Sample records for charge medicale apres

  1. APR3 modulates oxidative stress and mitochondrial function in ARPE-19 cells.

    PubMed

    Li, Yuan; Zou, Xuan; Gao, Jing; Cao, Ke; Feng, Zhihui; Liu, Jiankang

    2018-05-24

    Impairment of retinal pigment epithelial (RPE) cells is considered a key contributor to the development of age-related macular degeneration. Apoptosis-related protein 3 (APR3) was recently discovered after treatment with all- trans retinoic acid, a pivotal molecule in RPE cells. However, the function of APR3 remains poorly understood. In the present study, we found that APR3 could interact with nuclear factor (erythroid-derived 2)-like 2, which is a regulator of phase II enzymes, and that knockdown of APR3 promoted nuclear factor (erythroid-derived 2)-like 2 nuclear translocation and activated expression of phase II enzymes, which was accompanied by improved redox status and mitochondrial activity. Overexpression of APR3 revealed its mitochondrial localization and induced a robust production of reactive oxygen species that was accompanied by impaired mitochondrial oxygen consumption, complex activity, and lower ATP content, resulting in significant changes in mitochondrial structure, which may contribute to cell apoptosis. High doses of all- trans retinoic acid treatment were found to significantly induce APR3 expression, increase reactive oxygen species levels, and decrease ATP content, which were abolished by knockdown of APR3. These results indicate that APR3 plays a vital role in regulating redox status and mitochondrial activity and thus suggest APR3 might be a potential novel target for study of treatment of age-related macular degeneration.-Li, Y., Zou, X., Gao, J., Cao, K., Feng, Z., Liu, J. APR3 modulates oxidative stress and mitochondrial function in ARPE-19 cells.

  2. The trauma registry compared to All Patient Refined Diagnosis Groups (APR-DRG).

    PubMed

    Hackworth, Jodi; Askegard-Giesmann, Johanna; Rouse, Thomas; Benneyworth, Brian

    2017-05-01

    Literature has shown there are significant differences between administrative databases and clinical registry data. Our objective was to compare the identification of trauma patients using All Patient Refined Diagnosis Related Groups (APR-DRG) as compared to the Trauma Registry and estimate the effects of those discrepancies on utilization. Admitted pediatric patients from 1/2012-12/2013 were abstracted from the trauma registry. The patients were linked to corresponding administrative data using the Pediatric Health Information System database at a single children's hospital. APR-DRGs referencing trauma were used to identify trauma patients. We compared variables related to utilization and diagnosis to determine the level of agreement between the two datasets. There were 1942 trauma registry patients and 980 administrative records identified with trauma-specific APR-DRG during the study period. Forty-two percent (816/1942) of registry records had an associated trauma-specific APR-DRG; 69% of registry patients requiring ICU care had trauma APR-DRGs; 73% of registry patients with head injuries had trauma APR-DRGs. Only 21% of registry patients requiring surgical management had associated trauma APR-DRGs, and 12.5% of simple fractures had associated trauma APR-DRGs. APR-DRGs appeared to only capture a fraction of the entire trauma population and it tends to be the more severely ill patients. As a result, the administrative data was not able to accurately answer hospital or operating room utilization as well as specific information on diagnosis categories regarding trauma patients. APR-DRG administrative data should not be used as the only data source for evaluating the needs of a trauma program. Copyright © 2016 Elsevier Ltd. All rights reserved.

  3. Reliability enhancement of APR + diverse protection system regarding common cause failures

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

    Oh, Y. G.; Kim, Y. M.; Yim, H. S.

    2012-07-01

    The Advanced Power Reactor Plus (APR +) nuclear power plant design has been developed on the basis of the APR1400 (Advanced Power Reactor 1400 MWe) to further enhance safety and economics. For the mitigation of Anticipated Transients Without Scram (ATWS) as well as Common Cause Failures (CCF) within the Plant Protection System (PPS) and the Emergency Safety Feature - Component Control System (ESF-CCS), several design improvement features have been implemented for the Diverse Protection System (DPS) of the APR + plant. As compared to the APR1400 DPS design, the APR + DPS has been designed to provide the Safety Injectionmore » Actuation Signal (SIAS) considering a large break LOCA accident concurrent with the CCF. Additionally several design improvement features, such as channel structure with redundant processing modules, and changes of system communication methods and auto-system test methods, are introduced to enhance the functional reliability of the DPS. Therefore, it is expected that the APR + DPS can provide an enhanced safety and reliability regarding possible CCF in the safety-grade I and C systems as well as the DPS itself. (authors)« less

  4. 78 FR 37531 - Agency Information Collection Activities; Comment Request; Annual Performance Reporting (APR...

    Federal Register 2010, 2011, 2012, 2013, 2014

    2013-06-21

    ...; Comment Request; Annual Performance Reporting (APR) System for NIDRR Grantees (RERCs, RRTCS, FIPs, ARRTs... of Collection: Annual Performance Reporting (APR) System for NIDRR Grantees (RERCs, RRTCS, FIPs... requests an extension of the Annual Performance Reporting (APR) System for NIDRR Grantees (RERCs, RRTCS...

