface <span class="hlt">charge</span> density that originates from enhanced screening of deprotonated silanol groups (≡Si-O(-)) by counterions in the condensed ion layer. The increased <span class="hlt">negative</span> surface <span class="hlt">charge</span> density results in an electrostatic repulsion from the vapor-water interface that is seen to a lesser extent for larger particles that have a reduced <span class="hlt">charge</span> density in the XPS measurements. We compare the results and interpretation of the in-situ XPS and corrected Debye-Hückel theory for surface complexation calculations with traditional surface tension measurements. Our results show that controlling the surface <span class="hlt">charge</span> density of colloid particles can regulate their adsorption to the interface between two dielectrics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015Icar..258..109P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015Icar..258..109P"><span>Electron-molecule chemistry and <span class="hlt">charging</span> processes on organic ices and Titan's icy aerosol surrogates</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pirim, C.; Gann, R. D.; McLain, J. L.; Orlando, T. M.</p> <p>2015-09-01</p> <p>Electron-induced polymerization processes and <span class="hlt">charging</span> events that can occur within Titan's atmosphere or on its surface were simulated using electron irradiation and dissociative electron attachment (DEA) studies of nitrogen-containing organic condensates. The DEA studies probe the desorption of H- from hydrogen cyanide (HCN), acetonitrile (CH3CN), and aminoacetonitrile (NH2CH2CN) ices, as well as from synthesized tholin materials condensed or deposited onto a graphite substrate maintained at low temperature (90-130 K). The peak cross sections for H- desorption during low-energy (3-15 eV) electron irradiation were measured and range from 3 × 10-21 to 2 × 10-18 cm2. Chemical and structural transformations of HCN ice upon 2 keV electron irradiation were investigated using X-ray photoelectron and Fourier-transform infrared spectroscopy techniques. The electron-beam processed materials displayed optical properties very similar to tholins produced by conventional discharge methods. Electron and <span class="hlt">negative</span> ion trapping lead to 1011 <span class="hlt">charges</span> cm-2 on a flat surface which, assuming a radius of 0.05 μm for Titan aerosols, is ∼628 <span class="hlt">charges</span>/radius (in μm). The facile <span class="hlt">charge</span> trapping indicates that electron interactions with nitriles and complex tholin-like molecules could affect the conductivity of Titan's atmosphere due to the formation of large <span class="hlt">negative</span> ion complexes. These <span class="hlt">negatively</span> <span class="hlt">charged</span> complexes can also precipitate onto Titan's surface and possibly contribute to surface reactions and the formation of dunes.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li class="active"><span>20</span></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_20 --> <div id="page_21" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li class="active"><span>21</span></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="401"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28491052','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28491052"><span>Receptor-Mediated Melanoma Targeting with Radiolabeled α-Melanocyte-Stimulating Hormone: Relevance of the Net <span class="hlt">Charge</span> of the Ligand.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Bapst, Jean-Philippe; Eberle, Alex N</p> <p>2017-01-01</p> <p>A majority of melanotic and amelanotic melanomas overexpress melanocortin type 1 receptors (MC1Rs) for α-melanocyte-stimulating hormone. Radiolabeled linear or cyclic analogs of α-MSH have a great potential as diagnostic or therapeutic tools for the management of malignant melanoma. Compounds such as [ 111 In]DOTA-NAP-amide exhibit high affinity for the MC1R in vitro , good tumor uptake in vivo , but they may suffer from relatively high kidney uptake and retention in vivo . We have shown previously that the introduction of <span class="hlt">negative</span> <span class="hlt">charges</span> into radiolabeled DOTA-NAP-amide peptide analogs may enhance their excretion and reduce kidney retention. To address the question of where to place <span class="hlt">negative</span> <span class="hlt">charges</span> within the ligand, we have extended these studies by designing two novel peptides, Ac-Nle-Asp-His-d-Phe-Arg-Trp-Gly-Lys(DOTA)-d-Asp-d-Asp-OH (DOTA-NAP-d-Asp-d-Asp) with three <span class="hlt">negative</span> <span class="hlt">charges</span> at the C -terminal end (overall net <span class="hlt">charge</span> of the molecule -2) and DOTA-Gly-Tyr(P)-Nle-Asp-His-d-Phe-Arg-Trp-NH 2 (DOTA-Phospho-MSH 2-9 ) with two <span class="hlt">negative</span> <span class="hlt">charges</span> in the N -terminal region (net <span class="hlt">charge</span> -1). The former peptide showed markedly reduced receptor affinity and biological activity by >10-fold compared to DOTA-NAP-amide as reference compound, and the latter peptide displayed similar bioactivity and receptor affinity as the reference compound. The uptake by melanoma tumor tissue of [ 111 In]DOTA-Phospho-MSH 2-9 was 7.33 ± 0.47 %ID/g 4 h after injection, i.e., almost equally high as with [ 111 In]DOTA-NAP-amide. The kidney retention was 2.68 ± 0.18 %ID/g 4 h after injection and hence 44% lower than that of [ 111 In]DOTA-NAP-amide. Over an observation period from 4 to 48 h, the tumor-to-kidney ratio of [ 111 In]DOTA-Phospho-MSH 2-9 was 35% more favorable than that of the reference compound. In a comparison of DOTA-NAP-d-Asp-d-Asp, DOTA-Phospho-MSH 2-9 and DOTA-NAP-amide with five previously published analogs of DOTA-NAP-amide that altogether cover a</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5405074','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5405074"><span>Receptor-Mediated Melanoma Targeting with Radiolabeled α-Melanocyte-Stimulating Hormone: Relevance of the Net <span class="hlt">Charge</span> of the Ligand</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Bapst, Jean-Philippe; Eberle, Alex N.</p> <p>2017-01-01</p> <p>A majority of melanotic and amelanotic melanomas overexpress melanocortin type 1 receptors (MC1Rs) for α-melanocyte-stimulating hormone. Radiolabeled linear or cyclic analogs of α-MSH have a great potential as diagnostic or therapeutic tools for the management of malignant melanoma. Compounds such as [111In]DOTA-NAP-amide exhibit high affinity for the MC1R in vitro, good tumor uptake in vivo, but they may suffer from relatively high kidney uptake and retention in vivo. We have shown previously that the introduction of <span class="hlt">negative</span> <span class="hlt">charges</span> into radiolabeled DOTA-NAP-amide peptide analogs may enhance their excretion and reduce kidney retention. To address the question of where to place <span class="hlt">negative</span> <span class="hlt">charges</span> within the ligand, we have extended these studies by designing two novel peptides, Ac-Nle-Asp-His-d-Phe-Arg-Trp-Gly-Lys(DOTA)-d-Asp-d-Asp-OH (DOTA-NAP-d-Asp-d-Asp) with three <span class="hlt">negative</span> <span class="hlt">charges</span> at the C-terminal end (overall net <span class="hlt">charge</span> of the molecule −2) and DOTA-Gly-Tyr(P)-Nle-Asp-His-d-Phe-Arg-Trp-NH2 (DOTA-Phospho-MSH2-9) with two <span class="hlt">negative</span> <span class="hlt">charges</span> in the N-terminal region (net <span class="hlt">charge</span> −1). The former peptide showed markedly reduced receptor affinity and biological activity by >10-fold compared to DOTA-NAP-amide as reference compound, and the latter peptide displayed similar bioactivity and receptor affinity as the reference compound. The uptake by melanoma tumor tissue of [111In]DOTA-Phospho-MSH2-9 was 7.33 ± 0.47 %ID/g 4 h after injection, i.e., almost equally high as with [111In]DOTA-NAP-amide. The kidney retention was 2.68 ± 0.18 %ID/g 4 h after injection and hence 44% lower than that of [111In]DOTA-NAP-amide. Over an observation period from 4 to 48 h, the tumor-to-kidney ratio of [111In]DOTA-Phospho-MSH2-9 was 35% more favorable than that of the reference compound. In a comparison of DOTA-NAP-d-Asp-d-Asp, DOTA-Phospho-MSH2-9 and DOTA-NAP-amide with five previously published analogs of DOTA-NAP-amide that altogether cover a range of peptides</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20130001853','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20130001853"><span>Extreme Spacecraft <span class="hlt">Charging</span> in Polar Low Earth Orbit</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Colson, Andrew D.; Minow, Joseph I.; NeergaardParker, Linda</p> <p>2012-01-01</p> <p>Spacecraft in low altitude, high inclination (including sun-synchronous) orbits are widely used for remote sensing of the Earth's land surface and oceans, monitoring weather and climate, communications, scientific studies of the upper atmosphere and ionosphere, and a variety of other scientific, commercial, and military applications. These systems episodically <span class="hlt">charge</span> to frame potentials in the kilovolt range when exposed to space weather environments characterized by a high flux of energetic (10 s kilovolt) electrons in regions of low background plasma density which is similar in some ways to the space weather conditions in geostationary orbit responsible for spacecraft <span class="hlt">charging</span> to kilovolt levels. We first review the physics of space environment interactions with spacecraft materials that control auroral <span class="hlt">charging</span> rates and the anticipated maximum potentials that should be observed on spacecraft surfaces during disturbed space weather conditions. We then describe how the theoretical values compare to the observational history of extreme <span class="hlt">charging</span> in auroral environments. Finally, a set of extreme DMSP <span class="hlt">charging</span> events are described varying in maximum <span class="hlt">negative</span> frame potential from 0.6 kV to 2 kV, focusing on the characteristics of the <span class="hlt">charging</span> events that are of importance both to the space system designer and to spacecraft operators. The goal of the presentation is to bridge the gap between scientific studies of auroral <span class="hlt">charging</span> and the need for engineering teams to understand how space weather impacts both spacecraft design and operations for vehicles on orbital trajectories that traverse auroral <span class="hlt">charging</span> environments.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21410204','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21410204"><span>Long-range interaction between heterogeneously <span class="hlt">charged</span> membranes.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Jho, Y S; Brewster, R; Safran, S A; Pincus, P A</p> <p>2011-04-19</p> <p>Despite their neutrality, surfaces or membranes with equal amounts of positive and <span class="hlt">negative</span> <span class="hlt">charge</span> can exhibit long-range electrostatic interactions if the surface <span class="hlt">charge</span> is heterogeneous; this can happen when the surface <span class="hlt">charges</span> form finite-size domain structures. These domains can be formed in lipid membranes where the balance of the different ranges of strong but short-ranged hydrophobic interactions and longer-ranged electrostatic repulsion result in a finite, stable domain size. If the domain size is large enough, oppositely <span class="hlt">charged</span> domains in two opposing surfaces or membranes can be strongly correlated by the electrostatic interactions; these correlations give rise to an attractive interaction of the two membranes or surfaces over separations on the order of the domain size. We use numerical simulations to demonstrate the existence of strong attractions at separations of tens of nanometers. Large line tensions result in larger domains but also increase the <span class="hlt">charge</span> density within the domain. This promotes correlations and, as a result, increases the intermembrane attraction. On the other hand, increasing the salt concentration increases both the domain size and degree of domain anticorrelation, but the interactions are ultimately reduced due to increased screening. The result is a decrease in the net attraction as salt concentration is increased. © 2011 American Chemical Society</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/910593-charge-associated-effects-fullerene-derivatives-microbialstructural-integrity-central-metabolism','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/910593-charge-associated-effects-fullerene-derivatives-microbialstructural-integrity-central-metabolism"><span><span class="hlt">Charge</span>-associated effects of fullerene derivatives on microbialstructural integrity and central metabolism</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Tang, Yinjie J.; Ashcroft, Jared M.; Chen, Ding</p> <p>2007-01-23</p> <p>The effects of four types of fullerene compounds (C60,C60-OH, C60-COOH, C60-NH2) were examined on two model microorganisms(Escherichia coli W3110 and Shewanella oneidensis MR-1). Positivelycharged C60-NH2 at concentrations as low as 10 mg/L inhibited growth andreduced substrate uptake for both microorganisms. Scanning ElectronMicroscopy (SEM) revealed damage to cellular structures.Neutrally-<span class="hlt">charged</span> C60 and C60-OH had mild <span class="hlt">negative</span> effects on S.oneidensis MR-1, whereas the <span class="hlt">negatively-charged</span> C60-COOH did not affecteither microorganism s growth. The effect of fullerene compounds onglobal metabolism was further investigated using [3-13C]L-lactateisotopic labeling, which tracks perturbations to metabolic reaction ratesin bacteria by examining the change in the isotopic labeling pattern inthe resultingmore » metabolites (often amino acids).1-3 The 13C isotopomeranalysis from all fullerene-exposed cultures revealed no significantdifferences in isotopomer distributions from unstressed cells. Thisresult indicates that microbial central metabolism is robust toenvironmental stress inflicted by fullerene nanoparticles. In <span class="hlt">addition</span>,although C60-NH2 compounds caused mechanical stress on the cell wall ormembrane, both S. oneidensis MR-1 and E. coli W3110 can efficientlyalleviate such stress by cell aggregation and precipitation of the toxicnanoparticles. The results presented here favor the hypothesis thatfullerenes cause more membrane stress4, 5, 6 than perturbation to energymetabolism7« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20130003217','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20130003217"><span>Extreme Spacecraft <span class="hlt">Charging</span> in Polar Low Earth Orbit</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Colson, Andrew D.; Minow, Joseph I.; Parker, L. Neergaard</p> <p>2012-01-01</p> <p>Spacecraft in low altitude, high inclination (including sun -synchronous) orbits are widely used for remote sensing of the Earth fs land surface and oceans, monitoring weather and climate, communications, scientific studies of the upper atmosphere and ionosphere, and a variety of other scientific, commercial, and military applications. These systems episodically <span class="hlt">charge</span> to frame potentials in the kilovolt range when exposed to space weather environments characterized by a high flux of energetic (approx.10 fs kilovolt) electrons in regions of low background plasma density. Auroral <span class="hlt">charging</span> conditions are similar in some ways to the space weather conditions in geostationary orbit responsible for spacecraft <span class="hlt">charging</span> to kilovolt levels. We first review the physics of space environment interactions with spacecraft materials that control auroral <span class="hlt">charging</span> rates and the anticipated maximum potentials that should be observed on spacecraft surfaces during disturbed space weather conditions. We then describe how the theoretical values compare to the observational history of extreme <span class="hlt">charging</span> in auroral environments. Finally, a set of extreme DMSP <span class="hlt">charging</span> events are described varying in maximum <span class="hlt">negative</span> frame potential from approx.0.6 kV to approx.2 kV, focusing on the characteristics of the <span class="hlt">charging</span> events that are of importance both to the space system designer and to spacecraft operators. The goal of the presentation is to bridge the gap between scientific studies of auroral <span class="hlt">charging</span> and the need for engineering teams to understand how space weather impacts both spacecraft design and operations for vehicles on orbital trajectories that traverse auroral <span class="hlt">charging</span> environments.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010PhLA..374.1534G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010PhLA..374.1534G"><span>Dissociation of methane on the surface of <span class="hlt">charged</span> defective carbon nanotubes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Guo, Z. H.; Yan, X. H.; Xiao, Y.</p> <p>2010-03-01</p> <p>Based on the framework of density functional theory (CASTEP and DMOL 3 codes), we simulate the dissociation of methane (CH 4) molecule on the surface of <span class="hlt">charged</span> defective carbon nanotubes (CNTs). The results display that a <span class="hlt">charged</span> CNT with carbon (C) and molybdenum (Mo) dopants can effectively dissociate CH 4 molecule, and the adsorption strength of H and CH 3 can be controlled by the injected <span class="hlt">negative</span> <span class="hlt">charges</span>. Moreover, the barrier between the transition state (TS) and the reactant is 0.1014 eV, and a single imaginary frequency of -0.3 cm is found for the transition state structure.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016Nanos...810649I','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016Nanos...810649I"><span>Effective cytoplasmic release of siRNA from liposomal carriers by controlling the electrostatic interaction of siRNA with a <span class="hlt">charge</span>-invertible peptide, in response to cytoplasmic pH</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Itakura, Shoko; Hama, Susumu; Matsui, Ryo; Kogure, Kentaro</p> <p>2016-05-01</p> <p> effectively released via electrostatic repulsion of siRNA with <span class="hlt">negatively</span> <span class="hlt">charged</span> SAPSP at cytoplasmic pH (7.4). The condensed complex of siRNA and positively-<span class="hlt">charged</span> SAPSP at acidic pH (siRNA/SAPSP) was found to result in almost complete release of siRNA upon <span class="hlt">charge</span> inversion of SAPSP at pH 7.4, with the resultant <span class="hlt">negatively-charged</span> SAPSP having no undesirable interactions with endogenous mRNA. Moreover, liposomes encapsulating siRNA/SAPSP demonstrated knockdown efficiencies comparable to those of commercially available siRNA carriers. Taken together, SAPSP may be very useful as a siRNA condenser, as it facilitates effective cytoplasmic release of siRNA, and subsequent induction of specific RNAi effects. Electronic supplementary information (ESI) available: De-condensation of siRNA cores by <span class="hlt">addition</span> of heparin; time-lapse moving image of the siRNA release. See DOI: 10.1039/c5nr08365f</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title7-vol3/pdf/CFR-2010-title7-vol3-sec91-38.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title7-vol3/pdf/CFR-2010-title7-vol3-sec91-38.pdf"><span>7 CFR 91.38 - <span class="hlt">Additional</span> fees for appeal of analysis.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-01-01</p> <p>... 7 Agriculture 3 2010-01-01 2010-01-01 false <span class="hlt">Additional</span> fees for appeal of analysis. 91.38 Section... LABORATORY TESTING PROGRAMS SERVICES AND GENERAL INFORMATION Fees and <span class="hlt">Charges</span> § 91.38 <span class="hlt">Additional</span> fees for appeal of analysis. (a) The applicant for appeal sample testing will be <span class="hlt">charged</span> a fee at the hourly rate...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title7-vol3/pdf/CFR-2013-title7-vol3-sec91-38.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title7-vol3/pdf/CFR-2013-title7-vol3-sec91-38.pdf"><span>7 CFR 91.38 - <span class="hlt">Additional</span> fees for appeal of analysis.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2013&page.go=Go">Code of Federal Regulations, 2013 CFR</a></p> <p></p> <p>2013-01-01</p> <p>... 7 Agriculture 3 2013-01-01 2013-01-01 false <span class="hlt">Additional</span> fees for appeal of analysis. 91.38 Section... LABORATORY TESTING PROGRAMS SERVICES AND GENERAL INFORMATION Fees and <span class="hlt">Charges</span> § 91.38 <span class="hlt">Additional</span> fees for appeal of analysis. (a) The applicant for appeal sample testing will be <span class="hlt">charged</span> a fee at the hourly rate...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1985PhDT........37T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1985PhDT........37T"><span><span class="hlt">Negatively</span> <span class="hlt">Charged</span> Hydrogen Production in a Multicusp Microwave Plasma</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Trow, John Robert</p> <p>1985-06-01</p> <p>High energy neutral beams are necessary for the continued development of magnetically confined fusion plasma devices. Neutral beams based on positive ions are not efficient at beam energies of 100 keV or above, however <span class="hlt">negative</span> ion based neutral beam systems are efficient, even at high beam energies. Volume production of H('-) has many advantages over the other methods, chiefly: simplicity of design and operation, and no need for alkalai metals. Since volume production requires a low electron temperature ((TURN)1 eV) but also requires molecular intermediates only formed by more energetic electrons (>20 eV), double plasma devices with a separate hot electron region are desirable. Therefore an experiment was undertaken to examine H('-) production by volume processes in a multicusp microwave discharge, part of the cusp field being enhanced to produce an ECR (electron cyclotron resonance), that would also isolate the hotter plasma formed there. This arrangement is analogous to the "magnetic filters" used in some other <span class="hlt">negative</span> ion sources. This work describes the experiment set up and the results obtained, which are a survey of the behavior of this type of device. Also included is a discussion of the volume processes associated with H('-) production including numerical estimates, based on the experimental measurements, which indicate H('-) production is by dissociative attachment of cold electrons to vibrationally excited hydrogen molecules, and loss is by mutual neutralization with positive ions. The experimental observations are consistent with this model. These are also the same mechanisms used in the models of Bacal and Hiskes. Since magnetic fields generated by samarium cobalt permanent magnets were an important part of this experiment a set of field calculations was undertaken and is included here as a separate chapter. This device is shown to be a viable scheme of H('-) (or D('-)) produc- tion and is worthy of further development. There are several more</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013ApJ...763...77M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013ApJ...763...77M"><span><span class="hlt">Charging</span> of Aggregate Grains in Astrophysical Environments</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ma, Qianyu; Matthews, Lorin S.; Land, Victor; Hyde, Truell W.