  5. Evaluating SPP/APR Improvement Activities

    ERIC Educational Resources Information Center

    National Early Childhood Technical Assistance Center (NECTAC), 2009

    2009-01-01

    This document is intended to assist State Education Agency (SEA) and Lead Agency (LA) staff and technical assistance providers in designing a meaningful evaluation for the State Performance Plan (SPP)/Annual Performance Report (APR) improvement activities. It provides: (1) information about the relevance of evaluation in the context of improvement…

  6. Exercise Limitation Imposed by an Approved Air Purifying Respirator (APR)

    DTIC Science & Technology

    2010-05-01

    mentioned that they did not have enough time to inhale, that inspiratory muscles were fatigued , that they got out of rhythm with their breathing and...with APR decreased with time during APR use, a decrease suggesting fatigue of respiratory muscles . Another two subjects did not continue long enough... muscle fatigue , the difference they noted may have been caused by the increase in VE during endurance exercise. The other investigators compared at

  7. 48 CFR 1552.235-76 - Treatment of Confidential Business Information (APR 1996).

    Code of Federal Regulations, 2010 CFR

    2010-10-01

    ... Business Information (APR 1996). 1552.235-76 Section 1552.235-76 Federal Acquisition Regulations System... Provisions and Clauses 1552.235-76 Treatment of Confidential Business Information (APR 1996). As prescribed in 1535.007-70(c), insert the following clause: Treatment of Confidential Business Information (TSCA...

  8. Multiplex PCR to detect bacteriophages from natural whey cultures of buffalo milk and characterisation of two phages active against Lactococcus lactis, ΦApr-1 and ΦApr-2.

    PubMed

    Aprea, Giuseppe; Mullan, William Michael; Murru, Nicoletta; Fitzgerald, Gerald; Buonanno, Marialuisa; Cortesi, Maria Luisa; Prencipe, Vincenza Annunziata; Migliorati, Giacomo

    2017-09-30

    This work investigated bacteriophage induced starter failures in artisanal buffalo Mozzarella production plants in Southern Italy. Two hundred and ten samples of whey starter cultures were screened for bacteriophage infection. Multiplex polymerase chain reaction (PCR) revealed phage infection in 28.56% of samples, all showing acidification problems during cheese making. Based on DNA sequences, bacteriophages for Lactococcus lactis (L. lactis), Lactobacillus delbruekii (L. delbruekii) and Streptococcus thermophilus (S. thermophilus) were detected. Two phages active against L. lactis, ΦApr-1 and ΦApr-2, were isolated and characterised. The genomes, approximately 31.4 kb and 31 kb for ΦApr-1 and ΦApr-2 respectively, consisted of double-stranded linear DNA with pac-type system. Sodium dodecyl sulfate polyacrylamide gel electrophoresis (SDS‑PAGE) showed one major structural protein of approximately 32.5 kDa and several minor proteins. This is the first report of phage isolation in buffalo milk and of the use of multiplex PCR to screen and study the diversity of phages against Lactic Acid Bacteria (LAB) strains in artisanal Water Buffalo Mozzarella starters.

  9. 48 CFR 1552.235-75 - Access to Toxic Substances Control Act Confidential Business Information (APR 1996).

    Code of Federal Regulations, 2010 CFR

    2010-10-01

    ... Control Act Confidential Business Information (APR 1996). 1552.235-75 Section 1552.235-75 Federal... Confidential Business Information (APR 1996). As prescribed in 1535.007(b), insert the following provision: Access to Toxic Substances Control Act Confidential Business Information (APR 1996) In order to perform...

  10. Flexible Design and Operation of a Smart Charging Microgrid (Briefing Charts)

    DTIC Science & Technology

    2014-04-08

    release; distribution unlimited 13. SUPPLEMENTARY NOTES Briefing Charts for SAE World Congress 2014 14. ABSTRACT A microgrid is a controllable ...UNCLASSIFIED Distribution Statement A: Approved for Public Release Flexible Design and Operation of a Smart Charging Microgrid Annette G... control number. 1. REPORT DATE 08 APR 2014 2. REPORT TYPE Briefing Charts 3. DATES COVERED 08-01-2014 to 09-03-2014 4. TITLE AND SUBTITLE

  11. Development of Nanosatellite Technology with APRS Module for Disaster Mitigation

    NASA Astrophysics Data System (ADS)

    Prahyang, S. Y.; Dhiya’Ulhaq, M. Z.; Golim, O. P.; Gunawan, R.; Suhandinata; Jahja, E.; Nelwan, E. R. G.; Ananta, C.; Chow, I. M.; Mali, N. D. F.

    2018-05-01

    Development of nanosatellite technology has enabled satellites to be developed with multiple capabilities for a specific mission in a short time with a low cost. Satellite communications are proved to be more effective in delivering information due to its large coverage area. Surya Satellite-1 will become the first Indonesian nanosatellite developed by undergraduate students. It is designed with low-cost commercial payloads, including an APRS module for communication and operated on VHF and UHF amateur radio frequencies. The mission of the satellites focused on disaster mitigation through APRS communication network with remote stations located on disaster-prone areas.

  12. APR-246/PRIMA-1Met Inhibits and Reverses Squamous Metaplasia in Human Conjunctival Epithelium.

    PubMed

    Li, Jing; Li, Cheng; Wang, Guoliang; Liu, Zhen; Chen, Pei; Yang, Qichen; Dong, Nuo; Wu, Huping; Liu, Zuguo; Li, Wei

    2016-02-01

    Squamous metaplasia is a common pathologic condition in ocular surface diseases for which there is no therapeutic medication in clinic. In this study, we investigated the effect of a small molecule, APR-246/PRIMA-1(Met), on squamous metaplasia in human conjunctival epithelium. Human conjunctival explants were cultured for up to 12 days under airlifting conditions. Epithelial cell differentiation and proliferation were assessed by Cytokeratin 10 (K10), K14, K19, Pax6, MUC5AC, and p63 immunostaining patterns. β-catenin and TCF-4 immunofluorescent staining and real-time PCR characterized Wnt signaling pathway involvement. Pterygium clinical samples were cultured under airlifting conditions with or without APR-246 for 4 days. p63, K10, β-catenin, and TCF-4 expression in pterygial epithelium was determined by immunofluorescent staining and real-time PCR. Airlift conjunctival explants resulted in increased stratification and intrastromal epithelial invagination. Such pathology was accompanied by increases in K10, K14, and p63 expression, whereas K19 and Pax6 levels declined when compared to those in freshly isolated tissue. On the other hand, APR-246 reversed all of these declines in K10, K14, and p63 expression. Furthermore, K19 and Pax6 increased along with rises in goblet cell density. These effects of APR-246 were accompanied by near restoration of normal conjunctival epithelial histology. APR-246 also reversed squamous metaplasia in pterygial epithelium that had developed after 4 days in ex vivo culture. Reductions in squamous metaplasia induced by APR-246 suggest it may provide a novel therapeutic approach in different squamous metaplasia-associated ocular surface diseases.

  13. The Ongoing Rediscovery of Après-Coup as a Central Freudian Concept.

    PubMed

    House, Jonathan

    2017-10-01

    Après-coup, Freud's Nachträglichkeit, is an essential psychoanalytic concept structuring each of four concepts, four mental processes that lie at the foundation of Freud's thinking: psychic trauma, repression, the creation of the unconscious, and the creation of infantile sexuality. It is argued here that infantile sexual drives, in contrast to the self-preservative instincts, arise from a two-step process of translation and repression in which the residues of failed translation become source-objects of the drives. These residues of failed translation have an associative resonance with adult sexuality, and the child is driven to ongoing attempts to translate them, to make them meaningful après coup. Thus, après-coup is at the heart of the human subject as a sexual creature who requires, desires, and creates meaning.

  14. 12. Historic American Buildings Survey Arthur C. Haskell, Photographer Apr. ...

    Library of Congress Historic Buildings Survey, Historic Engineering Record, Historic Landscapes Survey

    12. Historic American Buildings Survey Arthur C. Haskell, Photographer Apr. 1, 1939 (l) INT.- STAIRWAY, 4th FLOOR, LOOKING SOUTH - M.I.T., Rogers Building, 491 Boylston Street, Boston, Suffolk County, MA

  15. 9. Historic American Buildings Survey Arthur C. Haskell, Photographer Apr. ...

    Library of Congress Historic Buildings Survey, Historic Engineering Record, Historic Landscapes Survey

    9. Historic American Buildings Survey Arthur C. Haskell, Photographer Apr. 1, 1939 (i) INT.- STAIR HALL, 1st. FLOOR, LOOKING NORTH - M.I.T., Rogers Building, 491 Boylston Street, Boston, Suffolk County, MA

  16. 14 CFR Appendix H to Part 23 - Installation of An Automatic Power Reserve (APR) System

    Code of Federal Regulations, 2010 CFR

    2010-01-01

    ... 14 Aeronautics and Space 1 2010-01-01 2010-01-01 false Installation of An Automatic Power Reserve (APR) System H Appendix H to Part 23 Aeronautics and Space FEDERAL AVIATION ADMINISTRATION, DEPARTMENT... AIRPLANES Pt. 23, App. H Appendix H to Part 23—Installation of An Automatic Power Reserve (APR) System H23.1...

  17. Human factors engineering verification and validation for APR1400 computerized control room

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

    Shin, Y. C.; Moon, H. K.; Kim, J. H.

    2006-07-01

    This paper introduces the Advanced Power Reactor 1400 (APR1400) HFE V and V activities the Korea Hydro Nuclear Plant Co. LTD. (KHNP) has performed for the last 10 years and some of the lessons learned through these activities. The features of APR1400 main control room include large display panel, redundant compact workstations, computer-based procedure, and safety console. Several iterations of human factors evaluations have been performed from small scale proof of concept tests to large scale integrated system tests for identifying human engineering deficiencies in the human system interface design. Evaluations in the proof of concept test were focused onmore » checking the presence of any show stopper problems in the design concept. Later evaluations were mostly for finding design problems and for assuring the resolution of human factors issues of advanced control room. The results of design evaluations were useful not only for refining the control room design, but also for licensing the standard design. Several versions of APR1400 mock-ups with dynamic simulation models of currently operating Korea Standard Nuclear Plant (KSNP) have been used for the evaluations with the participation of operators from KSNP plants. (authors)« less

  18. [Evaluation of the capacity of the APR-DRG classification system to predict hospital mortality].