</p> <p>2013-02-01</p> <p>The <span class="hlt">charging</span> of dust grains in astrophysical environments has been investigated with the assumption that these grains are homogeneous spheres. However, there is evidence which suggests that many grains in astrophysical environments are irregularly shaped aggregates. Recent studies have shown that aggregates acquire higher <span class="hlt">charge</span>-to-mass ratios due to their complex structures, which in turn may alter their subsequent dynamics and evolution. In this paper, the <span class="hlt">charging</span> of aggregates is examined including secondary electron emission and photoemission in <span class="hlt">addition</span> to primary plasma currents. The results show that the equilibrium <span class="hlt">charge</span> on aggregates can differ markedly from spherical grains with the same mass, but that the <span class="hlt">charge</span> can be estimated for a given environment based on structural characteristics of the grain. The "small particle effect" due to secondary electron emission is also important for de terming the <span class="hlt">charge</span> of micron-sized aggregates consisting of nano-sized particles.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28151684','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28151684"><span>Complexation of Polyelectrolyte Micelles with Oppositely <span class="hlt">Charged</span> Linear Chains.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kalogirou, Andreas; Gergidis, Leonidas N; Miliou, Kalliopi; Vlahos, Costas</p> <p>2017-03-02</p> <p>The formation of interpolyelectrolyte complexes (IPECs) from linear AB diblock copolymer precursor micelles and oppositely <span class="hlt">charged</span> linear homopolymers is studied by means of molecular dynamics simulations. All beads of the linear polyelectrolyte (C) are <span class="hlt">charged</span> with elementary quenched <span class="hlt">charge</span> +1e, whereas in the diblock copolymer only the solvophilic (A) type beads have quenched <span class="hlt">charge</span> -1e. For the same Bjerrum length, the ratio of positive to <span class="hlt">negative</span> <span class="hlt">charges</span>, Z +/- , of the mixture and the relative length of <span class="hlt">charged</span> moieties r determine the size of IPECs. We found a nonmonotonic variation of the size of the IPECs with Z +/- . For small Z +/- values, the IPECs retain the size of the precursor micelle, whereas at larger Z +/- values the IPECs decrease in size due to the contraction of the corona and then increase as the aggregation number of the micelle increases. The minimum size of the IPECs is obtained at lower Z +/- values when the length of the hydrophilic block of the linear diblock copolymer decreases. The aforementioned findings are in agreement with experimental results. At a smaller Bjerrum length, we obtain the same trends but at even smaller Z +/- values. The linear homopolymer <span class="hlt">charged</span> units are distributed throughout the corona.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19198289','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19198289"><span>Control of single-electron <span class="hlt">charging</span> of metallic nanoparticles onto amorphous silicon surface.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Weis, Martin; Gmucová, Katarína; Nádazdy, Vojtech; Capek, Ignác; Satka, Alexander; Kopáni, Martin; Cirák, Július; Majková, Eva</p> <p>2008-11-01</p> <p>Sequential single-electron <span class="hlt">charging</span> of iron oxide nanoparticles encapsulated in oleic acid/oleyl amine envelope and deposited by the Langmuir-Blodgett technique onto Pt electrode covered with undoped hydrogenated amorphous silicon film is reported. Single-electron <span class="hlt">charging</span> (so-called quantized double-layer <span class="hlt">charging</span>) of nanoparticles is detected by cyclic voltammetry as current peaks and the <span class="hlt">charging</span> effect can be switched on/off by the electric field in the surface region induced by the excess of <span class="hlt">negative</span>/positive <span class="hlt">charged</span> defect states in the amorphous silicon layer. The particular <span class="hlt">charge</span> states in amorphous silicon are created by the simultaneous application of a suitable bias voltage and illumination before the measurement. The influence of <span class="hlt">charged</span> states on the electric field in the surface region is evaluated by the finite element method. The single-electron <span class="hlt">charging</span> is analyzed by the standard quantized double layer model as well as two weak-link junctions model. Both approaches are in accordance with experiment and confirm single-electron <span class="hlt">charging</span> by tunnelling process at room temperature. This experiment illustrates the possibility of the creation of a voltage-controlled capacitor for nanotechnology.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21432659','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21432659"><span><span class="hlt">Negative</span> emotions can attenuate the influence of beliefs on logical reasoning.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Goel, Vinod; Vartanian, Oshin</p> <p>2011-01-01</p> <p>Although the influence of beliefs on logical reasoning is well documented, how emotions modulate the effect of beliefs during reasoning remains unexamined. We instructed participants to reason about syllogisms involving neutral or emotionally <span class="hlt">charged</span> content. We also manipulated the consistency of beliefs with logical validity. When content was neutral, participants exhibited the belief-bias effect observed in previous studies of reasoning. In contrast, when confronted with emotionally <span class="hlt">charged</span> content participants were less likely to be influenced by their beliefs. Our results suggest that under certain conditions <span class="hlt">negative</span> emotions can attenuate the influence of beliefs during logical reasoning. Drawing on the affect infusion model, we attribute this effect to a more vigilant, systematic scrutiny of beliefs in the presence of <span class="hlt">negative</span> emotions. © 2010 Psychology Press, an imprint of the Taylor & Francis Group, an Informa business</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22299657-plasmon-excitation-metal-slab-fast-point-charge-role-additional-boundary-conditions-quantum-hydrodynamic-model','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22299657-plasmon-excitation-metal-slab-fast-point-charge-role-additional-boundary-conditions-quantum-hydrodynamic-model"><span>Plasmon excitation in metal slab by fast point <span class="hlt">charge</span>: The role of <span class="hlt">additional</span> boundary conditions in quantum hydrodynamic model</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Zhang, Ying-Ying; Department of Applied Mathematics, University of Waterloo, Waterloo, Ontario N2L 3G1; An, Sheng-Bai</p> <p>2014-10-15</p> <p>We study the wake effect in the induced potential and the stopping power due to plasmon excitation in a metal slab by a point <span class="hlt">charge</span> moving inside the slab. Nonlocal effects in the response of the electron gas in the metal are described by a quantum hydrodynamic model, where the equation of electronic motion contains both a quantum pressure term and a gradient correction from the Bohm quantum potential, resulting in a fourth-order differential equation for the perturbed electron density. Thus, besides using the condition that the normal component of the electron velocity should vanish at the impenetrable boundary ofmore » the metal, a consistent inclusion of the gradient correction is shown to introduce two possibilities for an <span class="hlt">additional</span> boundary condition for the perturbed electron density. We show that using two different sets of boundary conditions only gives rise to differences in the wake potential at large distances behind the <span class="hlt">charged</span> particle. On the other hand, the gradient correction in the quantum hydrodynamic model is seen to cause a reduction in the depth of the potential well closest to the particle, and a reduction of its stopping power. Even for a particle moving in the center of the slab, we observe nonlocal effects in the induced potential and the stopping power due to reduction of the slab thickness, which arise from the gradient correction in the quantum hydrodynamic model.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5878943','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5878943"><span>The consequences of patient <span class="hlt">charges</span> for prescription drugs in Canada: a cross-sectional survey</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Law, Michael R.; Cheng, Lucy; Kolhatkar, Ashra; Goldsmith, Laurie J.; Morgan, Steven G.; Holbrook, Anne M.; Dhalla, Irfan A.</p> <p>2018-01-01</p> <p>Background: Many Canadians face substantial out-of-pocket <span class="hlt">charges</span> for prescription drugs. Prior work suggests that this causes some patients to not take their medications as prescribed; however, we have little understanding of whether <span class="hlt">charges</span> for prescription medicines lead patients to forego basic needs or to use more health care services. Our study aimed to quantify the consequences of patient <span class="hlt">charges</span> for medicines in Canada. Methods: As part of the 2016 Canadian Community Health Survey, we designed and fielded cross-sectional questions to 28 091 Canadians regarding prescription drug affordability, consequent use of health care services and trade-offs with other expenditures. We calculated weighted population estimates and proportions, and used logistic regression to determine which patient characteristics were associated with these behaviours. Results: Overall, 5.5% (95% confidence interval 5.1%-6.0%) of Canadians reported being unable to afford 1 or more drugs in the prior year, representing 8.2% of those with at least 1 prescription. Drugs for mental health conditions were the most commonly reported drug class for cost-related nonadherence. About 303 000 Canadians had <span class="hlt">additional</span> doctor visits, about 93 000 sought care in the emergency department, and about 26 000 were admitted to hospital at the population level. Many Canadians forewent basic needs such as food (about 730 000 people), heat (about 238 000) and other health care expenses (about 239 000) because of drug costs. These outcomes were more common among females, younger adults, Aboriginal peoples, those with poorer health status, those lacking drug insurance and those with lower income. Interpretation: Out-of-pocket <span class="hlt">charges</span> for medicines for Canadians are associated with foregoing prescription drugs and other necessities as well as use of <span class="hlt">additional</span> health care services. Changes to protect vulnerable populations from drug costs might reduce these <span class="hlt">negative</span> outcomes. PMID:29440236</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JHEP...11..183D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JHEP...11..183D"><span><span class="hlt">Charged</span> structure constants from modularity</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Das, Diptarka; Datta, Shouvik; Pal, Sridip</p> <p>2017-11-01</p> <p>We derive a universal formula for the average heavy-heavy-light structure constants for 2 d CFTs with non-vanishing u(1) <span class="hlt">charge</span>. The derivation utilizes the modular properties of one-point functions on the torus. Refinements in N=2 SCFTs, show that the resulting Cardy-like formula for the structure constants has precisely the same shifts in the central <span class="hlt">charge</span> as that of the thermodynamic entropy found earlier. This analysis generalizes the recent results by Kraus and Maloney for CFTs with an <span class="hlt">additional</span> global u(1) symmetry [1]. Our results at large central <span class="hlt">charge</span> are also shown to match with computations from the holographic dual, which suggest that the averaged CFT three-point coefficient also serves as a useful probe of detecting black hole hair.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014APS..DMP.D1048B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014APS..DMP.D1048B"><span>Critical Nuclear <span class="hlt">Charge</span> of the Quantum Mechanical Three-Body Problem</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Busuttil, Michael; Moini, Amirreza; Drake, Gordon W. F.</p> <p>2014-05-01</p> <p>The critical nuclear <span class="hlt">charge</span> (Zc) for a three-body quantum mechanical system consisting of positive and <span class="hlt">negative</span> <span class="hlt">charges</span> is the minimum nuclear <span class="hlt">charge</span> that can keep the system in a bound state. Here we present a study of the critical nuclear <span class="hlt">charge</span> for two-electron (heliumlike) systems with infinite nuclear mass, and also a range of reduced mass ratio (μ / m) up to 0.5. The results help to resolve a discrepancy in the literature for the infinite mass case, and they are the first to study the dependence on reduced mass ratio. It was found that Zc has a local maximum with μ / m = 0 . 352 5 . The critical <span class="hlt">charge</span> for the infinite mass case is found to be Zc = 0 . 911 028 224 076 8 (1 0) . This value is more accurate than any previous value in the literature, and agrees with the upper bound Zc = 0 . 911 03 reported by Baker et al.. The critical nuclear <span class="hlt">charge</span> outside this range [0.5 - 1.0] still needs to be investigated in future works. Research Supported by NSERC and SHARCNET.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19770035201&hterms=VISWANATHAN&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26N%3D0%26No%3D20%26Ntt%3DVISWANATHAN','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19770035201&hterms=VISWANATHAN&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26N%3D0%26No%3D20%26Ntt%3DVISWANATHAN"><span>Model for thickness dependence of radiation <span class="hlt">charging</span> in MOS structures</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Viswanathan, C. R.; Maserjian, J.</p> <p>1976-01-01</p> <p>The model considers <span class="hlt">charge</span> buildup in MOS structures due to hole trapping in the oxide and the creation of sheet <span class="hlt">charge</span> at the silicon interface. The contribution of hole trapping causes the flatband voltage to increase with thickness in a manner in which square and cube dependences are limiting cases. Experimental measurements on samples covering a 200 - 1000 A range of oxide thickness are consistent with the model, using independently obtained values of hole-trapping parameters. An important finding of our experimental results is that a <span class="hlt">negative</span> interface <span class="hlt">charge</span> contribution due to surface states created during irradiation compensates most of the positive <span class="hlt">charge</span> in the oxide at flatband. The tendency of the surface states to 'track' the positive <span class="hlt">charge</span> buildup in the oxide, for all thicknesses, applies both in creation during irradiation and in annihilation during annealing. An explanation is proposed based on the common defect origin of hole traps and potential surface states.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li class="active"><span>21</span></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_21 --> <div id="page_22" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li class="active"><span>22</span></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="421"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20384999','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20384999"><span>Effect of <span class="hlt">negative</span> air ions on the potential for bacterial contamination of plastic medical equipment.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Shepherd, Simon J; Beggs, Clive B; Smith, Caroline F; Kerr, Kevin G; Noakes, Catherine J; Sleigh, P Andrew</p> <p>2010-04-12</p> <p>In recent years there has been renewed interest in the use of air ionizers to control the spread of infection in hospitals and a number of researchers have investigated the biocidal action of ions in both air and nitrogen. By comparison, the physical action of air ions on bacterial dissemination and deposition has largely been ignored. However, there is clinical evidence that air ions might play an important role in preventing the transmission of Acinetobacter infection. Although the reasons for this are unclear, it is hypothesized that a physical effect may be responsible: the production of air ions may <span class="hlt">negatively</span> <span class="hlt">charge</span> items of plastic medical equipment so that they repel, rather than attract, airborne bacteria. By <span class="hlt">negatively</span> <span class="hlt">charging</span> both particles in the air and items of plastic equipment, the ionizers minimize electrostatic deposition on these items. In so doing they may help to interrupt the transmission of Acinetobacter infection in certain healthcare settings such as intensive care units. A study was undertaken in a mechanically ventilated room under ambient conditions to accurately measure changes in surface potential exhibited by items of plastic medical equipment in the presence of <span class="hlt">negative</span> air ions. Plastic items were suspended on nylon threads, either in free space or in contact with a table surface, and exposed to <span class="hlt">negative</span> ions produced by an air ionizer. The <span class="hlt">charge</span> build-up on the specimens was measured using an electric field mill while the ion concentration in the room air was recorded using a portable ion counter. The results of the study demonstrated that common items of equipment such as ventilator tubes rapidly developed a large <span class="hlt">negative</span> <span class="hlt">charge</span> (i.e. generally >-100V) in the presence of a <span class="hlt">negative</span> air ionizer. While most items of equipment tested behaved in a similar manner to this, one item, a box from a urological collection and monitoring system (the only item made from styrene acrylonitrile), did however develop a positive <span class="hlt">charge</span> in the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27728826','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27728826"><span>Self assembly of oppositely <span class="hlt">charged</span> latex particles at oil-water interface.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Nallamilli, Trivikram; Ragothaman, Srikanth; Basavaraj, Madivala G</p> <p>2017-01-15</p> <p>In this study we explore the self assembly of oppositely <span class="hlt">charged</span> latex particles at decane water interfaces. Two spreading protocols have been proposed in this context. In the first method oppositely <span class="hlt">charged</span> particles are mixed prior to spreading at the interface, this is called "premixed-mixtures". In the second protocol <span class="hlt">negatively</span> <span class="hlt">charged</span> particles are first spread at the interface at known coverage followed by spreading positively <span class="hlt">charged</span> particles at known coverage and this is called "sequential-mixtures". In premixed mixtures depending on particle mixing ratio (composition) and total surface coverage a number of 2d structures ranging from 2d crystals, aggregate-crystal coexistence and 2d-gels are observed. A detailed phase diagram of this system has been explored. In sequential-mixtures for the first time we observed a new phase in colloidal monolayers called 2d-bi crystalline domains. These structures consisted regions of two crystal phases of oppositely <span class="hlt">charged</span> particles separated by a one dimensional chain of alternating positive and <span class="hlt">negative</span> particles. Phase diagram of this system has also been explored at various combinations of first spread and second spread particles. A possible mechanism leading to formation of these 2d bi crystalline structures has been discussed. A direct visualization of breakage and reformation of particle barriers separating the crystal phases has been demonstrated through videos. Effect of salt in the water sub phase and particle hydrophobicity on domain formation is also investigated. Copyright © 2016 Elsevier Inc. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2001PhDT.......325M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2001PhDT.......325M"><span><span class="hlt">Charged</span> systems in bulk and at interfaces</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Moreira, André Guérin</p> <p>2001-05-01</p> <p> remains a good approximation at low coupling values, while the strong coupling theory is shown to lead to the correct density profiles close to the wall (and at all couplings). For very large couplings, only systems where the difference between the dielectric constants of the wall and of the solvent is small are shown to be well described by SC. Another experimentally relevant modification to the simple double layer is to make the <span class="hlt">charges</span> at the plane discrete. The counterions are still assumed to be point-like, but we constraint the distance of approach between ions in the plane and counterions to a minimum distance D. The ratio between D and the distance between neighboring ions in the plane is, as we will see, one of the important quantities in determining the influence of the discrete nature of the <span class="hlt">charges</span> at the wall over the density profiles. Another parameter that plays an important role, as in the previous case, is the coupling as we will demonstrate, systems with higher coupling are more subject to discretization effects than systems with low coupling parameter. After studying the isolated double layer, we look at the interaction between two double layers. The system is composed by two equally <span class="hlt">charged</span> walls at distance d, with the counterions confined between them. The <span class="hlt">charge</span> at the walls is smeared out and the dielectric constant is the same everywhere. Using Monte-Carlo simulations we obtain the inter-plate pressure in the global parameter space, and the pressure is shown to be <span class="hlt">negative</span> (attraction) at certain conditions. The simulations also show that the equilibrium plate separation (where the pressure changes from attractive to repulsive) exhibits a novel unbinding transition. We compare the Monte Carlo results with the strong-coupling theory, which is shown to describe well the bound states of systems with moderate and high couplings. The regime where the two walls are very close to each other is also shown to be well described by the SC theory. Finally</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1196561-greybody-factors-charges-kerr-cft','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1196561-greybody-factors-charges-kerr-cft"><span>Greybody factors and <span class="hlt">charges</span> in Kerr/CFT</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Cvetič, Mirjam; Larsen, Finn</p> <p>2009-09-01</p> <p>We compute greybody factors for near extreme Kerr black holes in D = 4 and D = 5. In D = 4 we include four <span class="hlt">charges</span> so that our solutions can be continuously deformed to the BPS limit. In D = 5 we include two independent angular momenta so Left-Right symmetry is incorporated. We discuss the CFT interpretation of our emission amplitudes, including the overall frequency dependence and the dependence on all black hole parameters. We find that all <span class="hlt">additional</span> parameters can be incorporated Kerr/CFT, with central <span class="hlt">charge</span> independent of U(1) <span class="hlt">charges</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/15167803','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/15167803"><span>Heterogeneous surface <span class="hlt">charge</span> enhanced micromixing for electrokinetic flows.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Biddiss, Elaine; Erickson, David; Li, Dongqing</p> <p>2004-06-01</p> <p>Enhancing the species mixing in microfluidic applications is key to reducing analysis time and increasing device portability. The mixing in electroosmotic flow is usually diffusion-dominated. Recent numerical studies have indicated that the introduction of electrically <span class="hlt">charged</span> surface heterogeneities may augment mixing efficiencies by creating localized regions of flow circulation. In this study, we experimentally visualized the effects of surface <span class="hlt">charge</span> patterning and developed an optimized electrokinetic micromixer applicable to the low Reynolds number regime. Using the optimized micromixer, mixing efficiencies were improved between 22 and 68% for the applied potentials ranging from 70 to 555 V/cm when compared with the <span class="hlt">negatively</span> <span class="hlt">charged</span> homogeneous case. For producing a 95% mixture, this equates to a potential decrease in the required mixing channel length of up to 88% for flows with Péclet numbers between 190 and 1500.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AAS...23125504E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AAS...23125504E"><span><span class="hlt">Charge</span> Management in LISA Pathfinder: The Continuous Discharging Experiment</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ewing, Becca Elizabeth</p> <p>2018-01-01</p> <p>Test mass <span class="hlt">charging</span> is a significant source of excess force and force noise in LISA Pathfinder (LPF). The planned design scheme for mitigation of <span class="hlt">charge</span> induced force noise in LISA is a continuous discharge by UV light illumination. We report on analysis of a <span class="hlt">charge</span> management experiment on-board LPF conducted during December 2016. We discuss the measurement of test mass <span class="hlt">charging</span> noise with and without continuous UV illumination, in <span class="hlt">addition</span> to the dynamic response in the continuous discharge scheme. Results of the continuous discharge system will be discussed for their application to operating LISA with lower test mass <span class="hlt">charge</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22483045-overview-negative-ion-based-neutral-beam-injectors-iter','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22483045-overview-negative-ion-based-neutral-beam-injectors-iter"><span>Overview of the <span class="hlt">negative</span> ion based neutral beam injectors for ITER</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Schunke, B., E-mail: email@none.edu; Boilson, D.; Chareyre, J.</p> <p>2016-02-15</p> <p>The ITER baseline foresees 2 Heating Neutral Beams (HNB’s) based on 1 MeV 40 A D{sup −} <span class="hlt">negative</span> ion accelerators, each capable of delivering 16.7 MW of deuterium atoms to the DT plasma, with an optional 3rd HNB injector foreseen as a possible upgrade. In <span class="hlt">addition</span>, a dedicated diagnostic neutral beam will be injecting ≈22 A of H{sup 0} at 100 keV as the probe beam for <span class="hlt">charge</span> exchange recombination spectroscopy. The integration of the injectors into the ITER plant is nearly finished necessitating only refinements. A large number of components have passed the final design stage, manufacturing has started,more » and the essential test beds—for the prototype route chosen—will soon be ready to start.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2217050','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2217050"><span>Total <span class="hlt">Charge</span> Movement per Channel</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Sigg, Daniel; Bezanilla, Francisco</p> <p>1997-01-01</p> <p>One measure of the voltage dependence of ion channel conductance is the amount of gating <span class="hlt">charge</span> that moves during activation and vice versa. The limiting slope method, introduced by Almers (Almers, W. 1978. Rev. Physiol. Biochem. Pharmacol. 82:96–190), exploits the relationship of <span class="hlt">charge</span> movement and voltage sensitivity, yielding a lower limit to the range of single channel gating <span class="hlt">charge</span> displacement. In practice, the technique is plagued by low experimental resolution due to the requirement that the logarithmic voltage sensitivity of activation be measured at very low probabilities of opening. In <span class="hlt">addition</span>, the linear sequential models to which the original theory was restricted needed to be expanded to accommodate the complexity of mechanisms available for the activation of channels. In this communication, we refine the theory by developing a relationship between the mean activation <span class="hlt">charge</span> displacement (a measure of the voltage sensitivity of activation) and the gating <span class="hlt">charge</span> displacement (the integral of gating current). We demonstrate that recording the equilibrium gating <span class="hlt">charge</span> displacement as an adjunct to the limiting slope technique greatly improves accuracy under conditions where the plots of mean activation <span class="hlt">charge</span> displacement and gross gating <span class="hlt">charge</span> displacement versus voltage can be superimposed. We explore this relationship for a wide variety of channel models, which include those having a continuous density of states, nonsequential activation pathways, and subconductance states. We introduce new criteria for the appropriate use of the limiting slope procedure and provide a practical example of the theory applied to low resolution simulation data. PMID:8997663</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29622552','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29622552"><span>Clival Malformations in <span class="hlt">CHARGE</span> Syndrome.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Mahdi, E S; Whitehead, M T</p> <p>2018-06-01</p> <p><span class="hlt">CHARGE</span> syndrome is a multisystemic congenital disorder, most commonly including coloboma, heart malformations, choanal atresia, developmental delay, and genital and ear anomalies. The diagnostic criteria for <span class="hlt">CHARGE</span> syndrome have been refined with time. However, limited reports describe skull base and craniocervical junction abnormalities. Recently, a coronal clival cleft has been identified in association with <span class="hlt">CHARGE</span> syndrome. The aim of our study was to assess the prevalence of clival pathology in <span class="hlt">CHARGE</span> syndrome. In this retrospective study, the CT/MR imaging data base at a single academic children's hospital was queried for the phrase "<span class="hlt">CHARGE</span> syndrome" during a 17-year period (2001-2017). Electronic medical records were reviewed to confirm the diagnosis. Images were assessed for skull base anomalies, specifically clival hypoplasia and dysplasia. The search yielded 42 examinations (21 CTs and 21 MRIs) from 15 distinct patients (mean age, 4.1 ± 5.6 years; range, 2 days to 19 years). <span class="hlt">CHARGE</span> syndrome diagnosis was confirmed either by clinical and genetic testing ( n = 6) or by clinical diagnosis only ( n = 9). A coronal clival cleft was identified in 87% of patients (37 examinations, n = 13 patients), either partial (53%) or complete (33%). Clival hypoplasia without clefting was present in all 5 examinations from the remaining 2 patients. Clival pathology is universal in <span class="hlt">CHARGE</span> syndrome. Coronal clival clefts are extremely common, representing a useful <span class="hlt">additional</span> diagnostic finding. Detection of a clival cleft should alert the radiologist to examine the palate, choana, eyes, ears, and olfactory centers for other signs of <span class="hlt">CHARGE</span> syndrome. © 2018 by American Journal of Neuroradiology.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=35077&Lab=NRMRL&keyword=corona&actType=&TIMSType=+&TIMSSubTypeID=&DEID=&epaNumber=&ntisID=&archiveStatus=Both&ombCat=Any&dateBeginCreated=&dateEndCreated=&dateBeginPublishedPresented=&dateEndPublishedPresented=&dateBeginUpdated=&dateEndUpdated=&dateBeginCompleted=&dateEndCompleted=&personID=&role=Any&journalID=&publisherID=&sortBy=revisionDate&count=50','EPA-EIMS'); return false;" href="https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=35077&Lab=NRMRL&keyword=corona&actType=&TIMSType=+&TIMSSubTypeID=&DEID=&epaNumber=&ntisID=&archiveStatus=Both&ombCat=Any&dateBeginCreated=&dateEndCreated=&dateBeginPublishedPresented=&dateEndPublishedPresented=&dateBeginUpdated=&dateEndUpdated=&dateBeginCompleted=&dateEndCompleted=&personID=&role=Any&journalID=&publisherID=&sortBy=revisionDate&count=50"><span>PULSE ENERGIZATION IN THE TUFT CORONA REGIME OF <span class="hlt">NEGATIVE</span> CORONA</span></a></p> <p><a target="_blank" href="http://oaspub.epa.gov/eims/query.page">EPA Science Inventory</a></p> <p></p> <p></p> <p>The paper discusses pulse energization in the tuft corona regime of <span class="hlt">negative</span> corona. Fabric filtration, with integral particle <span class="hlt">charging</span> and collection in a combined electric and flow field, is sensitive to maldistribution of current among bags energized by one power source, espec...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25092587','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25092587"><span>Increasing binding density of yeast cells by control of surface <span class="hlt">charge</span> with allylamine grafting to ion modified polymer surfaces.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Tran, Clara T H; Kondyurin, Alexey; Chrzanowski, Wojciech; Bilek, Marcela M M; McKenzie, David R</p> <p>2014-10-01</p> <p>Plasma immersion ion implantation (PIII) treatment of polymers creates a biointerface capable of direct covalent immobilization of biomolecules. The immobilization of protein molecules is achieved by covalent bonds formed between embedded radicals on the treated surface and amino acid side chains and cells can be immobilized through cell-wall proteins. The attachment density of <span class="hlt">negatively</span> <span class="hlt">charged</span> entities on a PIII treated surface is inhibited by its <span class="hlt">negative</span> surface <span class="hlt">charge</span> at neutral pH. To reduce the <span class="hlt">negative</span> <span class="hlt">charge</span> of PIII treated surfaces in phosphate buffer (pH 7.4, 11mM), we develop an effective approach of grafting allylamine monomers onto the treated surface. The results reveal reactions between allylamine and radicals on the PIII treated surface. One of these triggers polymerization, increasing the number of amine groups grafted. As a consequence, the PIII treated polystyrene surface after allylamine exposure becomes more hydrophobic and less <span class="hlt">negatively</span> <span class="hlt">charged</span> in phosphate buffer. Using yeast cells as an example, we have shown a significant improvement (6-15 times) of cell density immobilized on the PIII treated surface after exposure to allylamine. Copyright © 2014 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=161049&Lab=NERL&keyword=contractor&actType=&TIMSType=+&TIMSSubTypeID=&DEID=&epaNumber=&ntisID=&archiveStatus=Both&ombCat=Any&dateBeginCreated=&dateEndCreated=&dateBeginPublishedPresented=&dateEndPublishedPresented=&dateBeginUpdated=&dateEndUpdated=&dateBeginCompleted=&dateEndCompleted=&personID=&role=Any&journalID=&publisherID=&sortBy=revisionDate&count=50','EPA-EIMS'); return false;" href="https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=161049&Lab=NERL&keyword=contractor&actType=&TIMSType=+&TIMSSubTypeID=&DEID=&epaNumber=&ntisID=&archiveStatus=Both&ombCat=Any&dateBeginCreated=&dateEndCreated=&dateBeginPublishedPresented=&dateEndPublishedPresented=&dateBeginUpdated=&dateEndUpdated=&dateBeginCompleted=&dateEndCompleted=&personID=&role=Any&journalID=&publisherID=&sortBy=revisionDate&count=50"><span>ELECTROSTATIC FORCES IN WIND-POLLINATION: PART 1: MEASUREMENT OF THE ELECTROSTATIC <span class="hlt">CHARGE</span> ON POLLEN</span></a></p> <p><a target="_blank" href="http://oaspub.epa.gov/eims/query.page">EPA Science Inventory</a></p> <p></p> <p></p> <p>Under fair weather conditions, a weak electric field exists between <span class="hlt">negative</span> <span class="hlt">charge</span> induced on the surface of plants and positive <span class="hlt">charge</span> in the air. This field is magnified around points (e.g. stigmas) and can reach values up to 3x10<SUP>6</SUP> V m<SUP>-1</SUP>. If wind-disperse...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1244677-price-incentivised-electric-vehicle-charge-control-community-voltage-regulation','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1244677-price-incentivised-electric-vehicle-charge-control-community-voltage-regulation"><span>Price Incentivised Electric Vehicle <span class="hlt">Charge</span> Control for Community Voltage Regulation</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Kelly, Damian; Baroncelli, Fabio; Fowler, Christopher</p> <p>2014-11-03</p> <p>With the growing availability of Electric Vehicles, there is a significant opportunity to use battery 'smart-<span class="hlt">charging</span>' for voltage regulation. This work designs and experimentally evaluates a system for price-incentivised electric vehicle <span class="hlt">charging</span>. The system is designed to eliminate <span class="hlt">negative</span> impacts to the user while minimising the cost of <span class="hlt">charging</span> and achieving a more favourable voltage behaviour throughout the local grid over time. The practical issues associated with a real-life deployment are identified and resolved. The efficacy of the system is evaluated in the challenging scenario in which EVs are deployed in six closely distributed homes, serviced by the same lowmore » voltage residential distribution feeder.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20020043395','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20020043395"><span>Performance of Li-Ion Cells Under Battery Voltage <span class="hlt">Charge</span> Control</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Rao, Gopalakrishna M.; Vaidyanathan, Hari; Day, John H. (Technical Monitor)</p> <p>2001-01-01</p> <p>A study consisting of electrochemical characterization and Low-Earth-Orbit (LEO) cycling of Li-Ion cells from three vendors was initiated in 1999 to determine the cycling performance and to infuse the new technology in the future NASA missions. The 8-cell batteries included in this evaluation are prismatic cells manufactured by Mine Safety Appliances Company (MSA), cylindrical cells manufactured by SAFT and prismatic cells manufactured by Yardney Technical Products, Inc. (YTP). The three batteries were cycle tested in the LEO regime at 40% depth of discharge, and under a <span class="hlt">charge</span> control technique that consists of battery voltage clamp with a current taper. The initial testing was conducted at 20 C; however, the batteries were cycled also intermittently at low temperatures. YTP 20 Ah cells consisted of mixed-oxide (Co and Ni) positive, graphitic carbon <span class="hlt">negative</span>, LIPF6 salt mixed with organic carbonate solvents. The battery voltage clamp was 32 V. The low temperature cycling tests started after 4575 cycles at 20 C. The cells were not capable of cycling. at low temperature since the <span class="hlt">charge</span> acceptance at battery level was poor. There was a cell in the battery that showed too high an end-of-<span class="hlt">charge</span> (EOC) voltage thereby limiting the ability to <span class="hlt">charge</span> the rest of the cells in the battery. The battery has completed 6714 cycles. SAFT 12 Ah cells consisted of mixed-oxide (Co and NO positive, graphitic carbon <span class="hlt">negative</span>, LiPF6 salt mixed with organic carbonate solvents. The battery voltage clamp was for 30.8 V. The low temperature cycling tests started after 4594 cycles at 20 C. A cell that showed low end of discharge (EOD) and EOC voltages and three other cells that showed higher EOC voltages limited the <span class="hlt">charge</span> acceptance at the selected voltage limit during <span class="hlt">charge</span>. The cells were capable of cycling at 10 C and 0 C but the <span class="hlt">charge</span> voltage limit had to be increased to 34.3 V (4.3 V per cell). The low temperature cycling may have induced poor chargeability since the voltage had to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1234891-single-bunch-transverse-instability-circular-accelerator-chromaticity-space-charge','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1234891-single-bunch-transverse-instability-circular-accelerator-chromaticity-space-charge"><span>Single bunch transverse instability in a circular accelerator with chromaticity and space <span class="hlt">charge</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Balbekov, V.</p> <p>2015-10-21</p> <p>The transverse instability of a bunch in a circular accelerator is elaborated in this paper. A new tree-modes model is proposed and developed to describe the most unstable modes of the bunch. This simple and flexible model includes chromaticity and space <span class="hlt">charge</span>, and can be used with any bunch and wake forms. The dispersion equation for the bunch eigentunes is obtained in form of a third-order algebraic equation. The known head-tail and TMCI modes appear as the limiting cases which are distinctly bounded at zero chromaticity only. It is shown that the instability parameters depend only slightly on the bunchmore » model but they are rather sensitive to the wake shape. In particular, space <span class="hlt">charge</span> effects are investigated in the paper and it is shown that their influence depends on sign of wake field enhancing the bunch stability if the wake is <span class="hlt">negative</span>. In <span class="hlt">addition</span>, the resistive wall wake is considered in detail including a comparison of single and collective effects. A comparison of the results with earlier publications is carried out.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27976580','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27976580"><span>Through-Space <span class="hlt">Charge</span> Interaction Substituent Effects in Molecular Catalysis Leading to the Design of the Most Efficient Catalyst of CO2-to-CO Electrochemical Conversion.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Azcarate, Iban; Costentin, Cyrille; Robert, Marc; Savéant, Jean-Michel</p> <p>2016-12-28</p> <p>The starting point of this study of through-space substituent effects on the catalysis of the electrochemical CO 2 -to-CO conversion by iron(0) tetraphenylporphyrins is the linear free energy correlation between through-structure electronic effects and the iron(I/0) standard potential that we established separately. The introduction of four positively <span class="hlt">charged</span> trimethylanilinium groups at the para positions of the tetraphenylporphyrin (TPP) phenyls results in an important positive deviation from the correlation and a parallel improvement of the catalytic Tafel plot. The assignment of this catalysis boosting effect to the Coulombic interaction of these positive <span class="hlt">charges</span> with the <span class="hlt">negative</span> <span class="hlt">charge</span> borne by the initial Fe 0 -CO 2 adduct is confirmed by the <span class="hlt">negative</span> deviation observed when the four positive <span class="hlt">charges</span> are replaced by four <span class="hlt">negative</span> <span class="hlt">charges</span> borne by sulfonate groups also installed in the para positions of the TPP phenyls. The climax of this strategy of catalysis boosting by means of Coulombic stabilization of the initial Fe 0 -CO 2 adduct is reached when four positively <span class="hlt">charged</span> trimethylanilinium groups are introduced at the ortho positions of the TPP phenyls. The <span class="hlt">addition</span> of a large concentration of a weak acid-phenol-helps by cleaving one of the C-O bonds of CO 2 . The efficiency of the resulting catalyst is unprecedented, as can be judged by the catalytic Tafel plot benchmarking with all presently available catalysts of the electrochemical CO 2 -to-CO conversion. The maximal turnover frequency (TOF) is as high as 10 6 s -1 and is reached at an overpotential of only 220 mV; the extrapolated TOF at zero overpotential is larger than 300 s -1 . This catalyst leads to a highly selective formation of CO (practically 100%) in spite of the presence of a high concentration of phenol, which could have favored H 2 evolution. It is also very stable, showing no significant alteration after more than 80 h of electrolysis.