    PubMed

    De Marco, Maria Francesca; Lorenzoni, Luca; Addari, Piero; Nante, Nicola

    2002-01-01

    Inpatient mortality has increasingly been used as an hospital outcome measure. Comparing mortality rates across hospitals requires adjustment for patient risks before making inferences about quality of care based on patient outcomes. Therefore it is essential to dispose of well performing severity measures. The aim of this study is to evaluate the ability of the All Patient Refined DRG system to predict inpatient mortality for congestive heart failure, myocardial infarction, pneumonia and ischemic stroke. Administrative records were used in this analysis. We used two statistics methods to assess the ability of the APR-DRG to predict mortality: the area under the receiver operating characteristics curve (referred to as the c-statistic) and the Hosmer-Lemeshow test. The database for the study included 19,212 discharges for stroke, pneumonia, myocardial infarction and congestive heart failure from fifteen hospital participating in the Italian APR-DRG Project. A multivariate analysis was performed to predict mortality for each condition in study using age, sex and APR-DRG risk mortality subclass as independent variables. Inpatient mortality rate ranges from 9.7% (pneumonia) to 16.7% (stroke). Model discrimination, calculated using the c-statistic, was 0.91 for myocardial infarction, 0.68 for stroke, 0.78 for pneumonia and 0.71 for congestive heart failure. The model calibration assessed using the Hosmer-Leme-show test was quite good. The performance of the APR-DRG scheme when used on Italian hospital activity records is similar to that reported in literature and it seems to improve by adding age and sex to the model. The APR-DRG system does not completely capture the effects of these variables. In some cases, the better performance might be due to the inclusion of specific complications in the risk-of-mortality subclass assignment.

  19. Review of APR+ Level 2 PSA. Revision 2

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

    Lehner, John R.; Mubayi, Vinod; Pratt, W. Trevor

    2012-02-17

    Brookhaven National Laboratory (BNL) assisted the Korea Institute of Nuclear Safety (KINS) in reviewing the Level 2 Probabilistic Safety Assessment (PSA) of the APR+ Advanced Pressurized Water Reactor (PWR) prepared by the Korea Hydro & Nuclear Power Co., Ltd (KHNP) and KEPCO Engineering & Construction Co., Inc. (KEPCO-E&C). The work described in this report involves a review of the APR+ Level 2 PSA submittal [Ref. 1]. The PSA and, therefore, the review is limited to consideration of accidents initiated by internal events. As part of the review process, the review team also developed three sets of Requests for Additional Informationmore » (RAIs). These RAIs were provided to KHNP and KEPCO-E&C for their evaluation and response. This final detailed report documents the review findings for each technical element of the PSA and includes consideration of all of the RAIs made by the reviewers as well as the associated responses. This final report was preceded by an interim report [Ref. 2] that focused on identifying important issues regarding the PSA. In addition, a final meeting on the project was held at BNL on November 21-22, 2011, where BNL and KINS reviewers discussed their preliminary review findings with KHNP and KEPCO-E&C staffs. Additional information obtained during this final meeting was also used to inform the review findings of this final report. The review focused not only on the robustness of the APR+ design to withstand severe accidents, but also on the capability and acceptability of the Level 2 PSA in terms of level of detail and completeness. The Korean nuclear regulatory authorities will decide whether the PSA is acceptable and the BNL review team is providing its comments for KINS consideration. Section 2.0 provides the basis for the BNL review. Section 3.0 presents the review of each technical element of the PSA. Conclusions and a summary are presented in Section 4.0. Section 5.0 contains the references.« less

  20. 81. Neg. No. F63, Apr 13, 1930, INTERIORASSEMBLY BUILDING, HOOD ...

    Library of Congress Historic Buildings Survey, Historic Engineering Record, Historic Landscapes Survey

    81. Neg. No. F-63, Apr 13, 1930, INTERIOR-ASSEMBLY BUILDING, HOOD DEPARTMENT - Ford Motor Company Long Beach Assembly Plant, Assembly Building, 700 Henry Ford Avenue, Long Beach, Los Angeles County, CA

  1. The Alberta Pregnancy Outcomes and Nutrition (APrON) cohort study: rationale and methods.

    PubMed

    Kaplan, Bonnie J; Giesbrecht, Gerald F; Leung, Brenda M Y; Field, Catherine J; Dewey, Deborah; Bell, Rhonda C; Manca, Donna P; O'Beirne, Maeve; Johnston, David W; Pop, Victor J; Singhal, Nalini; Gagnon, Lisa; Bernier, Francois P; Eliasziw, Misha; McCargar, Linda J; Kooistra, Libbe; Farmer, Anna; Cantell, Marja; Goonewardene, Laki; Casey, Linda M; Letourneau, Nicole; Martin, Jonathan W

    2014-01-01

    The Alberta Pregnancy Outcomes and Nutrition (APrON) study is an ongoing prospective cohort study that recruits pregnant women early in pregnancy and, as of 2012, is following up their infants to 3 years of age. It has currently enrolled approximately 5000 Canadians (2000 pregnant women, their offspring and many of their partners). The primary aims of the APrON study were to determine the relationships between maternal nutrient intake and status, before, during and after gestation, and (1) maternal mood; (2) birth and obstetric outcomes; and (3) infant neurodevelopment. We have collected comprehensive maternal nutrition, anthropometric, biological and mental health data at multiple points in the pregnancy and the post-partum period, as well as obstetrical, birth, health and neurodevelopmental outcomes of these pregnancies. The study continues to follow the infants through to 36 months of age. The current report describes the study design and methods, and findings of some pilot work. The APrON study is a significant resource with opportunities for collaboration. © 2012 John Wiley & Sons Ltd.