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/898849-relativistic-collisions-highly-charged-ions','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/898849-relativistic-collisions-highly-charged-ions"><span>Relativistic Collisions of Highly-<span class="hlt">Charged</span> Ions</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Ionescu, Dorin; Belkacem, Ali</p> <p>1998-11-19</p> <p>The physics of elementary atomic processes in relativistic collisions between highly-<span class="hlt">charged</span> ions and atoms or other ions is briefly discussed, and some recent theoretical and experimental results in this field are summarized. They include excitation, capture, ionization, and electron-positron pair creation. The numerical solution of the two-center Dirac equation in momentum space is shown to be a powerful nonperturbative method for describing atomic processes in relativistic collisions involving heavy and highly-<span class="hlt">charged</span> ions. By propagating <span class="hlt">negative</span>-energy wave packets in time the evolution of the QED vacuum around heavy ions in relativistic motion is investigated. Recent results obtained from numerical calculations usingmore » massively parallel processing on the Cray-T3E supercomputer of the National Energy Research Scientific Computer Center (NERSC) at Berkeley National Laboratory are presented.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20120003009','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120003009"><span>SA13B-1900 Auroral <span class="hlt">Charging</span> of the International Space Station</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Minow, Joseph I.; Chandler, Michael O.; Wright, Kenneth H., Jr.</p> <p>2011-01-01</p> <p>Electrostatic potential variations of the International Space Station (ISS) relative to the space plasma environment are dominated by interaction of the <span class="hlt">negatively</span> grounded 160 volt US photovoltaic power system with the plasma environment in sunlight and inductive potential variations across the ISS structure generated by motion of the vehicle across the Earth's magnetic field. Auroral <span class="hlt">charging</span> is also a source of potential variations because the 51.6? orbital inclination of ISS takes the vehicle to sufficiently high magnetic latitudes to encounter precipitating electrons during geomagnetic storms. Analysis of auroral <span class="hlt">charging</span> for small spacecraft or isolated insulating regions on ISS predict rapid <span class="hlt">charging</span> to high potentials of hundreds of volts but it has been thought that the large capacitance of the entire ISS structure on the order of 0.01 F will limit frame potentials to less than a volt when exposed to auroral conditions. We present three candidate auroral <span class="hlt">charging</span> events characterized by transient ISS structure potentials varying from approximately 2 to 17 volts. The events occur primarily at night when the solar arrays are unbiased and cannot therefore be due to solar array current collection. ISS potential decreases to more <span class="hlt">negative</span> values during the events indicating electron current collection and the events are always observed at the highest latitudes along the ISS trajectory. Comparison of the events with integral >30 keV electron flux measurements from NOAA TIROS spacecraft demonstrate they occur within regions of precipitating electron flux at levels consistent with the energetic electron thresholds reported for onset of auroral <span class="hlt">charging</span> of the DMSP and Freja satellites. In contrast to the DMSP and Freja events, one of the ISS <span class="hlt">charging</span> events occur in sunlight.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JPhD...51u5601S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JPhD...51u5601S"><span>Asymmetric injection and distribution of space <span class="hlt">charges</span> in propylene carbonate under impulse voltage</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sima, Wenxia; Chen, Qiulin; Sun, Potao; Yang, Ming; Guo, Hongda; Ye, Lian</p> <p>2018-05-01</p> <p>Space <span class="hlt">charge</span> can distort the electric field in high voltage stressed liquid dielectrics and lead to breakdown. Observing the evolution of space <span class="hlt">charge</span> in real time and determining the influencing factors are of considerable significance. The spatio-temporal evolution of space <span class="hlt">charge</span> in propylene carbonate, which is very complex under impulse voltage, was measured in this study through the time-continuous Kerr electro-optic field mapping measurement. We found that the injection <span class="hlt">charge</span> from a brass electrode displayed an asymmetric effect; that is, the <span class="hlt">negative</span> <span class="hlt">charge</span> injection near the cathode lags behind the positive <span class="hlt">charge</span> injection near the anode. Physical mechanisms, including <span class="hlt">charge</span> generation and drift, are analyzed, and a voltage-dependent saturated drift rectification model was established to explain the interesting phenomena. Mutual validation of models and our measurement data indicated that a barrier layer, which is similar to metal-semiconductor contact, was formed in the contact interface between the electrode and propylene carbonate and played an important role in the space <span class="hlt">charge</span> injection.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19800020918','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19800020918"><span>Analysis of differential and active <span class="hlt">charging</span> phenomena on ATS-5 and ATS-6</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Olsen, R. C.; Whipple, E. C., Jr.</p> <p>1980-01-01</p> <p>Spacecraft <span class="hlt">charging</span> on the differential <span class="hlt">charging</span> and artificial particle emission experiments on ATS 5 and ATS 6 were studied. Differential <span class="hlt">charging</span> of spacecraft surfaces generated large electrostatic barriers to spacecraft generated electrons, from photoemission, secondary emission, and thermal emitters. The electron emitter could partially or totally discharge the satellite, but the mainframe recharged <span class="hlt">negatively</span> in a few 10's of seconds. The time dependence of the <span class="hlt">charging</span> behavior was explained by the relatively large capacitance for differential <span class="hlt">charging</span> in comparison to the small spacecraft to space capacitance. A daylight <span class="hlt">charging</span> event on ATS 6 was shown to have a <span class="hlt">charging</span> behavior suggesting the dominance of differential <span class="hlt">charging</span> on the absolute potential of the mainframe. Ion engine operations and plasma emission experiments on ATS 6 were shown to be an effective means of controlling the spacecraft potential in eclipse and sunlight. Elimination of barrier effects around the detectors and improving the quality of the particle data are discussed.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li class="active"><span>22</span></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_22 --> <div id="page_23" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li class="active"><span>23</span></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="441"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004APS..DPPFP1060F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004APS..DPPFP1060F"><span>Measuring particle <span class="hlt">charge</span> in an rf dusty plasma</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fung, Jerome; Liu, Bin; Goree, John; Nosenko, Vladimir</p> <p>2004-11-01</p> <p>A dusty plasma is an ionized gas containing micron-size particles of solid matter. A particle gains a large <span class="hlt">negative</span> <span class="hlt">charge</span> by collecting electrons and ions from the plasma. In a gas discharge, particles can be levitated by the sheath electric field above a horizontal planar electrode. Most dusty plasma experiments require a knowledge of the particle <span class="hlt">charge</span>, which is a key parameter for all interactions with other particles and the plasma electric field. Several methods have been developed in the literature to measure the <span class="hlt">charge</span>. The vertical resonance method uses Langmuir probe measurements of the ion density and video camera measurements of the amplitude of vertical particle oscillations, which are excited by modulating the rf voltage. Here, we report a new method that is a variation of the vertical resonance method. It uses the plasma potential and particle height, which can be measured more accurately than the ion density. We tested this method and compared the resulting <span class="hlt">charge</span> to values obtained using the original resonance method as well as sound speed methods. Work supported by an NSF REU grant, NASA and DOE.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19484164','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19484164"><span>The impact of prescription <span class="hlt">charges</span> on asthma patients is uneven and unpredictable: evidence from qualitative interviews.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Schafheutle, Ellen I</p> <p>2009-12-01</p> <p>To explore whether, and how, prescription <span class="hlt">charges</span> affect asthma patients' disease management behaviour. Thirty qualitative interviews. Interviewees were aged between 21 and 59, 21 were women, 24 were paying individual prescription <span class="hlt">charges</span>, and six had prepayment certificates (PPCs). Most had a beta2-agonist 'reliever' and a steroid 'preventer' inhaler. Prescription <span class="hlt">charges</span> posed affordability issues for some, and for two patients cost-related reduction in 'preventer' use affected asthma control <span class="hlt">negatively</span>. Many described various ways of keeping medication cost down. Affordability issues, <span class="hlt">negative</span> views on paying <span class="hlt">charges</span>, and whether interviewees viewed their asthma medication as essential, were influential factors. Steroid inhalers were viewed more commonly as being less essential and affected by cost. The episodic nature of asthma meant that predicting benefit from PPCs was difficult. This study strengthens existing evidence that medication cost is a factor in asthma patients' management decisions, with a potential cost-related impact on asthma control.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..MAR.B5010D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..MAR.B5010D"><span><span class="hlt">Charge</span> Inversion in semi-permeable membranes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Das, Siddhartha; Sinha, Shayandev; Jing, Haoyuan</p> <p></p> <p>Role of semi-permeable membranes like lipid bilayer is ubiquitous in a myriad of physiological and pathological phenomena. Typically, lipid membranes are impermeable to ions and solutes; however, protein channels embedded in the membrane allow the passage of selective, small ions across the membrane enabling the membrane to adopt a semi-permeable nature. This semi-permeability, in turn, leads to electrostatic potential jump across the membrane, leading to effects such as regulation of intracellular calcium, extracellular-vesicle-membrane interactions, etc. In this study, we theoretically demonstrate that this semi-permeable nature may trigger the most remarkable <span class="hlt">charge</span> inversion (CI) phenomenon in the cytosol-side of the <span class="hlt">negatively-charged</span> lipid bilayer membrane that are selectively permeable to only positive ions of a given salt. This CI is manifested as the changing of the sign of the electrostatic potential from <span class="hlt">negative</span> to positive from the membrane-cytosol interface to deep within the cytosol. We study the impact of the parameters such as the concentration of this salt with selectively permeable ions as well as the concentration of an external salt in the development of this CI phenomenon. We anticipate such CI will profoundly influence the interaction of membrane and intra-cellular moieties (e.g., exosome or multi-cellular vesicles) having implications for a host of biophysical processes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=187743&keyword=microparticles&actType=&TIMSType=+&TIMSSubTypeID=&DEID=&epaNumber=&ntisID=&archiveStatus=Both&ombCat=Any&dateBeginCreated=&dateEndCreated=&dateBeginPublishedPresented=&dateEndPublishedPresented=&dateBeginUpdated=&dateEndUpdated=&dateBeginCompleted=&dateEndCompleted=&personID=&role=Any&journalID=&publisherID=&sortBy=revisionDate&count=50','EPA-EIMS'); return false;" href="https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=187743&keyword=microparticles&actType=&TIMSType=+&TIMSSubTypeID=&DEID=&epaNumber=&ntisID=&archiveStatus=Both&ombCat=Any&dateBeginCreated=&dateEndCreated=&dateBeginPublishedPresented=&dateEndPublishedPresented=&dateBeginUpdated=&dateEndUpdated=&dateBeginCompleted=&dateEndCompleted=&personID=&role=Any&journalID=&publisherID=&sortBy=revisionDate&count=50"><span>Functionally <span class="hlt">charged</span> nanosize particles differentially activate BV2 microglia.</span></a></p> <p><a target="_blank" href="http://oaspub.epa.gov/eims/query.page">EPA Science Inventory</a></p> <p></p> <p></p> <p>The effect of particle surface <span class="hlt">charge</span> on the biological activation of immortalized mouse microglia (BV2) was examined. Nanosize (860-950 nm) spherical polystyrene microparticles (SPM) were coated with carboxyl (COOH-) or dimethyl amino (CH3)2-N- groups to give a net <span class="hlt">negative</span> or p...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19950020375','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19950020375"><span>Adiabatic <span class="hlt">charging</span> of nickel-hydrogen batteries</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lurie, Chuck; Foroozan, S.; Brewer, Jeff; Jackson, Lorna</p> <p>1995-01-01</p> <p>Battery management during prelaunch activities has always required special attention and careful planning. The transition from nickel-cadium to nickel-hydrogen batteries, with their high self discharge rate and lower <span class="hlt">charge</span> efficiency, as well as longer prelaunch scenarios, has made this aspect of spacecraft battery management even more challenging. The AXAF-I Program requires high battery state of <span class="hlt">charge</span> at launch. The use of active cooling, to ensure efficient <span class="hlt">charging</span>, was considered and proved to be difficult and expensive. Alternative approaches were evaluated. Optimized <span class="hlt">charging</span>, in the absence of cooling, appeared promising and was investigated. Initial testing was conducted to demonstrate the feasibility of the 'Adiabatic <span class="hlt">Charging</span>' approach. Feasibility was demonstrated and <span class="hlt">additional</span> testing performed to provide a quantitative, parametric data base. The assumption that the battery is in an adiabatic environment during prelaunch <span class="hlt">charging</span> is a conservative approximation because the battery will transfer some heat to its surroundings by convective air cooling. The amount is small compared to the heat dissipated during battery overcharge. Because the battery has a large thermal mass, substantial overcharge can occur before the cells get too hot to <span class="hlt">charge</span> efficiently. The testing presented here simulates a true adiabatic environment. Accordingly the data base may be slightly conservative. The adiabatic <span class="hlt">charge</span> methodology used in this investigation begins with stabilizing the cell at a given starting temperature. The cell is then fully insulated on all sides. Battery temperature is carefully monitored and the <span class="hlt">charge</span> terminated when the cell temperature reaches 85 F. <span class="hlt">Charging</span> has been evaluated with starting temperatures from 55 to 75 F.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SPIE10173E..08X','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SPIE10173E..08X"><span><span class="hlt">Negative</span> response of HgCdTe photodiode induced by nanosecond laser pulse</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Xu, Zuodong; Zhang, Jianmin; Lin, Xinwei; Shao, Bibo; Yang, Pengling</p> <p>2017-05-01</p> <p>Photodetectors' behavior and mechanism of transient response are still not understood very well, especially under high photon injection. Most of the researches on this topic were carried out with ultra-short laser pulse, whose pulse width ranged from femtosecond scale to picosecond scale. However, in many applications the durations of incident light are in nanosecond order and the light intensities are strong. To investigate the transient response characteristics and mechanisms of narrow-bandgap photovoltaic detectors under short laser irradiation, we performed an experiment on HgCdTe photodiodes. The n+-on-p type HgCdTe photodiodes in the experiment were designed to work in spectrum from 1.0μm to 3.0μm, with conditions of zero bias and room temperature. They were exposed to in-band short laser pulses with dwell time of 20 nanosecond. When the intensity of incident laser beam rose to 0.1J/cm2 order, the photodiodes' response characteristics turned to be bipolar from unipolar. A much longer <span class="hlt">negative</span> response with duration of about 10μs to 100μs followed the positive light response. The amplitude of the <span class="hlt">negative</span> response increased with the laser intensity, while the dwell time of positive response decreased with the laser intensity. Considering the response characteristics and the device structure, it is proposed that the <span class="hlt">negative</span> response was caused by space <span class="hlt">charge</span> effect at the electrodes. Under intense laser irradiation, a temperature gradient formed in the HgCdTe material. Due to the temperature gradient, the majority carriers diffused away from upper surface and left space <span class="hlt">charge</span> at the electrodes. Then <span class="hlt">negative</span> response voltage could be measured in the external circuit. With higher incident laser intensity, the degree of the space <span class="hlt">charge</span> effect would become higher, and then the <span class="hlt">negative</span> response would come earlier and show larger amplitude.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19323501','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19323501"><span>Adsorption of nonuniformly <span class="hlt">charged</span> fullerene-like nanoparticles on planar polyelectrolyte brushes in aqueous solutions.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Hu, Yiyu; Cao, Dapeng</p> <p>2009-05-05</p> <p>On the basis of the coarse grained model, we investigated the adsorption of nonuniformly <span class="hlt">charged</span> fullerene-like nanoparticles on planar polyelectrolyte brushes (PEBs) in aqueous solution by using Brownian dynamics simulation. It is found that the electroneutral nanoparticles can be adsorbed by the PEB, which is attributed to the asymmetrical electrostatic interactions of the PEB with the positively <span class="hlt">charged</span> sites and <span class="hlt">negatively</span> <span class="hlt">charged</span> sites of the fullerene-like nanoparticles. The simulation results indicated that the adsorption amount exhibits non-monotonic behavior with the dipole moment of nanoparticles. First, the adsorption amount increases with the dipole moment and then reaches the maximum at the dipole moment of micro = 10.45. Finally, the adsorption falls at the dipole moment of micro = 14.39. The reason may be that, at the extremely large dipole moment of micro = 14.39, the fullerene-like nanoparticles aggregate together to form a big cluster in the bulk phase, which can be confirmed by the extremely high peak in the radial distribution function between nanoparticles. Accordingly, it is difficult for nanoparticles to enter into the PEB at the dipole moment of micro = 14.39. In <span class="hlt">addition</span>, it is also found that the brush grafting density is an important factor affecting the brush thickness.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=1464246','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=1464246"><span>Effect of hydration on interstitial distribution of <span class="hlt">charged</span> albumin in rat dermis in vitro</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Wiig, Helge; Tenstad, Olav; Bert, Joel L</p> <p>2005-01-01</p> <p>At physiological pH, <span class="hlt">negatively</span> <span class="hlt">charged</span> glycosaminoglycans in the extracellular matrix may influence distribution volume of macromolecular probes, a phenomenon of importance for hydration of the interstitium and therefore for body fluid balance. We hypothesized that such <span class="hlt">charge</span> effect was dependent on hydration. Human serum albumin (HSA) (the pH value for the isoelectric point (pI) = 4.9) was made neutral by cationization (cHSA) (pI = 7.6). Rat dermis was studied in vitro in a specially designed equilibration cell allowing control of hydration. Using a buffer containing labelled native HSA and cHSA, the distribution volumes were calculated relative to that of 51Cr-EDTA, an extracellular tracer. During changes in hydration (H), defined as (wet weight – dry weight) (dry weight)−1), the slope of the equation describing the relationship between extracellular fluid volume (Vx) (in g H2O (g dry weight)−1) and H (Vx = 0.925 H + 0.105) differed significantly from that for available volumes of cHSA (Va,cHSA = 0.624 H – 0.538) and HSA (Va,HSA = 0.518 H – 0.518). A gradual reduction in H led to a reduction in difference between available volumes for the two albumin species. Screening the fixed <span class="hlt">charges</span> by 1 m NaCl resulted in similar available and excluded volumes of native HSA and neutral cHSA. We conclude that during gradual dehydration, there is a reduced effect of fixed <span class="hlt">negative</span> <span class="hlt">charges</span> on interstitial exclusion of <span class="hlt">charged</span> macromolecules. This effect may be explained by a reduced hydration domain surrounding tissue and probe macromolecules in conditions of increased electrostatic interactions. Furthermore, screening of <span class="hlt">negative</span> <span class="hlt">charges</span> suggested that hyaluronan associated with collagen may influence intrafibrillar volume of collagen and thereby available and excluded volume fraction. PMID:16210353</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title42-vol2/pdf/CFR-2010-title42-vol2-sec405-506.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title42-vol2/pdf/CFR-2010-title42-vol2-sec405-506.pdf"><span>42 CFR 405.506 - <span class="hlt">Charges</span> higher than customary or prevailing <span class="hlt">charges</span> or lowest <span class="hlt">charge</span> levels.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-10-01</p> <p>... 42 Public Health 2 2010-10-01 2010-10-01 false <span class="hlt">Charges</span> higher than customary or prevailing <span class="hlt">charges</span>... prevailing <span class="hlt">charges</span> or lowest <span class="hlt">charge</span> levels. A <span class="hlt">charge</span> which exceeds the customary <span class="hlt">charge</span> of the physician or other person who rendered the medical or other health service, or the prevailing <span class="hlt">charge</span> in the locality...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014cosp...40E3483V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014cosp...40E3483V"><span>Dust Grain <span class="hlt">Charge</span> above the Lunar terminator</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vaverka, Jakub; Richterova, Ivana; Nemecek, Zdenek; Safrankova, Jana; Pavlu, Jiri; Vysinka, Marek</p> <p></p> <p>Interaction of a lunar surface with the solar wind and magnetosphere leads to its <span class="hlt">charging</span> by several processes as photoemission, a collection of primary particles, and secondary electron emission. Nevertheless, <span class="hlt">charging</span> of the lunar surface is complicated by a shielding of solar light and solar wind ions by hills, craters, and boulders that can locally influence the surface potential. Moreover, a presence of a plasma wake can strongly affect this potential at the night side of the Moon. A typical surface potential varies from slightly positive (dayside) to <span class="hlt">negative</span> values of the order of several hundred volts (night side). An electric field above the <span class="hlt">charged</span> surface can lead to a levitation of dust grains as it has been observed by several spacecraft and by astronauts during Apollo missions. Although <span class="hlt">charging</span> and transport of dust grains above the lunar surface are in the center of interest for many years, these phenomena are not still completely understood. We present calculation of an equilibrium potential of dust grains above the lunar surface. We focus on a terminator area during the Earth’s plasma sheet crossing. We use the secondary electron emission model for dust grains which takes into account an influence of the grain size, material, and surface roughness and findings from laboratory experiments with <span class="hlt">charging</span> of lunar dust simulants by an electron beam.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014JPS...263..186G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014JPS...263..186G"><span>Modeling of the cranking and <span class="hlt">charging</span> processes of conventional valve regulated lead acid (VRLA) batteries in micro-hybrid applications</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gou, Jun; Lee, Anson; Pyko, Jan</p> <p>2014-10-01</p> <p>The cranking and <span class="hlt">charging</span> processes of a VRLA battery during stop-start cycling in micro-hybrid applications were simulated by one dimensional mathematical modeling, to study the formation and distribution of lead sulfate across the cell and analyze the resulting effect on battery aging. The battery focused on in this study represents a conventional VRLA battery without any carbon <span class="hlt">additives</span> in the electrodes or carbon-based electrodes. The modeling results were validated against experimental data and used to analyze the "sulfation" of <span class="hlt">negative</span> electrodes - the common failure mode of lead acid batteries under high-rate partial state of <span class="hlt">charge</span> (HRPSoC) cycling. The analyses were based on two aging mechanisms proposed in previous studies and the predictions showed consistency with the previous teardown observations that the sulfate formed at the <span class="hlt">negative</span> interface is more difficult to be converted back than anywhere else in the electrodes. The impact of cranking pulses during stop-start cycling on current density and the corresponding sulfate layer production was estimated. The effects of some critical design parameters on sulfate formation, distribution and aging over cycling were investigated, which provided guidelines for developing models and designing of VRLA batteries in micro-hybrid applications.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27832265','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27832265"><span>Prevalence of Semicircular Canal Hypoplasia in Patients With <span class="hlt">CHARGE</span> Syndrome: 3C Syndrome.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wineland, Andre; Menezes, Maithilee D; Shimony, Joshua S; Shinawi, Marwan S; Hullar, Timothy E; Hirose, Keiko</p> <p>2017-02-01</p> <p><span class="hlt">CHARGE</span> syndrome refers to a syndrome involving coloboma, heart defects, atresia choanae, retardation of growth and development, genitourinary disorders, and ear anomalies. However, Verloes revised the characteristics of <span class="hlt">CHARGE</span> syndrome in 2005 to define this syndrome more broadly. Deficiency of the semicircular canals is now a major criterion for <span class="hlt">CHARGE</span> syndrome. To characterize patients with <span class="hlt">CHARGE</span> syndrome at our center using Verloes' criteria and to reevaluate the nomenclature for this condition. We performed a medical chart review of patients with <span class="hlt">CHARGE</span> syndrome and reviewed their temporal bone imaging studies at a tertiary care children's hospital affiliated with Washington University in St Louis. Two authors independently reviewed each imaging study (A.W. and K.H.). Radiologic studies, physical findings, genetic tests, and other diagnostic tests were included. Patients with no temporal bone imaging studies were excluded. Eighteen children were included in this study; 13 children (72%) were male, and the mean (median; range) age of patients at the time of inner ear imaging studies was 2 years (4.5 years; 8 months to 8 years). Coloboma was present in 13 patients (72%) and choanal atresia in 5 (28%); semicircular canal anomalies were present in all patients. <span class="hlt">Additionally</span>, 13 patients (72%) were diagnosed as having hindbrain anomalies, 17 (94%) as having endocrine disorders, 17 (94%) as having mediastinal organ malformations, and all as having middle or external ear abnormalities and development delay. Cleft lip and cleft palate were found in 6 of 14 patients (43%) who did not have choanal atresia. We tested 16 patients for mutations in the CHD7 gene; 10 were positive (63%) for mutations, 4 (25%) were <span class="hlt">negative</span>, and 2 (13%) were inconclusive. Semicircular canal anomalies were the most consistent finding in our patients with <span class="hlt">CHARGE</span> syndrome. Given the high prevalence of semicircular canal hypoplasia and importance of imaging for diagnosing <span class="hlt">CHARGE</span> syndrome, we</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EPJC...77..828B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EPJC...77..828B"><span>Electromagnetic dipole moments of <span class="hlt">charged</span> baryons with bent crystals at the LHC</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bagli, E.; Bandiera, L.; Cavoto, G.; Guidi, V.; Henry, L.; Marangotto, D.; Martinez Vidal, F.; Mazzolari, A.; Merli, A.; Neri, N.; Ruiz Vidal, J.</p> <p>2017-12-01</p> <p>We propose a unique program of measurements of electric and magnetic dipole moments of charm, beauty and strange <span class="hlt">charged</span> baryons at the LHC, based on the phenomenon of spin precession of channeled particles in bent crystals. Studies of crystal channeling and spin precession of positively- and <span class="hlt">negatively-charged</span> particles are presented, along with feasibility studies and expected sensitivities for the proposed experiment using a layout based on the LHCb detector.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1346581-transverse-mode-coupling-instability-threshold-space-charge-different-wakefields','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1346581-transverse-mode-coupling-instability-threshold-space-charge-different-wakefields"><span>Transverse mode coupling instability threshold with space <span class="hlt">charge</span> and different wakefields</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Balbekov, V.</p> <p></p> <p>Transverse mode coupling instability of a bunch with space <span class="hlt">charge</span> and wake field is considered in frameworks of the boxcar model. Eigenfunctions of the bunch without wake are used as the basis for solution of the equations with the wake field included. Dispersion equation for the bunch eigentunes is obtained in the form of an infinite continued fraction. It is shown that influence of space <span class="hlt">charge</span> on the instability essentially depends on the wake sign. In particular, threshold of the <span class="hlt">negative</span> wake increases in absolute value until the space <span class="hlt">charge</span> tune shift is rather small, and goes to zero atmore » higher space <span class="hlt">charge</span>. The explanation of this behavior is developed by analysis of the bunch spectrum. As a result, a comparison of the results with published articles is represented.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1346581-transverse-mode-coupling-instability-threshold-space-charge-different-wakefields','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1346581-transverse-mode-coupling-instability-threshold-space-charge-different-wakefields"><span>Transverse mode coupling instability threshold with space <span class="hlt">charge</span> and different wakefields</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Balbekov, V.</p> <p>2017-03-10</p> <p>Transverse mode coupling instability of a bunch with space <span class="hlt">charge</span> and wake field is considered in frameworks of the boxcar model. Eigenfunctions of the bunch without wake are used as the basis for solution of the equations with the wake field included. Dispersion equation for the bunch eigentunes is obtained in the form of an infinite continued fraction. It is shown that influence of space <span class="hlt">charge</span> on the instability essentially depends on the wake sign. In particular, threshold of the <span class="hlt">negative</span> wake increases in absolute value until the space <span class="hlt">charge</span> tune shift is rather small, and goes to zero atmore » higher space <span class="hlt">charge</span>. The explanation of this behavior is developed by analysis of the bunch spectrum. As a result, a comparison of the results with published articles is represented.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22611422-negative-charge-trapping-effects-al-sub-sub-films-grown-atomic-layer-deposition-onto-thermally-oxidized-sic','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22611422-negative-charge-trapping-effects-al-sub-sub-films-grown-atomic-layer-deposition-onto-thermally-oxidized-sic"><span><span class="hlt">Negative</span> <span class="hlt">charge</span> trapping effects in Al{sub 2}O{sub 3} films grown by atomic layer deposition onto thermally oxidized 4H-SiC</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Schilirò, Emanuela, E-mail: emanuela.schiliro@imm.cnr.it; Dipartimento di Scienze Chimiche, Università degli Studi di Catania, and INSTM udr Catania, viale Andrea Doria 6, 95125, Catania; Lo Nigro, Raffaella</p> <p></p> <p>This letter reports on the <span class="hlt">negative</span> <span class="hlt">charge</span> trapping in Al{sub 2}O{sub 3} thin films grown by atomic layer deposition onto oxidized silicon carbide (4H-SiC). The films exhibited a permittivity of 8.4, a breakdown field of 9.2 MV/cm and small hysteresis under moderate bias cycles. However, severe electron trapping inside the Al{sub 2}O{sub 3} film (1 × 10{sup 12} cm{sup −2}) occurs upon high positive bias stress (>10 V). Capacitance-voltage measurements at different temperatures and stress conditions have been used to determine an activation energy of 0.1 eV. The results provide indications on the possible nature of the trapping defects and,more » hence, on the strategies to improve this technology for 4H-SiC devices.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018OPP.....6....1A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018OPP.....6....1A"><span>The effect of PbS nanocrystal <span class="hlt">additives</span> on the <span class="hlt">charge</span> transfer state recombination in a bulk heterojunction blend</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Abdu-Aguye, Mustapha; Protesescu, Loredana; Dirin, Dmitry N.; Kovalenko, Maksym V.; Loi, Maria Antonietta</p> <p>2018-05-01</p> <p>A persistent limitation of organic semiconductors is their low dielectric constant єr, which limits the performance of bulk heterojunction (BHJ) solar cells. One way to increase єr is to employ high-єr <span class="hlt">additives</span>, such as PbS nanocrystals (QDs) to BHJ blends. In this work, we use the recombination of the interfacial <span class="hlt">charge</span> transfer (CT) state as a means to study the effects of PbS nanocrystals on blends of a narrow bandgap copolymer: poly[2,6-(4,4-bis-(2-ethylhexyl)-4H-cyclopenta[2,1- b;3,4-b']dithiophene)-alt-4,7-(2,1,3-benzothiadiazole)] (PCPDTBT), and phenyl-C61-butyric acid methyl ester (PCBM). We show that at low dilution levels (0.25% - 0.75% by weight), there is a decrease in the relative weight of the CT recombination lifetime (longer decay component); suggesting that there is an increase in the local єr of the ternary blend.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5738629','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5738629"><span>Probing the Surface <span class="hlt">Charge</span> on the Basal Planes of Kaolinite Particles with High-Resolution Atomic Force Microscopy</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p></p> <p>2017-01-01</p> <p>High-resolution atomic force microscopy is used to map the surface <span class="hlt">charge</span> on the basal planes of kaolinite nanoparticles in an ambient solution of variable pH and NaCl or CaCl2 concentration. Using DLVO theory with <span class="hlt">charge</span> regulation, we determine from the measured force–distance curves the surface <span class="hlt">charge</span> distribution on both the silica-like and the gibbsite-like basal plane of the kaolinite particles. We observe that both basal planes do carry <span class="hlt">charge</span> that varies with pH and salt concentration. The silica facet was found to be <span class="hlt">negatively</span> <span class="hlt">charged</span> at pH 4 and above, whereas the gibbsite facet is positively <span class="hlt">charged</span> at pH below 7 and <span class="hlt">negatively</span> <span class="hlt">charged</span> at pH above 7. Investigations in CaCl2 at pH 6 show that the surface <span class="hlt">charge</span> on the gibbsite facet increases for concentration up to 10 mM CaCl2 and starts to decrease upon further increasing the salt concentration to 50 mM. The increase of surface <span class="hlt">charge</span> at low concentration is explained by Ca2+ ion adsorption, while Cl– adsorption at higher CaCl2 concentrations partially neutralizes the surface <span class="hlt">charge</span>. Atomic resolution imaging and density functional theory calculations corroborate these observations. They show that hydrated Ca2+ ions can spontaneously adsorb on the gibbsite facet of the kaolinite particle and form ordered surface structures, while at higher concentrations Cl– ions will co-adsorb, thereby changing the observed ordered surface structure. PMID:29140711</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29140711','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29140711"><span>Probing the Surface <span class="hlt">Charge</span> on the Basal Planes of Kaolinite Particles with High-Resolution Atomic Force Microscopy.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kumar, N; Andersson, M P; van den Ende, D; Mugele, F; Siretanu, I</p> <p>2017-12-19</p> <p>High-resolution atomic force microscopy is used to map the surface <span class="hlt">charge</span> on the basal planes of kaolinite nanoparticles in an ambient solution of variable pH and NaCl or CaCl 2 concentration. Using DLVO theory with <span class="hlt">charge</span> regulation, we determine from the measured force-distance curves the surface <span class="hlt">charge</span> distribution on both the silica-like and the gibbsite-like basal plane of the kaolinite particles. We observe that both basal planes do carry <span class="hlt">charge</span> that varies with pH and salt concentration. The silica facet was found to be <span class="hlt">negatively</span> <span class="hlt">charged</span> at pH 4 and above, whereas the gibbsite facet is positively <span class="hlt">charged</span> at pH below 7 and <span class="hlt">negatively</span> <span class="hlt">charged</span> at pH above 7. Investigations in CaCl 2 at pH 6 show that the surface <span class="hlt">charge</span> on the gibbsite facet increases for concentration up to 10 mM CaCl 2 and starts to decrease upon further increasing the salt concentration to 50 mM. The increase of surface <span class="hlt">charge</span> at low concentration is explained by Ca 2+ ion adsorption, while Cl - adsorption at higher CaCl 2 concentrations partially neutralizes the surface <span class="hlt">charge</span>. Atomic resolution imaging and density functional theory calculations corroborate these observations. They show that hydrated Ca 2+ ions can spontaneously adsorb on the gibbsite facet of the kaolinite particle and form ordered surface structures, while at higher concentrations Cl - ions will co-adsorb, thereby changing the observed ordered surface structure.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=36008&Lab=ORD&keyword=corona&actType=&TIMSType=+&TIMSSubTypeID=&DEID=&epaNumber=&ntisID=&archiveStatus=Both&ombCat=Any&dateBeginCreated=&dateEndCreated=&dateBeginPublishedPresented=&dateEndPublishedPresented=&dateBeginUpdated=&dateEndUpdated=&dateBeginCompleted=&dateEndCompleted=&personID=&role=Any&journalID=&publisherID=&sortBy=revisionDate&count=50','EPA-EIMS'); return false;" href="https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=36008&Lab=ORD&keyword=corona&actType=&TIMSType=+&TIMSSubTypeID=&DEID=&epaNumber=&ntisID=&archiveStatus=Both&ombCat=Any&dateBeginCreated=&dateEndCreated=&dateBeginPublishedPresented=&dateEndPublishedPresented=&dateBeginUpdated=&dateEndUpdated=&dateBeginCompleted=&dateEndCompleted=&personID=&role=Any&journalID=&publisherID=&sortBy=revisionDate&count=50"><span><span class="hlt">CHARGE</span> MEASUREMENTS ON INDIVIDUAL PARTICLES EXITING LABORATORY PRECIPITATORS WITH POSITIVE AND <span class="hlt">NEGATIVE</span> CORONA AT VARIOUS TEMPERATURES</span></a></p> <p><a target="_blank" href="http://oaspub.epa.gov/eims/query.page">EPA Science Inventory</a></p> <p></p> <p></p> <p>The paper reports measurements of <span class="hlt">charge</span> values on individual particles exiting three different laboratory electrostatic precipitators (ESPs) in an experimental apparatus containing a Millikan cell. Dioctylphthalate (DOP) droplets and fly ash particles were measured at temperatur...</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li class="active"><span>23</span></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_23 --> <div id="page_24" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li class="active"><span>24</span></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="461"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=Electricity&pg=4&id=EJ1001303','ERIC'); return false;" href="https://eric.ed.gov/?q=Electricity&pg=4&id=EJ1001303"><span>Bipolar Transistors Can Detect <span class="hlt">Charge</span> in Electrostatic Experiments</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Dvorak, L.</p> <p>2012-01-01</p> <p>A simple <span class="hlt">charge</span> indicator with bipolar transistors is described that can be used in various electrostatic experiments. Its behaviour enables us to elucidate links between 'static electricity' and electric currents. In <span class="hlt">addition</span> it allows us to relate the sign of static <span class="hlt">charges</span> to the sign of the terminals of an ordinary battery. (Contains 7 figures…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014IJMPB..2850088M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014IJMPB..2850088M"><span>A temperature dependent study on <span class="hlt">charge</span> dynamics in organic molecular device: Effect of shallow traps on space <span class="hlt">charge</span> limited behavior</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mukherjee, A. K.; Kavala, A. K.</p> <p>2014-04-01</p> <p>Shallow traps play a significant role in influencing <span class="hlt">charge</span> dynamics through organic molecular thin films, such as pentacene. Sandwich cells of pentacene capped by gold electrodes are an excellent specimen to study the nature of underlying <span class="hlt">charge</span> dynamics. In this paper, self-consistent numerical simulation of I-V characteristics is performed at various temperatures. The results have revealed <span class="hlt">negative</span> value of Poole Frenkel coefficient. The location of trap energy level is found to be located at 0.24 eV above the highest occupied molecular orbit (HOMO) level of pentacene. Other physical parameters related to trap levels, such as density of states due to traps and effective carrier density due to traps, have also been estimated in this study.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/6512695','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/6512695"><span>Ionic currents and <span class="hlt">charge</span> movements in organ-cultured rat skeletal muscle.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Hollingworth, S; Marshall, M W; Robson, E</p> <p>1984-12-01</p> <p>The middle of the fibre voltage-clamp technique was used to measure ionic currents and non-linear <span class="hlt">charge</span> movements in intact, organ-cultured (in vitro denervated) mammalian fast-twitch (rat extensor digitorum longus) muscle fibres. Muscle fibres organ cultured for 4 days can be used as electrophysiological and morphological models for muscles in vivo denervated for the same length of time. Sodium currents in organ-cultured muscle fibres are similar to innervated fibres except that in the temperature range 0-20 degrees C (a) in the steady state, the voltage distribution of inactivation in cultured fibres is shifted <span class="hlt">negatively</span> some 20 mV; (b) at the same temperature and membrane potential, the time constant of inactivation in cultured fibres is about twice that of innervated fibres. Potassium currents in innervated and cultured fibres at 15 degrees C can be fitted with the Hodgkin-Huxley n variable raised to the second power. Despite the large range we would estimate that the maximum value of the steady-state potassium conductance of cultured fibres is about one-half that of innervated fibres. The estimated maximum amount of <span class="hlt">charge</span> moved in cultured fibre is about one-third that in innervated fibres. Compared to innervated fibres, culturing doubles the kinetics of the decay phase of <span class="hlt">charge</span> movement. The possibility of a <span class="hlt">negative</span> shift of the voltage distribution of <span class="hlt">charge</span> movements in cultured fibres is discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20160008910','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20160008910"><span>Impact of Airspace <span class="hlt">Charges</span> on Transatlantic Aircraft Trajectories</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Sridhar, Banavar; Ng, Hok K.; Linke, Florian; Chen, Neil Y.