  2. 83. Neg. No. F53, Apr 13, 1930, INTERIORASSEMBLY BUILDING, BACK ...

    Library of Congress Historic Buildings Survey, Historic Engineering Record, Historic Landscapes Survey

    83. Neg. No. F-53, Apr 13, 1930, INTERIOR-ASSEMBLY BUILDING, BACK TRIM LINE - Ford Motor Company Long Beach Assembly Plant, Assembly Building, 700 Henry Ford Avenue, Long Beach, Los Angeles County, CA

  3. 86. Neg. No. F64, Apr 13, 1930, INTERIORASSEMBLY BUILDING, BODY ...

    Library of Congress Historic Buildings Survey, Historic Engineering Record, Historic Landscapes Survey

    86. Neg. No. F-64, Apr 13, 1930, INTERIOR-ASSEMBLY BUILDING, BODY STORAGE CONVEYOR - Ford Motor Company Long Beach Assembly Plant, Assembly Building, 700 Henry Ford Avenue, Long Beach, Los Angeles County, CA

  4. 15 CFR 782.1 - Overview of reporting requirements under the APR.

    Code of Federal Regulations, 2013 CFR

    2013-01-01

    ... Foreign Trade (Continued) BUREAU OF INDUSTRY AND SECURITY, DEPARTMENT OF COMMERCE ADDITIONAL PROTOCOL... (see § 782.5 of the APR). In addition, forms may be downloaded from the Internet at http://www.ap.gov. ...

  5. 15 CFR 782.1 - Overview of reporting requirements under the APR.

    Code of Federal Regulations, 2012 CFR

    2012-01-01

    ... Foreign Trade (Continued) BUREAU OF INDUSTRY AND SECURITY, DEPARTMENT OF COMMERCE ADDITIONAL PROTOCOL... (see § 782.5 of the APR). In addition, forms may be downloaded from the Internet at http://www.ap.gov. ...

  6. 15 CFR 782.1 - Overview of reporting requirements under the APR.

    Code of Federal Regulations, 2011 CFR

    2011-01-01

    ... Foreign Trade (Continued) BUREAU OF INDUSTRY AND SECURITY, DEPARTMENT OF COMMERCE ADDITIONAL PROTOCOL... (see § 782.5 of the APR). In addition, forms may be downloaded from the Internet at http://www.ap.gov. ...

  7. 15 CFR 782.1 - Overview of reporting requirements under the APR.

    Code of Federal Regulations, 2014 CFR

    2014-01-01

    ... Foreign Trade (Continued) BUREAU OF INDUSTRY AND SECURITY, DEPARTMENT OF COMMERCE ADDITIONAL PROTOCOL... (see § 782.5 of the APR). In addition, forms may be downloaded from the Internet at http://www.ap.gov. ...

  8. 85. Neg. No. F51, Apr 13, 1930, INTERIORASSEMBLY BUILDING, BODY ...

    Library of Congress Historic Buildings Survey, Historic Engineering Record, Historic Landscapes Survey

    85. Neg. No. F-51, Apr 13, 1930, INTERIOR-ASSEMBLY BUILDING, BODY AND CUSHION LINE - Ford Motor Company Long Beach Assembly Plant, Assembly Building, 700 Henry Ford Avenue, Long Beach, Los Angeles County, CA

  9. Assistant Personal Robot (APR): Conception and Application of a Tele-Operated Assisted Living Robot.

    PubMed

    Clotet, Eduard; Martínez, Dani; Moreno, Javier; Tresanchez, Marcel; Palacín, Jordi

    2016-04-28

    This paper presents the technical description, mechanical design, electronic components, software implementation and possible applications of a tele-operated mobile robot designed as an assisted living tool. This robotic concept has been named Assistant Personal Robot (or APR for short) and has been designed as a remotely telecontrolled robotic platform built to provide social and assistive services to elderly people and those with impaired mobility. The APR features a fast high-mobility motion system adapted for tele-operation in plain indoor areas, which incorporates a high-priority collision avoidance procedure. This paper presents the mechanical architecture, electrical fundaments and software implementation required in order to develop the main functionalities of an assistive robot. The APR uses a tablet in order to implement the basic peer-to-peer videoconference and tele-operation control combined with a tactile graphic user interface. The paper also presents the development of some applications proposed in the framework of an assisted living robot.

  10. 84. Neg. No. F62, Apr 13, 1930, INTERIORASSEMBLY BUILDING, FRAME ...

    Library of Congress Historic Buildings Survey, Historic Engineering Record, Historic Landscapes Survey

    84. Neg. No. F-62, Apr 13, 1930, INTERIOR-ASSEMBLY BUILDING, FRAME AND MOTOR STORAGE CONVEYOR - Ford Motor Company Long Beach Assembly Plant, Assembly Building, 700 Henry Ford Avenue, Long Beach, Los Angeles County, CA

  11. 76. Neg. No. F58, Apr 13, 1930, INTERIORASSEMBLY BUILDING, BURNOFF, ...