</p> <p>2015-01-01</p> <p>Aircraft flying over the airspace of different countries are subject to over-flight <span class="hlt">charges</span>. These <span class="hlt">charges</span> vary from country to country. Airspace <span class="hlt">charges</span>, while necessary to support the communication, navigation and surveillance services, may lead to aircraft flying routes longer than wind-optimal routes and produce <span class="hlt">additional</span> carbon dioxide and other gaseous emissions. This paper develops an optimal route between city pairs by modifying the cost function to include an airspace cost whenever an aircraft flies through a controlled airspace without landing or departing from that airspace. It is assumed that the aircraft will fly the trajectory at a constant cruise altitude and constant speed. The computationally efficient optimal trajectory is derived by solving a non-linear optimal control problem. The operational strategies investigated in this study for minimizing aircraft fuel burn and emissions include flying fuel-optimal routes and flying cost-optimal routes that may completely or partially reduce airspace <span class="hlt">charges</span> en route. The results in this paper use traffic data for transatlantic flights during July 2012. The mean daily savings in over-flight <span class="hlt">charges</span>, fuel cost and total operation cost during the period are 17.6 percent, 1.6 percent, and 2.4 percent respectively, along the cost- optimal trajectories. The transatlantic flights can potentially save $600,000 in fuel cost plus $360,000 in over-flight <span class="hlt">charges</span> daily by flying the cost-optimal trajectories. In <span class="hlt">addition</span>, the aircraft emissions can be potentially reduced by 2,070 metric tons each day. The airport pairs and airspace regions that have the highest potential impacts due to airspace <span class="hlt">charges</span> are identified for possible reduction of fuel burn and aircraft emissions for the transatlantic flights. The results in the paper show that the impact of the variation in fuel price on the optimal routes is to reduce the difference between wind-optimal and cost-optimal routes as the fuel price increases. The</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20369881','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20369881"><span>Aggregation and <span class="hlt">charge</span> behavior of metallic and nonmetallic nanoparticles in the presence of competing similarly-<span class="hlt">charged</span> inorganic ions.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Mukherjee, Biplab; Weaver, James W</p> <p>2010-05-01</p> <p>The influence of competing, similarly <span class="hlt">charged</span>, inorganic ions on the size and <span class="hlt">charge</span> behavior of suspended titanium-dioxide (nTiO(2)), silver (nAg) and fullerene (nC(60)) nanoparticles (NPs) was investigated. Under pH and ionic conditions similar to natural water bodies, Ca(2+) induced aggregation of nTiO(2) and nAg NPs more strongly than K(+) and Na(+). Although K(+) and Na(+) had a similar effect on aggregation, K(+) provided better screening of the particle surface <span class="hlt">charge</span> presumably because of its small hydrated radius. These effects were decidedly more prominent for TiO(2) than Ag. Anions (co-ions), SO(4)(2-) and Cl(-), affected the surface <span class="hlt">charge</span> behavior of nTiO(2) but not of nAg NPs. The zeta potential (ZP) of nTiO(2) NPs was more <span class="hlt">negative</span> at higher SO(4)(2-)/Cl(-) ratios than lower. When Mg(2+) was the counterion, <span class="hlt">charge</span> inversion and rapid aggregation of nC(60) NPs occurred under alkaline conditions, with a more pronounced effect for Cl(-) than SO(4)(2-). Response dissimilarities suggest fundamental differences in the interfacial-interaction characteristics of these NPs in the aquatic environment with corresponding differences in transport of these particles. Our study also shows the important role played by the iso-electric point pH (pH(iep)) of the NPs in determining their aggregation kinetics in the environment.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1996AIPC..380....3R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1996AIPC..380....3R"><span>Study of <span class="hlt">negative</span> ion transport phenomena in a plasma source</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Riz, D.; Paméla, J.</p> <p>1996-07-01</p> <p>NIETZSCHE (<span class="hlt">Negative</span> Ions Extraction and Transport ZSimulation Code for HydrogEn species) is a <span class="hlt">negative</span> ion (NI) transport code developed at Cadarache. This code calculates NI trajectories using a 3D Monte-Carlo technique, taking into account the main destruction processes, as well as elastic collisions (H-/H+) and <span class="hlt">charge</span> exchanges (H-/H0). It determines the extraction probability of a NI created at a given position. According to the simulations, we have seen that in the case of volume production, only NI produced close to the plasma grid (PG) can be extracted. Concerning the surface production, we have studied how NI produced on the PG and accelerated by the plasma sheath backward into the source could be extracted. We demonstrate that elastic collisions and <span class="hlt">charge</span> exchanges play an important role, which in some conditions dominates the magnetic filter effect, which acts as a magnetic mirror. NI transport in various conditions will be discussed: volume/surface production, high/low plasmas density, tent filter/transverse filter.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JPS...367..237B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JPS...367..237B"><span>Enabling fast <span class="hlt">charging</span> - Infrastructure and economic considerations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Burnham, Andrew; Dufek, Eric J.; Stephens, Thomas; Francfort, James; Michelbacher, Christopher; Carlson, Richard B.; Zhang, Jiucai; Vijayagopal, Ram; Dias, Fernando; Mohanpurkar, Manish; Scoffield, Don; Hardy, Keith; Shirk, Matthew; Hovsapian, Rob; Ahmed, Shabbir; Bloom, Ira; Jansen, Andrew N.; Keyser, Matthew; Kreuzer, Cory; Markel, Anthony; Meintz, Andrew; Pesaran, Ahmad; Tanim, Tanvir R.</p> <p>2017-11-01</p> <p>The ability to <span class="hlt">charge</span> battery electric vehicles (BEVs) on a time scale that is on par with the time to fuel an internal combustion engine vehicle (ICEV) would remove a significant barrier to the adoption of BEVs. However, for viability, fast <span class="hlt">charging</span> at this time scale needs to also occur at a price that is acceptable to consumers. Therefore, the cost drivers for both BEV owners and <span class="hlt">charging</span> station providers are analyzed. In <span class="hlt">addition</span>, key infrastructure considerations are examined, including grid stability and delivery of power, the design of fast <span class="hlt">charging</span> stations and the design and use of electric vehicle service equipment. Each of these aspects have technical barriers that need to be addressed, and are directly linked to economic impacts to use and implementation. This discussion focuses on both the economic and infrastructure issues which exist and need to be addressed for the effective implementation of fast <span class="hlt">charging</span> at 400 kW and above. In so doing, it has been found that there is a distinct need to effectively manage the intermittent, high power demand of fast <span class="hlt">charging</span>, strategically plan infrastructure corridors, and to further understand the cost of operation of <span class="hlt">charging</span> infrastructure and BEVs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.afdc.energy.gov/case/2832','SCIGOVWS'); return false;" href="https://www.afdc.energy.gov/case/2832"><span>Alternative Fuels Data Center: DC Fast <span class="hlt">Charging</span> at the Workplace:</span></a></p> <p><a target="_blank" href="http://www.science.gov/aboutsearch.html">Science.gov Websites</a></p> <p></p> <p></p> <p>alleviate <span class="hlt">charging</span> congestion <em>when</em> there are more PEV drivers than Level 1 or 2 <span class="hlt">charging</span> at a worksite. DCFC can also be beneficial in emergencies or other situations <em>when</em> PEV drivers do not have time to <span class="hlt">charge</span> electrical capacity for the DCFC's <em>high</em> power needs. There may also be <span class="hlt">additional</span> costs to permitting or</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006IJMSp.253..156R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006IJMSp.253..156R"><span>Positive and <span class="hlt">negative</span> ion mode ESI-MS and MS/MS for studying drug-DNA complexes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rosu, Frédéric; Pirotte, Sophie; Pauw, Edwin De; Gabelica, Valérie</p> <p>2006-07-01</p> <p>We report systematic investigation of duplex DNA complexes with minor groove binders (Hoechsts 33258 and 33342, netropsin and DAPI) and intercalators (daunomycin, doxorubicin, actinomycin D, ethidium, cryptolepine, neocryptolepine, m-Amsacrine, proflavine, ellipticine and mitoxantrone) by ESI-MS and ESI-MS/MS in the <span class="hlt">negative</span> ion mode and in the positive ion mode. The apparent solution phase equilibrium binding constants can be determined by measuring relative intensities in the ESI-MS spectrum. While <span class="hlt">negative</span> ion mode gives reliable results, positive ion mode gives a systematic underestimation of the binding constants and even a complete suppression of the complexes for intercalators lacking functional groups capable of interacting in the grooves. In the second part of the paper we systematically compare MS/MS fragmentation channels and breakdown curves in the positive and the <span class="hlt">negative</span> modes, and discuss the possible uses and caveats of MS/MS in drug-DNA complexes. In the <span class="hlt">negative</span> mode, the drugs can be separated in three groups: (1) those that leave the complex with no net <span class="hlt">charge</span>; (2) those that leave the complex with a <span class="hlt">negative</span> <span class="hlt">charge</span>; and (3) those that remain attached on the strands upon dissociation of the duplex due to their positive <span class="hlt">charge</span>. In the positive ion mode, all complexes fragment via the loss of protonated drug. Information on the stabilization of the complex by drug-DNA noncovalent interactions can be obtained straightforwardly only in the case of neutral drug loss. In all other cases, proton affinity (in the positive ion mode), gas-phase basicity (in the <span class="hlt">negative</span> ion mode) and coulombic repulsion are the major factors influencing the fragmentation channel and the dissociation kinetics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMAE22A..03W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMAE22A..03W"><span>Why does <span class="hlt">negative</span> CG lightning have subsequent return strokes?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wilkes, R. A.; Kotovsky, D. A.; Uman, M. A.; Carvalho, F. L.; Jordan, D.</p> <p>2017-12-01</p> <p>It is not understood why cloud-to-ground (CG) lightning flashes lowering <span class="hlt">negative</span> <span class="hlt">charge</span> often produce discrete dart-leader/return-stroke sequences rather than having the first stroke drain the available cloud <span class="hlt">charge</span>, as is almost always the case for CG lightning lowering positive <span class="hlt">charge</span>. Triggered lightning data obtained at the International Center for Lightning Research and Testing (ICLRT) in north-central Florida have been analyzed to clarify the subsequent return-stroke process. In summers 2013 through 2016 at the ICLRT, 53% of the rocket launches did not initiate any part of a lightning flash, 13% of the rocket launches created an initial stage only (ISO) and failed to produce a following dart-leader/return-stroke sequences, and 34% of rocket launches produced an initial stage (IS) followed by return strokes. The IS of the triggered lightning consists of the upward positive leader and a following initial continuing current, both being responsible for transporting <span class="hlt">negative</span> <span class="hlt">charge</span> from the cloud to ground. Our ISO events may well have some commonality with the roughly 20 percent of natural CG flashes that fail to produce a dart-leader/return-stroke. We have analyzed the IS of 41 triggered lightning flashes with (19 cases) and without (22 cases) following return strokes and compared areas and heights of the flash using data collected by a Lightning Mapping Array (LMA). In our preliminary analysis, we can find no geometrical feature of the lightning channel during the IS that will predict the occurrence or lack of occurrence of following return strokes. We also have compared the triggered-lightning electrical current and <span class="hlt">charge</span> transfer observed at the ground. We found that the average current, duration, and <span class="hlt">charge</span> transfer during the IS for ISO events is each about half that of ISs analyzed which are followed by dart-leader/return-stroke sequences, contrary to the results presented from the GCOELD in China. Summarizing, there appear to be no differences in the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/21266457-rocket-borne-mass-analyzer-charged-aerosol-particles-mesosphere','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/21266457-rocket-borne-mass-analyzer-charged-aerosol-particles-mesosphere"><span>A rocket-borne mass analyzer for <span class="hlt">charged</span> aerosol particles in the mesosphere</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Knappmiller, Scott; Robertson, Scott; Sternovsky, Zoltan</p> <p>2008-10-15</p> <p>An electrostatic mass spectrometer for nanometer-sized <span class="hlt">charged</span> aerosol particles in the mesosphere has been developed and tested. The analyzer is mounted on the forward end of a rocket and has a slit opening for admitting a continuous sample of air that is exhausted through ports at the sides. Within the instrument housing are two sets of four collection plates that are biased with positive and <span class="hlt">negative</span> voltages for the collection of <span class="hlt">negative</span> and positive aerosol particles, respectively. Each collection plate spans about an order of magnitude in mass which corresponds to a factor of 2 in radius. The number densitymore » of the <span class="hlt">charge</span> is calculated from the current collected by the plates. The mean free path for molecular collisions in the mesosphere is comparable to the size of the instrument opening; thus, the analyzer performance is modeled by a Monte Carlo computer code that finds the aerosol particles trajectories within the instrument including both the electrostatic force and the forces from collisions of the aerosol particles with air molecules. Mass sensitivity curves obtained using the computer models are near to those obtained in the laboratory using an ion source. The first two flights of the instrument returned data showing the <span class="hlt">charge</span> number densities of both positive and <span class="hlt">negative</span> aerosol particles in four mass ranges.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27720635','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27720635"><span>Isolated effects of external bath osmolality, solute concentration, and electrical <span class="hlt">charge</span> on solute transport across articular cartilage.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Pouran, Behdad; Arbabi, Vahid; Zadpoor, Amir A; Weinans, Harrie</p> <p>2016-12-01</p> <p>The metabolic function of cartilage primarily depends on transport of solutes through diffusion mechanism. In the current study, we use contrast enhanced micro-computed tomography to determine equilibrium concentration of solutes through different cartilage zones and solute flux in the cartilage, using osteochondral plugs from equine femoral condyles. Diffusion experiments were performed with two solutes of different <span class="hlt">charge</span> and approximately equal molecular weight, namely iodixanol (neutral) and ioxaglate (<span class="hlt">charge</span>=-1) in order to isolate the effects of solute's <span class="hlt">charge</span> on diffusion. Furthermore, solute concentrations as well as bath osmolality were changed to isolate the effects of steric hindrance on diffusion. Bath concentration and bath osmolality only had minor effects on the diffusion of the neutral solute through cartilage at the surface, middle and deep zones, indicating that the diffusion of the neutral solute was mainly Fickian. The <span class="hlt">negatively</span> <span class="hlt">charged</span> solute diffused considerably slower through cartilage than the neutral solute, indicating a large non-Fickian contribution in the diffusion of <span class="hlt">charged</span> molecules. The numerical models determined maximum solute flux in the superficial zone up to a factor of 2.5 lower for the <span class="hlt">negatively</span> <span class="hlt">charged</span> solutes (<span class="hlt">charge</span>=-1) as compared to the neutral solutes confirming the importance of <span class="hlt">charge</span>-matrix interaction in diffusion of molecules across cartilage. Copyright © 2016 IPEM. Published by Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22340171-revised-big-bang-nucleosynthesis-long-lived-negatively-charged-massive-particles-updated-recombination-rates-primordial-sup-nucleosynthesis-impact-new-sup-li-limits','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22340171-revised-big-bang-nucleosynthesis-long-lived-negatively-charged-massive-particles-updated-recombination-rates-primordial-sup-nucleosynthesis-impact-new-sup-li-limits"><span>REVISED BIG BANG NUCLEOSYNTHESIS WITH LONG-LIVED, <span class="hlt">NEGATIVELY</span> <span class="hlt">CHARGED</span> MASSIVE PARTICLES: UPDATED RECOMBINATION RATES, PRIMORDIAL {sup 9}Be NUCLEOSYNTHESIS, AND IMPACT OF NEW {sup 6}Li LIMITS</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Kusakabe, Motohiko; Kim, K. S.; Cheoun, Myung-Ki</p> <p></p> <p>We extensively reanalyze the effects of a long-lived, <span class="hlt">negatively</span> <span class="hlt">charged</span> massive particle, X {sup –}, on big bang nucleosynthesis (BBN). The BBN model with an X {sup –} particle was originally motivated by the discrepancy between the {sup 6,} {sup 7}Li abundances predicted in the standard BBN model and those inferred from observations of metal-poor stars. In this model, {sup 7}Be is destroyed via the recombination with an X {sup –} particle followed by radiative proton capture. We calculate precise rates for the radiative recombinations of {sup 7}Be, {sup 7}Li, {sup 9}Be, and {sup 4}He with X {sup –}. Inmore » nonresonant rates, we take into account respective partial waves of scattering states and respective bound states. The finite sizes of nuclear <span class="hlt">charge</span> distributions cause deviations in wave functions from those of point-<span class="hlt">charge</span> nuclei. For a heavy X {sup –} mass, m{sub X} ≳ 100 GeV, the d-wave → 2P transition is most important for {sup 7}Li and {sup 7,} {sup 9}Be, unlike recombination with electrons. Our new nonresonant rate of the {sup 7}Be recombination for m{sub X} = 1000 GeV is more than six times larger than the existing rate. Moreover, we suggest a new important reaction for {sup 9}Be production: the recombination of {sup 7}Li and X {sup –} followed by deuteron capture. We derive binding energies of X nuclei along with reaction rates and Q values. We then calculate BBN and find that the amount of {sup 7}Be destruction depends significantly on the <span class="hlt">charge</span> distribution of {sup 7}Be. Finally, updated constraints on the initial abundance and the lifetime of the X {sup –} are derived in the context of revised upper limits to the primordial {sup 6}Li abundance. Parameter regions for the solution to the {sup 7}Li problem and the primordial {sup 9}Be abundances are revised.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20200752','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20200752"><span>A new battery-<span class="hlt">charging</span> method suggested by molecular dynamics simulations.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Abou Hamad, Ibrahim; Novotny, M A; Wipf, D O; Rikvold, P A</p> <p>2010-03-20</p> <p>Based on large-scale molecular dynamics simulations, we propose a new <span class="hlt">charging</span> method that should be capable of <span class="hlt">charging</span> a lithium-ion battery in a fraction of the time needed when using traditional methods. This <span class="hlt">charging</span> method uses an <span class="hlt">additional</span> applied oscillatory electric field. Our simulation results show that this <span class="hlt">charging</span> method offers a great reduction in the average intercalation time for Li(+) ions, which dominates the <span class="hlt">charging</span> time. The oscillating field not only increases the diffusion rate of Li(+) ions in the electrolyte but, more importantly, also enhances intercalation by lowering the corresponding overall energy barrier.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29733605','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29733605"><span>Effect of Surface Hydration on Antifouling Properties of Mixed <span class="hlt">Charged</span> Polymers.