    Library of Congress Historic Buildings Survey, Historic Engineering Record, Historic Landscapes Survey

    76. Neg. No. F-58, Apr 13, 1930, INTERIOR-ASSEMBLY BUILDING, BURNOFF, LOAD END OF ENAMEL OVEN - Ford Motor Company Long Beach Assembly Plant, Assembly Building, 700 Henry Ford Avenue, Long Beach, Los Angeles County, CA

  12. New tools for NTD vaccines: A case study of quality control assays for product development of the human hookworm vaccine Na-APR-1M74.

    PubMed

    Pearson, Mark S; Jariwala, Amar R; Abbenante, Giovanni; Plieskatt, Jordan; Wilson, David; Bottazzi, Maria Elena; Hotez, Peter J; Keegan, Brian; Bethony, Jeffrey M; Loukas, Alex

    2015-01-01

    Na-APR-1(M74) is an aspartic protease that is rendered enzymatically inactive by site-directed mutagenesis and is a candidate antigen component in the Human Hookworm Vaccine. The mutant protease exerts vaccine efficacy by inducing antibodies that neutralize the enzymatic activity of wild type enzyme (Na-APR-1wt) in the gut of the hookworm, thereby depriving the worm of its ability to digest its blood meal. Previously, canines immunized with Na-APR-1(M74) and challenged with Ancylostoma caninum were partially protected against hookworm challenge infection, especially from the loss in hemoglobin observed in control canines and canine immunoglobulin (Ig) G raised against Na-APR-1 was shown to inhibit the enzymatic activity of Na-APR-1 wt in vitro, thereby providing proof of concept of Na-APR-1(M74) as a vaccine antigen. The mutated version, Na-APR-1(M74), was then expressed at the cGMP level using a Nicotiana benthamiana expression system (Fraunhofer, CMB, Delaware, MD), formulated with Alhydrogel®, and used to immunize mice in a dose-ranging study to explore the enzyme-neutralizing capacity of the resulting anti- Na-APR-1(M74) IgG. As little as 0.99 μg of recombinant Na-APR-1(M74) could induce anti Na-APR-1(M74) IgG in mice that were capable of inhibiting Na-APR-1w t-mediated digestion of a peptide substrate by 89%. In the absence of enzymatic activity of Na-APR-1(M74) as a surrogate marker of protein functionality, we developed an assay based on the binding of a quenched fluorescence-labeled inhibitor of aspartic proteases, BODIPY-FL pepstatin A (BDP). Binding of BDP in the active site of Na-APR-1 wt was demonstrated by inhibition of enzymatic activity, and competitive binding with unlabelled pepstatin A. BDP also bound to Na-APR-1(M74) which was assessed by fluorescence polarization, but with an ∼ 50-fold reduction in the dissociation constant. Taken together, these assays comprise a "toolbox" that could be useful for the analyses of Na-APR-1(M74) as it

  13. New tools for NTD vaccines: A case study of quality control assays for product development of the human hookworm vaccine Na-APR-1M74

    PubMed Central

    Pearson, Mark S; Jariwala, Amar R; Abbenante, Giovanni; Plieskatt, Jordan; Wilson, David; Bottazzi, Maria Elena; Hotez, Peter J; Keegan, Brian; Bethony, Jeffrey M; Loukas, Alex

    2015-01-01

    Na-APR-1M74 is an aspartic protease that is rendered enzymatically inactive by site-directed mutagenesis and is a candidate antigen component in the Human Hookworm Vaccine. The mutant protease exerts vaccine efficacy by inducing antibodies that neutralize the enzymatic activity of wild type enzyme (Na-APR-1wt) in the gut of the hookworm, thereby depriving the worm of its ability to digest its blood meal. Previously, canines immunized with Na-APR-1M74 and challenged with Ancylostoma caninum were partially protected against hookworm challenge infection, especially from the loss in hemoglobin observed in control canines and canine immunoglobulin (Ig) G raised against Na-APR-1 was shown to inhibit the enzymatic activity of Na-APR-1wt in vitro, thereby providing proof of concept of Na-APR-1M74 as a vaccine antigen. The mutated version, Na-APR-1M74, was then expressed at the cGMP level using a Nicotiana benthamiana expression system (Fraunhofer, CMB, Delaware, MD), formulated with Alhydrogel®, and used to immunize mice in a dose-ranging study to explore the enzyme-neutralizing capacity of the resulting anti- Na-APR-1M74 IgG. As little as 0.99 μg of recombinant Na-APR-1M74 could induce anti Na-APR-1M74 IgG in mice that were capable of inhibiting Na-APR-1wt-mediated digestion of a peptide substrate by 89%. In the absence of enzymatic activity of Na-APR-1M74 as a surrogate marker of protein functionality, we developed an assay based on the binding of a quenched fluorescence-labeled inhibitor of aspartic proteases, BODIPY-FL pepstatin A (BDP). Binding of BDP in the active site of Na-APR-1wt was demonstrated by inhibition of enzymatic activity, and competitive binding with unlabelled pepstatin A. BDP also bound to Na-APR-1M74 which was assessed by fluorescence polarization, but with an ∼50-fold reduction in the dissociation constant. Taken together, these assays comprise a “toolbox” that could be useful for the analyses of Na-APR-1M74 as it proceeds through the

  14. 15 CFR 782.5 - Where to obtain APR report forms.

    Code of Federal Regulations, 2010 CFR

    2010-01-01

    ... (Continued) BUREAU OF INDUSTRY AND SECURITY, DEPARTMENT OF COMMERCE ADDITIONAL PROTOCOL REGULATIONS GENERAL... forms required by the APR may be downloaded from the Internet at http://www.ap.gov. You also may obtain these forms by contacting: Treaty Compliance Division, Bureau of Industry and Security, U.S. Department...

  15. 15 CFR 782.5 - Where to obtain APR report forms.

    Code of Federal Regulations, 2013 CFR

    2013-01-01

    ... (Continued) BUREAU OF INDUSTRY AND SECURITY, DEPARTMENT OF COMMERCE ADDITIONAL PROTOCOL REGULATIONS GENERAL... forms required by the APR may be downloaded from the Internet at http://www.ap.gov. You also may obtain these forms by contacting: Treaty Compliance Division, Bureau of Industry and Security, U.S. Department...

  16. 15 CFR 782.5 - Where to obtain APR report forms.

    Code of Federal Regulations, 2011 CFR

    2011-01-01

    ... (Continued) BUREAU OF INDUSTRY AND SECURITY, DEPARTMENT OF COMMERCE ADDITIONAL PROTOCOL REGULATIONS GENERAL... forms required by the APR may be downloaded from the Internet at http://www.ap.gov. You also may obtain these forms by contacting: Treaty Compliance Division, Bureau of Industry and Security, U.S. Department...

  17. 15 CFR 782.5 - Where to obtain APR report forms.

    Code of Federal Regulations, 2012 CFR

    2012-01-01

    ... (Continued) BUREAU OF INDUSTRY AND SECURITY, DEPARTMENT OF COMMERCE ADDITIONAL PROTOCOL REGULATIONS GENERAL... forms required by the APR may be downloaded from the Internet at http://www.ap.gov. You also may obtain these forms by contacting: Treaty Compliance Division, Bureau of Industry and Security, U.S. Department...

  18. 15 CFR 782.5 - Where to obtain APR report forms.

    Code of Federal Regulations, 2014 CFR

    2014-01-01

    ... (Continued) BUREAU OF INDUSTRY AND SECURITY, DEPARTMENT OF COMMERCE ADDITIONAL PROTOCOL REGULATIONS GENERAL... forms required by the APR may be downloaded from the Internet at http://www.ap.gov. You also may obtain these forms by contacting: Treaty Compliance Division, Bureau of Industry and Security, U.S. Department...

  19. Après-Coup in French Psychoanalysis: The Long Afterlife of Nachträglichkeit: The First Hundred Years, 1893 to 1993.

    PubMed

    House, Jonathan; Slotnick, Julie

    2015-10-01

    Après-coup finds its origins in Freud's earliest psychoanalytic writings, but it was only half a century ago that French psychoanalysts rediscovered, clarified, and developed the concept and so brought it recognition as an essential Freudian concept. Because the history of après-coup is embedded in the French reading of Freud, this article will give an account of that reading in relation to après-coup.

  20. 79. Neg. No. F61A, Apr 13, 1930, INTERIORASSEMBLY BUILDING, BODY ...

    Library of Congress Historic Buildings Survey, Historic Engineering Record, Historic Landscapes Survey

    79. Neg. No. F-61A, Apr 13, 1930, INTERIOR-ASSEMBLY BUILDING, BODY CONSTRUCTION - Ford Motor Company Long Beach Assembly Plant, Assembly Building, 700 Henry Ford Avenue, Long Beach, Los Angeles County, CA

  1. 77. Neg. No. F65A, Apr 13, 1930, INTERIORASSEMBLY BUILDING, UNLOADING ...

    Library of Congress Historic Buildings Survey, Historic Engineering Record, Historic Landscapes Survey

    77. Neg. No. F-65A, Apr 13, 1930, INTERIOR-ASSEMBLY BUILDING, UNLOADING THE ENAMEL OVEN - Ford Motor Company Long Beach Assembly Plant, Assembly Building, 700 Henry Ford Avenue, Long Beach, Los Angeles County, CA

  2. 90. Neg. No. F59A, Apr 13, 1930, INTERIORASSEMBLY BUILDING, CHASSIS ...

    Library of Congress Historic Buildings Survey, Historic Engineering Record, Historic Landscapes Survey

    90. Neg. No. F-59A, Apr 13, 1930, INTERIOR-ASSEMBLY BUILDING, CHASSIS LINE, LOOKING SOUTH - Ford Motor Company Long Beach Assembly Plant, Assembly Building, 700 Henry Ford Avenue, Long Beach, Los Angeles County, CA

  3. 82. Neg. No. F66A, Apr 13, 1930, INTERIORASSEMBLY BUILDING, TRIM ...

    Library of Congress Historic Buildings Survey, Historic Engineering Record, Historic Landscapes Survey

    82. Neg. No. F-66A, Apr 13, 1930, INTERIOR-ASSEMBLY BUILDING, TRIM LINE AND GLASS DEPARTMENTS - Ford Motor Company Long Beach Assembly Plant, Assembly Building, 700 Henry Ford Avenue, Long Beach, Los Angeles County, CA

  4. 78. Neg. No. F143A, Apr 1, 1932, INTERIORASSEMBLY BUILDING, CONVEYOR ...