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Leng, Chuan; Huang, Hao; Zhang, Kexin; Hung, Hsiang-Chieh; Xu, Yao; Li, Yaoxin; Jiang, Shaoyi; Chen, Zhan</p> <p>2018-05-07</p> <p>Interfacial water structure on a polymer surface in water (or surface hydration) is related to the antifouling activity of the polymer. Zwitterionic polymer materials exhibit excellent antifouling activity due to their strong surface hydration. It was proposed to replace zwitterionic polymers using mixed <span class="hlt">charged</span> polymers because it is much easier to prepare mixed <span class="hlt">charged</span> polymer samples with much lower costs. In this study, using sum frequency generation (SFG) vibrational spectroscopy, we investigated interfacial water structures on mixed <span class="hlt">charged</span> polymer surfaces in water, and how such structures change while exposing to salt solutions and protein solutions. The 1:1 mixed <span class="hlt">charged</span> polymer exhibits excellent antifouling property while other mixed <span class="hlt">charged</span> polymers with different ratios of the positive/<span class="hlt">negative</span> <span class="hlt">charges</span> do not. It was found that on the 1:1 mixed <span class="hlt">charged</span> polymer surface, SFG water signal is dominated by the contribution of the strongly hydrogen bonded water molecules, indicating strong hydration of the polymer surface. The responses of the 1:1 mixed <span class="hlt">charged</span> polymer surface to salt solutions are similar to those of zwitterionic polymers. Interestingly, exposure to high concentrations of salt solutions leads to stronger hydration of the 1:1 mixed <span class="hlt">charged</span> polymer surface after replacing the salt solution with water. Protein molecules do not substantially perturb the interfacial water structure on the 1:1 mixed <span class="hlt">charged</span> polymer surface and do not adsorb to the surface, showing that this mixed <span class="hlt">charged</span> polymer is an excellent antifouling material.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=1396124','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=1396124"><span>Fixed <span class="hlt">charge</span> in the cell membrane</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Elul, R.</p> <p>1967-01-01</p> <p>1. Focal electric field was generated by passing a current of 5 × 10-7 to 1 × 10-5 A from a micropipette into the culture medium. Movement of cells at a distance of 5-50 μ from the electrode tip was observed. In case of cells embedded in the culture only local deformation of the membrane was observed. 2. The cell species explored included neurones, glia, muscle fibres, connective cells, malignant cells and erythrocytes. All cells responded in a similar manner to the electric field, and the current required was in the same range. 3. Cells were attracted to a positive micropipette and repelled from a <span class="hlt">negative</span> one: the only exception was observed in certain malignant cells which moved in the opposite direction. 4. Movement and membrane deformation could be obtained with electrodes filled with various concentrated and isotonic solutions. The composition of the culture medium also had no qualitative influence on these effects. 5. Metabolic poisons or rupture of the cell membrane had no effect on the movement. Isolated membrane fragments showed movement similar to that of intact cells. 6. The possibility of artifacts due to proximity of the focal electrode is considered. It is shown that electro-osmosis cannot account for the present observations. Some other artifacts are also excluded. 7. It is proposed that the most satisfactory way to account for the present observations is by a membrane carrying <span class="hlt">negative</span> fixed <span class="hlt">charge</span> of the order of 2·5 × 103 e.s.u./cm2. Some physiological consequences of presence of <span class="hlt">negative</span> <span class="hlt">charge</span> in the membrane are briefly discussed. ImagesFig. 1Fig. 2Fig. 3 PMID:6040152</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28959051','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28959051"><span><span class="hlt">Additive</span> <span class="hlt">negative</span> effects of anthropogenic sedimentation and warming on the survival of coral recruits.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Fourney, Francesca; Figueiredo, Joana</p> <p>2017-09-28</p> <p>Corals worldwide are facing population declines due to global climate change and local anthropogenic impacts. Global climate change effects are hard to tackle but recent studies show that some coral species can better handle climate change stress when provided with <span class="hlt">additional</span> energy resources. The local stressor that most undermines energy acquisition is sedimentation because it impedes coral heterotrophic feeding and their ability to photosynthesize. To investigate if reducing local sedimentation will enable corals to better endure ocean warming, we quantitatively assessed the combined effects of increased temperature and sedimentation (concentration and turbidity) on the survival of coral recruits of the species, Porites astreoides. We used sediment from a reef and a boat basin to mimic natural sediment (coarse) and anthropogenic (fine) sediment (common in dredging), respectively. Natural sediment did not <span class="hlt">negatively</span> impact coral survival, but anthropogenic sediment did. We found that the capacity of coral recruits to survive under warmer temperatures is less compromised when anthropogenic sedimentation is maintained at the lowest level (30 mg.cm -2 ). Our study suggests that a reduction of US-EPA allowable turbidity from 29 Nephelometric Turbidity Units (NTU) above background to less than 7 NTU near coral reefs would facilitate coral recruit survival under current and higher temperatures.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016APS..APRC15007G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016APS..APRC15007G"><span>Nonlinear evolution and final fate of (<span class="hlt">charged</span>) superradiant instability</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Green, Stephen; Bosch, Pablo; Lehner, Luis</p> <p>2016-03-01</p> <p>We describe the full nonlinear development of the superradiant instability for a <span class="hlt">charged</span> massless scalar field, coupled to general relativity and electromagnetism, in the vicinity of a Reissner-Nordstrom-AdS black hole. The presence of the <span class="hlt">negative</span> cosmological constant provides a natural context for considering perfectly reflecting boundary conditions and studying the dynamics as the scalar field interacts repeateadly with the black hole. At early times, small superradiant perturbations grow as expected from linearized studies. Backreaction then causes the black hole to lose <span class="hlt">charge</span> and mass until the perturbation becomes nonsuperradiant, with the final state described by a stable hairy black hole. For large gauge coupling, the instability extracts a large amount of <span class="hlt">charge</span> per unit mass, resulting in greater entropy increase. We discuss the implications of the observed behavior for the general problem of superradiance in black hole spacetimes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29904093','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29904093"><span>Multi-material <span class="hlt">Additive</span> Manufacturing of Metamaterials with Giant, Tailorable <span class="hlt">Negative</span> Poisson's Ratios.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Chen, Da; Zheng, Xiaoyu</p> <p>2018-06-14</p> <p>Nature has evolved with a recurring strategy to achieve unusual mechanical properties through coupling variable elastic moduli from a few GPa to below KPa within a single tissue. The ability to produce multi-material, three-dimensional (3D) micro-architectures with high fidelity incorporating dissimilar components has been a major challenge in man-made materials. Here we show multi-modulus metamaterials whose architectural element is comprised of encoded elasticity ranging from rigid to soft. We found that, in contrast to ordinary architected materials whose <span class="hlt">negative</span> Poisson's ratio is dictated by their geometry, these type of metamaterials are capable of displaying Poisson's ratios from extreme <span class="hlt">negative</span> to zero, independent of their 3D micro-architecture. The resulting low density metamaterials is capable of achieving functionally graded, distributed strain amplification capabilities within the metamaterial with uniform micro-architectures. Simultaneous tuning of Poisson's ratio and moduli within the 3D multi-materials could open up a broad array of material by design applications ranging from flexible armor, artificial muscles, to actuators and bio-mimetic materials.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1239696-spacecraft-surface-charging-within-geosynchronous-orbit-observed-van-allen-probes','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1239696-spacecraft-surface-charging-within-geosynchronous-orbit-observed-van-allen-probes"><span>Spacecraft surface <span class="hlt">charging</span> within geosynchronous orbit observed by the Van Allen Probes</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Sarno-Smith, Lois K.; Larsen, Brian A.; Skoug, Ruth M.; ...</p> <p>2016-02-27</p> <p>Using the Helium Oxygen Proton Electron (HOPE) and Electric Field and Waves (EFW) instruments from the Van Allen Probes, we explored the relationship between electron energy fluxes in the eV and keV ranges and spacecraft surface <span class="hlt">charging</span>. We present statistical results on spacecraft <span class="hlt">charging</span> within geosynchronous orbit by L and MLT. An algorithm to extract the H+ <span class="hlt">charging</span> line in the HOPE instrument data was developed to better explore intense <span class="hlt">charging</span> events. Also, this study explored how spacecraft potential relates to electron number density, electron pressure, electron temperature, thermal electron current, and low-energy ion density between 1 and 210 eV.more » It is demonstrated that it is imperative to use both EFW potential measurements and the HOPE instrument ion <span class="hlt">charging</span> line for examining times of extreme spacecraft <span class="hlt">charging</span> of the Van Allen Probes. The results of this study show that elevated electron energy fluxes and high-electron pressures are present during times of spacecraft <span class="hlt">charging</span> but these same conditions may also occur during noncharging times. Furthermore, we also show noneclipse significant <span class="hlt">negative</span> <span class="hlt">charging</span> events on the Van Allen Probes.« less</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li class="active"><span>24</span></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_24 --> <div id="page_25" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li class="active"><span>25</span></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="481"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006GeCoA..70..267C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006GeCoA..70..267C"><span>Acid base activity of live bacteria: Implications for quantifying cell wall <span class="hlt">charge</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Claessens, Jacqueline; van Lith, Yvonne; Laverman, Anniet M.; Van Cappellen, Philippe</p> <p>2006-01-01</p> <p>To distinguish the buffering capacity associated with functional groups in the cell wall from that resulting from metabolic processes, base or acid consumption by live and dead cells of the Gram-<span class="hlt">negative</span> bacterium Shewanella putrefaciens was measured in a pH stat system. Live cells exhibited fast consumption of acid (pH 4) or base (pH 7, 8, 9, and 10) during the first few minutes of the experiments. At pH 5.5, no acid or base was required to maintain the initial pH constant. The initial amounts of acid or base consumed by the live cells at pH 4, 8, and 10 were of comparable magnitudes as those neutralized at the same pHs by intact cells killed by exposure to gamma radiation or ethanol. Cells disrupted in a French press required higher amounts of acid or base, due to <span class="hlt">additional</span> buffering by intracellular constituents. At pH 4, acid neutralization by suspensions of live cells stopped after 50 min, because of loss of viability. In contrast, under neutral and alkaline conditions, base consumption continued for the entire duration of the experiments (5 h). This long-term base neutralization was, at least partly, due to active respiration by the cells, as indicated by the build-up of succinate in solution. Qualitatively, the acid-base activity of live cells of the Gram-positive bacterium Bacillus subtilis resembled that of S. putrefaciens. The pH-dependent <span class="hlt">charging</span> of ionizable functional groups in the cell walls of the live bacteria was estimated from the initial amounts of acid or base consumed in the pH stat experiments. From pH 4 to 10, the cell wall <span class="hlt">charge</span> increased from near-zero values to about -4 × 10 -16 mol cell -1 and -6.5 × 10 -16 mol cell -1 for S. putrefaciens and B. subtilis, respectively. The similar cell wall <span class="hlt">charging</span> of the two bacterial strains is consistent with the inferred low contribution of lipopolysaccharides to the buffering capacity of the Gram-<span class="hlt">negative</span> cell wall (of the order of 10%).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23784258','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23784258"><span><span class="hlt">Negative</span> quantum capacitance induced by midgap states in single-layer graphene.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wang, Lin; Wang, Yang; Chen, Xiaolong; Zhu, Wei; Zhu, Chao; Wu, Zefei; Han, Yu; Zhang, Mingwei; Li, Wei; He, Yuheng; Xiong, Wei; Law, Kam Tuen; Su, Dangsheng; Wang, Ning</p> <p>2013-01-01</p> <p>We demonstrate that single-layer graphene (SLG) decorated with a high density of Ag adatoms displays the unconventional phenomenon of <span class="hlt">negative</span> quantum capacitance. The Ag adatoms act as resonant impurities and form nearly dispersionless resonant impurity bands near the <span class="hlt">charge</span> neutrality point (CNP). Resonant impurities quench the kinetic energy and drive the electrons to the Coulomb energy dominated regime with <span class="hlt">negative</span> compressibility. In the absence of a magnetic field, <span class="hlt">negative</span> quantum capacitance is observed near the CNP. In the quantum Hall regime, <span class="hlt">negative</span> quantum capacitance behavior at several Landau level positions is displayed, which is associated with the quenching of kinetic energy by the formation of Landau levels. The <span class="hlt">negative</span> quantum capacitance effect near the CNP is further enhanced in the presence of Landau levels due to the magnetic-field-enhanced Coulomb interactions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3687226','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3687226"><span><span class="hlt">Negative</span> Quantum Capacitance Induced by Midgap States in Single-layer Graphene</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Wang, Lin; Wang, Yang; Chen, Xiaolong; Zhu, Wei; Zhu, Chao; Wu, Zefei; Han, Yu; Zhang, Mingwei; Li, Wei; He, Yuheng; Xiong, Wei; Law, Kam Tuen; Su, Dangsheng; Wang, Ning</p> <p>2013-01-01</p> <p>We demonstrate that single-layer graphene (SLG) decorated with a high density of Ag adatoms displays the unconventional phenomenon of <span class="hlt">negative</span> quantum capacitance. The Ag adatoms act as resonant impurities and form nearly dispersionless resonant impurity bands near the <span class="hlt">charge</span> neutrality point (CNP). Resonant impurities quench the kinetic energy and drive the electrons to the Coulomb energy dominated regime with <span class="hlt">negative</span> compressibility. In the absence of a magnetic field, <span class="hlt">negative</span> quantum capacitance is observed near the CNP. In the quantum Hall regime, <span class="hlt">negative</span> quantum capacitance behavior at several Landau level positions is displayed, which is associated with the quenching of kinetic energy by the formation of Landau levels. The <span class="hlt">negative</span> quantum capacitance effect near the CNP is further enhanced in the presence of Landau levels due to the magnetic-field-enhanced Coulomb interactions. PMID:23784258</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23589580','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23589580"><span>S1-S3 counter <span class="hlt">charges</span> in the voltage sensor module of a mammalian sodium channel regulate fast inactivation.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Groome, James R; Winston, Vern</p> <p>2013-05-01</p> <p>The movement of positively <span class="hlt">charged</span> S4 segments through the electric field drives the voltage-dependent gating of ion channels. Studies of prokaryotic sodium channels provide a mechanistic view of activation facilitated by electrostatic interactions of <span class="hlt">negatively</span> <span class="hlt">charged</span> residues in S1 and S2 segments, with positive counterparts in the S4 segment. In mammalian sodium channels, S4 segments promote domain-specific functions that include activation and several forms of inactivation. We tested the idea that S1-S3 countercharges regulate eukaryotic sodium channel functions, including fast inactivation. Using structural data provided by bacterial channels, we constructed homology models of the S1-S4 voltage sensor module (VSM) for each domain of the mammalian skeletal muscle sodium channel hNaV1.4. These show that side chains of putative countercharges in hNaV1.4 are oriented toward the positive <span class="hlt">charge</span> complement of S4. We used mutagenesis to define the roles of conserved residues in the extracellular <span class="hlt">negative</span> <span class="hlt">charge</span> cluster (ENC), hydrophobic <span class="hlt">charge</span> region (HCR), and intracellular <span class="hlt">negative</span> <span class="hlt">charge</span> cluster (INC). Activation was inhibited with <span class="hlt">charge</span>-reversing VSM mutations in domains I-III. <span class="hlt">Charge</span> reversal of ENC residues in domains III (E1051R, D1069K) and IV (E1373K, N1389K) destabilized fast inactivation by decreasing its probability, slowing entry, and accelerating recovery. Several INC mutations increased inactivation from closed states and slowed recovery. Our results extend the functional characterization of VSM countercharges to fast inactivation, and support the premise that these residues play a critical role in domain-specific gating transitions for a mammalian sodium channel.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25723372','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25723372"><span>Quantifying reactivity for electrophilic aromatic substitution reactions with Hirshfeld <span class="hlt">charge</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Liu, Shubin</p> <p>2015-03-26</p> <p>An electrophilic aromatic substitution is a process where one atom or group on an aromatic ring is replaced by an incoming electrophile. The reactivity and regioselectivity of this category of reactions is significantly impacted by the group that is already attached to the aromatic ring. Groups promoting substitution at the ortho/para and meta position are called ortho/para and meta directing groups, respectively. Earlier, we have shown that regioselectivity of the electrophilic aromatic substitution is dictated by the nucleophilicity of the substituted aromatic ring, which is proportional to the Hirshfeld <span class="hlt">charge</span> on the regioselective site. Ortho/para directing groups have the largest <span class="hlt">negative</span> <span class="hlt">charge</span> values at the ortho/para positions, whereas meta directing groups often have the largest <span class="hlt">negative</span> <span class="hlt">charge</span> value at the meta position. The electron donation or acceptance feature of a substitution group is irrelevant to the regioselectivity. In this contribution, we extend our previous study by quantifying the reactivity for this kind of reactions. To that end, we examine the transition-state structure and activation energy of an identity reaction for a series of monosubstituted-benzene molecules reacting with hydrogen fluoride using BF3 as the catalyst in the gas phase. A total of 18 substitution groups will be considered, nine of which are ortho/para directing and the other nine groups meta directing. From this study, we found that the barrier height of these reactions strongly correlates with the Hirshfeld <span class="hlt">charge</span> on the regioselective site for both ortho/para and meta directing groups, with the correlation coefficient R(2) both better than 0.96. We also discovered a less accurate correlation between the barrier height and HOMO energy. These results reconfirm the validity and effectiveness of employing the Hirshfeld <span class="hlt">charge</span> as a reliable descriptor of both reactivity and regioselectivity for this vastly important category of chemical transformations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=schizophrenia&pg=5&id=EJ954534','ERIC'); return false;" href="https://eric.ed.gov/?q=schizophrenia&pg=5&id=EJ954534"><span>Schizophrenia and Crime: How Predictable Are <span class="hlt">Charges</span>, Convictions and Violence?</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Heinrichs, R. Walter; Sam, Eleanor P.</p> <p>2012-01-01</p> <p>The schizophrenia-crime relationship was studied in 151 research participants meeting DSM-IV criteria for schizophrenia or schizoaffective disorder and with histories positive or <span class="hlt">negative</span> for criminal <span class="hlt">charges</span>, convictions and offences involving violence. These crime-related variables were regressed on a block of nine predictors reflecting…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23679138','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23679138"><span>Controlling electrostatic <span class="hlt">charging</span> of nanocrystalline diamond at nanoscale.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Verveniotis, Elisseos; Kromka, Alexander; Rezek, Bohuslav</p> <p>2013-06-11</p> <p>Constant electrical current in the range of -1 to -200 pA is applied by an atomic force microscope (AFM) in contact mode regime to induce and study local electrostatic <span class="hlt">charging</span> of oxygen-terminated nanocrystalline diamond (NCD) thin films. The NCD films are deposited on silicon in 70 nm thickness and with 60% relative sp(2) phase content. <span class="hlt">Charging</span> current is monitored by conductive AFM. Electric potential contrast induced by the current is evaluated by Kelvin force microscopy (KFM). KFM shows well-defined, homogeneous, and reproducible microscopic patterns that are not influenced by inherent tip-surface junction fluctuations during the <span class="hlt">charging</span> process. The <span class="hlt">charged</span> patterns are persistent for at least 72 h due to <span class="hlt">charge</span> trapping inside the NCD film. The current-induced <span class="hlt">charging</span> also clearly reveals field-induced detrapping at current amplitudes >-50 pA and tip instability at >-150 pA, both of which limit the achievable potential contrast. In <span class="hlt">addition</span>, we show that the field also determines the range of electronic states that can trap the <span class="hlt">charge</span>. We present a model and discuss implications for control of the nanoscale <span class="hlt">charging</span> process.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/863281','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/863281"><span>Method for forming electrically <span class="hlt">charged</span> laser targets</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Goodman, Ronald K.; Hunt, Angus L.</p> <p>1979-01-01</p> <p>Electrically chargeable laser targets and method for forming such <span class="hlt">charged</span> targets in order to improve their guidance along a predetermined desired trajectory. This is accomplished by the incorporation of a small amount of an <span class="hlt">additive</span> to the target material which will increase the electrical conductivity thereof, and thereby enhance the <span class="hlt">charge</span> placed upon the target material for guidance thereof by electrostatic or magnetic steering mechanisms, without adversely affecting the target when illuminated by laser energy.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19905021','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19905021"><span>Effect of headgroup size, <span class="hlt">charge</span>, and solvent structure on polymer-micelle interactions, studied by molecular dynamics simulations.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Shang, Barry Z; Wang, Zuowei; Larson, Ronald G</p> <p>2009-11-19</p> <p>We performed atomistic molecular dynamics simulations of anionic and cationic micelles in the presence of poly(ethylene oxide) (PEO) to understand why nonionic water-soluble polymers such as PEO interact strongly with anionic micelles but only weakly with cationic micelles. Our micelles include sodium n-dodecyl sulfate (SDS), n-dodecyl trimethylammonium chloride (DTAC), n-dodecyl ammonium chloride (DAC), and micelles in which we artificially reverse the sign of partial <span class="hlt">charges</span> in SDS and DTAC. We observe that the polymer interacts hydrophobically with anionic SDS but only weakly with cationic DTAC and DAC, in agreement with experiment. However, the polymer also interacts with the artificial anionic DTAC but fails to interact hydrophobically with the artificial cationic SDS, illustrating that large headgroup size does not explain the weak polymer interaction with cationic micelles. In <span class="hlt">addition</span>, we observe through simulation that this preference for interaction with anionic micelles still exists in a dipolar "dumbbell" solvent, indicating that water structure and hydrogen bonding alone cannot explain this preferential interaction. Our simulations suggest that direct electrostatic interactions between the micelle and polymer explain the preference for interaction with anionic micelles, even though the polymer overall carries no net <span class="hlt">charge</span>. This is possible given the asymmetric distribution of <span class="hlt">negative</span> <span class="hlt">charges</span> on smaller atoms and positive <span class="hlt">charges</span> on larger units in the polymer chain.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JEMat..45.5334B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JEMat..45.5334B"><span>Simulation of Space <span class="hlt">Charge</span> Dynamic in Polyethylene Under DC Continuous Electrical Stress</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Boukhari, Hamed; Rogti, Fatiha</p> <p>2016-10-01</p> <p>The space <span class="hlt">charge</span> dynamic plays a very important role in the aging and breakdown of polymeric insulation materials under high voltage. This is due to the intensification of the local electric field and the attendant chemical-mechanical effects in the vicinity around the trapped <span class="hlt">charge</span>. In this paper, we have investigated the space <span class="hlt">charge</span> dynamic in low-density polyethylene under high direct-current voltage, which is evaluated by experimental conditions. The evaluation is on the basis of simulation using a bipolar <span class="hlt">charge</span> transport model consisting of <span class="hlt">charge</span> injection, transports, trapping, detrapping, and recombination phenomena. The theoretical formulation of the physical problem is based on the Poisson, the continuity, and the transport equations. Numerical results provide temporal and local distributions of the electric field, the space <span class="hlt">charge</span> density for the different kinds of <span class="hlt">charges</span> (net <span class="hlt">charge</span> density, mobile and trapped of electron density, mobile hole density), conduction and displacement current densities, and the external current. The result shows the appearance of the <span class="hlt">negative</span> packet-like space <span class="hlt">charge</span> with a large amount of the bulk under the dc electric field of 100 kV/mm, and the induced distortion of the electric field is largely near to the anode, about 39% higher than the initial electric field applied.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvB..97o5123S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvB..97o5123S"><span>Numerical renormalization group method for entanglement <span class="hlt">negativity</span> at finite temperature</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shim, Jeongmin; Sim, H.-S.; Lee, Seung-Sup B.</p> <p>2018-04-01</p> <p>We develop a numerical method to compute the <span class="hlt">negativity</span>, an entanglement measure for mixed states, between the impurity and the bath in quantum impurity systems at finite temperature. We construct a thermal density matrix by using the numerical renormalization group (NRG), and evaluate the <span class="hlt">negativity</span> by implementing the NRG approximation that reduces computational cost exponentially. We apply the method to the single-impurity Kondo model and the single-impurity Anderson model. In the Kondo model, the <span class="hlt">negativity</span> exhibits a power-law scaling at temperature much lower than the Kondo temperature and a sudden death at high temperature. In the Anderson model, the <span class="hlt">charge</span> fluctuation of the impurity contributes to the <span class="hlt">negativity</span> even at zero temperature when the on-site Coulomb repulsion of the impurity is finite, while at low temperature the <span class="hlt">negativity</span> between the impurity spin and the bath exhibits the same power-law scaling behavior as in the Kondo model.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28787163','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28787163"><span>Structure and Electronic Properties of Neutral and <span class="hlt">Negatively</span> <span class="hlt">Charged</span> RhBn Clusters (n = 3-10): A Density Functional Theory Study.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Li, Peifang; Mei, Tingting; Lv, Linxia; Lu, Cheng; Wang, Weihua; Bao, Gang; Gutsev, Gennady L</p> <p>2017-08-31</p> <p>The geometrical structure and electronic properties of the neutral RhB n and singly <span class="hlt">negatively</span> <span class="hlt">charged</span> RhB n - clusters are obtained in the range of 3 ≤ n ≤ 10 using the unbiased CALYPSO structure search method and density functional theory (DFT). A combination of the PBE0 functional and the def2-TZVP basis set is used for determining global minima on potential energy surfaces of the Rh-doped B n clusters. The photoelectron spectra of the anions are simulated using the time-dependent density functional theory (TD-DFT) method. Good agreement between our simulated and experimentally obtained photoelectron spectra for RhB 9 - provides support to the validity of our theoretical method. The relative stabilities of the ground-state RhB n and RhB n - clusters are estimated using the calculated binding energies, second-order total energy differences, and HOMO-LUMO gaps. It is found that RhB 7 and RhB 8 - are the most stable species in the neutral and anionic series, respectively. The chemical bonding analysis reveals that the RhB 8 - cluster possesses two sets of delocalized σ and π bonds. In both cases, the Hückel 4N + 2 rule is fulfilled and this cluster possesses both σ and π aromaticities.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20120013151','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120013151"><span>Models for Cometary Comae Containing <span class="hlt">Negative</span> Ions</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Cordiner, M. A.; Charnley, S. B.</p> <p>2012-01-01</p> <p>The presence of <span class="hlt">negative</span> ions (anions) in cometary comae is known from Giotto mass spectrometry of IP/Halley. The anions O(-), OH(-), C(-), CH(-) and CN(-) have been detected, as well as unidentified anions with masses 22-65 and 85-110 amu [I]. Organic molecular anions such as C4H(-) and C6H(-) are known to have a significant impact on the <span class="hlt">charge</span> balance of interstellar clouds and circumstellar envelopes and have been shown to act as catalysts for the gas phase synthesis of larger hydrocarbon molecules in the ISM, but their importance in cometary comae has not yet been fully explored. We present details of our new models for the chemistry of cometary comae that include atomic and molecular anions. We calculate the impact of these anions on the <span class="hlt">charge</span> balance and examine their importance for cometary coma chemistry.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28319867','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28319867"><span>Phototherapeutic spectrum expansion through synergistic effect of mesoporous silica trio-nanohybrids against antibiotic-resistant gram-<span class="hlt">negative</span> bacterium.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kuthati, Yaswanth; Kankala, Ranjith Kumar; Busa, Prabhakar; Lin, Shi-Xiang; Deng, Jin-Pei; Mou, Chung-Yuan; Lee, Chia-Hung</p> <p>2017-04-01</p> <p>The extensive impact of antibiotic resistance has led to the exploration of new anti-bacterial modalities. We designed copper impregnated mesoporous silica nanoparticles (Cu-MSN) with immobilizing silver nanoparticles (SNPs) to apply photodynamic inactivation (PDI) of antibiotic-resistant E. coli. SNPs were decorated over the Cu-MSN surfaces by coordination of silver ions on diamine-functionalized Cu-MSN and further reduced to silver nanoparticles with formalin. We demonstrate that silver is capable of sensitizing the gram-<span class="hlt">negative</span> bacteria E. coli to a gram-positive specific phototherapeutic agent in vitro; thereby expanding curcumin's phototherapeutic spectrum. The mesoporous structure of Cu-MSN remains intact after the exterior decoration with silver nanoparticles and subsequent curcumin loading through an enhanced effect from copper metal-curcumin affinity interaction. The synthesis, as well as successful assembly of the functional nanomaterials, was confirmed by various physical characterization techniques. Curcumin is capable of producing high amounts of reactive oxygen species (ROS) under light irradiation, which can further improve the silver ion release kinetics for antibacterial activity. In <span class="hlt">addition</span>, the positive <span class="hlt">charged</span> modified surfaces of Cu-MSN facilitate antimicrobial response through electrostatic attractions towards <span class="hlt">negatively</span> <span class="hlt">charged</span> bacterial cell membranes. The antibacterial action of the synthesized nanocomposites can be activated through a synergistic mechanism of energy transfer of the absorbed light from SNP to curcumin. Copyright © 2017 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2000JAP....88.3601T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2000JAP....88.3601T"><span>Study of space <span class="hlt">charge</span> layer in silver bromide microcrystals by means of ultraviolet photoelectron spectroscopy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tani, Tadaaki; Inami, Yoshiyasu</p> <p>2000-09-01</p> <p>Ultraviolet photoelectron spectroscopy has been successfully used to measure the heights of the tops of the valence bands of the surfaces of AgBr layers on Ag substrates for the verification of the space <span class="hlt">charge</span> layer model. According to this model, the positive space <span class="hlt">charge</span> layer (composed of <span class="hlt">negative</span> <span class="hlt">charges</span> with excess <span class="hlt">negative</span> kink sites on the surface and corresponding positive <span class="hlt">charges</span> with interstitial silver ions in the interior) is formed in silver halides, causing the difference in the electronic energy levels between their surface and interior. The depression of the positive space <span class="hlt">charge</span> layer of AgBr caused by such adsorbates as photographic stabilizers and antifoggants was estimated from the decrease in the ionic conductivity of cubic AgBr microcrystals by the adsorbates. It was confirmed by the decrease in the heights of the tops of the valence bands of the surfaces of AgBr layers caused by the adsorbates in the presence of thin gelatin membranes on their surfaces. This result provided the explanation for the fact that the adsorbates increased the number of the microcrystals which formed latent image centers on the surface and decreased the number of the microcrystals, which formed latent image centers in the interior.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016Nanot..27A4005O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016Nanot..27A4005O"><span><span class="hlt">Charge</span>-state dynamics in electrostatic force spectroscopy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ondráček, Martin; Hapala, Prokop; Jelínek, Pavel</p> <p>2016-07-01</p> <p>We present a numerical model that allows us to study the response of an oscillating probe in electrostatic force spectroscopy to <span class="hlt">charge</span> switching in quantum dots at various time scales. The model provides more insight into the behavior of frequency shift and dissipated energy under different scanning conditions when measuring a temporarily <span class="hlt">charged</span> quantum dot on a surface. Namely, we analyze the dependence of the frequency shift, the dissipated energy, and their fluctuations on the resonance frequency of the tip and on the electron tunneling rates across the tip-quantum dot and quantum dot-sample junctions. We discuss two complementary approaches to simulating the <span class="hlt">charge</span> dynamics, a stochastic and a deterministic one. In <span class="hlt">addition</span>, we derive analytic formulas valid for small amplitudes, describing relations between the frequency shift, dissipated energy, and the characteristic rates driving the <span class="hlt">charging</span> and discharging processes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1996RScI...67.1221S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1996RScI...67.1221S"><span>Neutralization of space <span class="hlt">charge</span> forces using ionized background gas</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Steski, D. B.; Zarcone, M. J.; Smith, K. S.; Thieberger, P.</p> <p>1996-03-01</p> <p>The Tandem Van de Graaff at Brookhaven National Laboratory has delivered pulsed gold beam to the Alternating Gradient Synchrotron (AGS) and AGS Booster since 1992 for relativistic heavy ion physics. There is an ongoing effort to improve the quality and intensity of the <span class="hlt">negative</span> ion beam delivered to the Tandem from the present Cs sputter sources. Because the beam energy is low (approximately 30 keV) and the current high, there are significant losses due to space <span class="hlt">charge</span> forces. One of the ways being explored to overcome these losses is to neutralize the space <span class="hlt">charge</span> forces with ionized background gas. On an ion source test bench, using three different gases (Ar, N2, and Xe), the percentage of current transported from the source to a downstream Faraday cup was increased from 10% to 40% by bleeding in gas. Bleeding in Xe resulted in the best transmission. The time dependence of the neutralization as a function of gas pressure was also observed. This system is presently being transferred to the <span class="hlt">Negative</span> Ion Injector of the Tandem for use in upcoming heavy ion experiments.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018NJPh...20d3027G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018NJPh...20d3027G"><span>Spontaneous topological <span class="hlt">charging</span> of tactoids in a living nematic</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Genkin, Mikhail M.; Sokolov, Andrey; Aranson, Igor S.</p> <p>2018-04-01</p> <p>Living nematic is a realization of an active matter combining a nematic liquid crystal with swimming bacteria. The material exhibits a remarkable tendency towards spatio-temporal self-organization manifested in formation of dynamic textures of self-propelled half-integer topological defects (disclinations). Here we report on the study of such living nematic near normal inclusions, or tactoids, naturally realized in liquid crystals close to the isotropic-nematic (I–N) phase transition. On the basis of the computational analysis, we have established that tactoid’s I–N interface spontaneously acquire <span class="hlt">negative</span> topological <span class="hlt">charge</span> which is proportional to the tactoid’s size and depends on the concentration of bacteria. The observed <span class="hlt">negative</span> <span class="hlt">charging</span> is attributed to the drastic difference in the mobilities of +1/2 and ‑1/2 topological defects in active systems. The effect is described in the framework of a kinetic theory for point-like weakly-interacting defects with different mobilities. Our dedicated experiment fully confirmed the theoretical prediction. The results hint into new strategies for control of active matter.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015APS..MARZ50013W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015APS..MARZ50013W"><span>Observation of Iron Specific Interaction with a <span class="hlt">Charge</span> Neutral Phospholipid</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, Wenjie; Zhang, Honghu; Feng, Shuren; San Emeterio, Josue; Kuzmenko, Ivan; Nilsen-Hamilton, Marit; Mallapragada, Surya; Vaknin, David</p> <p>2015-03-01</p> <p>Using surface sensitive X-ray scattering and spectroscopic techniques we show that phosphatidyl choline (PC) head groups attract positively <span class="hlt">charged</span> iron ions and complexes even at pH values that are lower than 3. DPPC (1,2-dipalmitoyl-sn-glycero-3-phosphocholine) is a zwitterionic lipid typically used as a model system for cell membranes. Within a large pH range (3 -11), it carries a <span class="hlt">negative</span> <span class="hlt">charge</span> on the phosphate group and a positive <span class="hlt">charge</span> on the quaternary ammonium cation, thus appears <span class="hlt">charge</span> neutral. Further lowering the pH, i.e. adding a proton to the phosphate group, results in a positively <span class="hlt">charged</span> headgroup. Surprisingly, we detect significant enrichment of iron at the interface of the DPPC monolayer and the aqueous subphase with the pH maintained at 3 or even lower. With a supposedly <span class="hlt">charge</span> neutral or even positive surface, the observation of surface bound, <span class="hlt">charge</span> positive iron ions or iron hydroxides is counter-intuitive and suggests iron-specific interaction with the phospholipid headgroup, which is not governed by electrostatic interaction. The effect of the integration of Mms6, a membrane protein that promotes the formation of magnetic nanocrystals, into the DPPC monolayer will also be discussed. Research supported by the U.S. Department of Energy under Contract No. DE-AC02-07CH11358 and DE-AC02-06CH11357.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1021957-charging-properties-cassiterite-alfa-sno2-surfaces','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1021957-charging-properties-cassiterite-alfa-sno2-surfaces"><span><span class="hlt">Charging</span> properties of cassiterite (alfa-SnO2) surfaces</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Rosenqvist, Jorgen K; Machesky, Michael L.; Vlcek, L.</p> <p></p> <p>The acid-base properties of cassiterite (alfa-SnO2) surfaces at 10 50 C were studied using potentiometric titrations of powder suspensions in aqueous NaCl and RbCl media. The proton sorption isotherms exhibited common intersection points in the pH-range 4.0 to 4.5 at all conditions and the magnitude of <span class="hlt">charging</span> was similar but not identical in NaCl and RbCl. The hydrogen bonding configuration at the oxide-water interface, obtained from classical Molecular Dynamics (MD) simulations, was analyzed in detail and the results were explicitly incorporated in calculations of protonation constants for the reactive surface sites using the revised MUSIC model. The calculations indicated thatmore » the terminal SnOH2 group is more acidic than the bridging Sn2OH group, with protonation constants (log KH) of 3.60 and 5.13 at 25 C, respectively. This is contrary to the situation on the isostructural alfa-TiO2 (rutile), apparently due to the difference in electronegativity between Ti and Sn. MD simulations and speciation calculations indicated considerable differences in the speciation of Na+ and Rb+, despite the similarities in overall <span class="hlt">charging</span>. Adsorbed sodium ions are almost exclusively found in bidentate surface complexes, while adsorbed rubidium ions form comparable amounts of bidentate and tetradentate complexes. Also, the distribution of adsorbed Na+ between the different complexes shows a considerable dependence on surface <span class="hlt">charge</span> density (pH), while the distribution of adsorbed Rb+ is almost independent of pH. A Surface Complexation Model (SCM) capable of accurately describing both the measured surface <span class="hlt">charge</span> and the MD predicted speciation of adsorbed Na+/Rb+ was formulated. According to the SCM, the deprotonated terminal group (SnOH-0.40) and the protonated bridging group (Sn2OH+0.36) dominate the surface speciation over the entire pH-range (2.7 10), illustrating the ability of positively and <span class="hlt">negatively</span> <span class="hlt">charged</span> surface groups to coexist. Complexation of the medium</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li class="active"><span>25</span></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_25 --> <div class="footer-extlink text-muted" style="margin-bottom:1rem; text-align:center;">Some links on this page may take you to non-federal websites. 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