    Library of Congress Historic Buildings Survey, Historic Engineering Record, Historic Landscapes Survey

    78. Neg. No. F-143A, Apr 1, 1932, INTERIOR-ASSEMBLY BUILDING, CONVEYOR LINE WITH CAR CHASSIS - Ford Motor Company Long Beach Assembly Plant, Assembly Building, 700 Henry Ford Avenue, Long Beach, Los Angeles County, CA

  5. 15 CFR 782.1 - Overview of reporting requirements under the APR.

    Code of Federal Regulations, 2010 CFR

    2010-01-01

    ... 15 Commerce and Foreign Trade 2 2010-01-01 2010-01-01 false Overview of reporting requirements under the APR. 782.1 Section 782.1 Commerce and Foreign Trade Regulations Relating to Commerce and Foreign Trade (Continued) BUREAU OF INDUSTRY AND SECURITY, DEPARTMENT OF COMMERCE ADDITIONAL PROTOCOL...

  6. Main steam line break accident simulation of APR1400 using the model of ATLAS facility

    NASA Astrophysics Data System (ADS)

    Ekariansyah, A. S.; Deswandri; Sunaryo, Geni R.

    2018-02-01

    A main steam line break simulation for APR1400 as an advanced design of PWR has been performed using the RELAP5 code. The simulation was conducted in a model of thermal-hydraulic test facility called as ATLAS, which represents a scaled down facility of the APR1400 design. The main steam line break event is described in a open-access safety report document, in which initial conditions and assumptionsfor the analysis were utilized in performing the simulation and analysis of the selected parameter. The objective of this work was to conduct a benchmark activities by comparing the simulation results of the CESEC-III code as a conservative approach code with the results of RELAP5 as a best-estimate code. Based on the simulation results, a general similarity in the behavior of selected parameters was observed between the two codes. However the degree of accuracy still needs further research an analysis by comparing with the other best-estimate code. Uncertainties arising from the ATLAS model should be minimized by taking into account much more specific data in developing the APR1400 model.

  7. Le don après un décès d'origine cardiocirculatoire au Canada

    PubMed Central

    Shemie, Sam D.; Baker, Andrew J.; Knoll, Greg; Wall, William; Rocker, Graeme; Howes, Daniel; Davidson, Janet; Pagliarello, Joe; Chambers-Evans, Jane; Cockfield, Sandra; Farrell, Catherine; Glannon, Walter; Gourlay, William; Grant, David; Langevin, Stéphan; Wheelock, Brian; Young, Kimberly; Dossetor, John

    2006-01-01

    Résumé Ces recommandations sont le fruit d'un processus multidisciplinaire national ayant duré un an et visant à déterminer si et comment l'on pourrait procéder au don d'organes après un décès d'origine cardiocirculatoire («don après le décès cardiocirculatoire», ou DDC) au Canada. Le forum national organisé en février 2005 a permis aux participants de discuter et d'élaborer des recommandations sur les principes, interventions et pratiques se rapportant au DDC. Les aspects éthiques et juridiques ont été abordés dans les discussions. À la fin du Forum, la majorité des participants ont été favorables à l'implantation de programmes de DDC au Canada. Les participants du Forum ont également convenu qu'il fallait formuler et prôner des valeurs fondamentales pour orienter l'élaboration de programmes et de protocoles basés sur le cadre médical, éthique et juridique établi lors de cette réunion. Même si la possibilité d'un don d'organes et de tissus doit faire partie intégrante des soins de fin de vie, il faut insister sur le fait que le devoir de diligence envers les patients mourants et leurs familles doit demeurer la priorité des équipes soignantes. La complexité et les répercussions profondes du décès sont reconnues et doivent être respectées, de même que les différences personnelles, ethnoculturelles et religieuses face à la mort et au don d'organes. Les décisions d'arrêter le traitement de maintien des fonctions vitales, la prise en charge des derniers moments de la vie et le diagnostic de décès selon des critères cardiocirculatoires doivent être distincts et indépendants des processus de don et transplantation. Ce rapport contient des recommandations destinées aux gestionnaires de program, aux autorités sanitaires régionales et aux instances appelés à élaborer les protocoles de DDC. Les programmes doivent être conçus en fonction des éléments suivants : direction et planification locales, éducation et

  8. 91. Neg. No. F174A, Apr 24, 1936, INTERIORASSEMBLY BUILDING, FINISHED ...

    Library of Congress Historic Buildings Survey, Historic Engineering Record, Historic Landscapes Survey

    91. Neg. No. F-174A, Apr 24, 1936, INTERIOR-ASSEMBLY BUILDING, FINISHED CARS AT THE END OF THE ASSEMBLY LINE - Ford Motor Company Long Beach Assembly Plant, Assembly Building, 700 Henry Ford Avenue, Long Beach, Los Angeles County, CA

  9. Privacy Impact Assessment for the TRIO Programs Annual Performance Report (APR) System

    ERIC Educational Resources Information Center

    US Department of Education, 2008

    2008-01-01

    The TRIO Programs Annual Performance Report (APR) System collects individual student records on individuals served by the following Federal TRIO Programs: Upward Bound (which includes regular Upward Bound (UB), Upward Bound Math-Science (UBMS), and Veterans Upward Bound (VUB)); Student Support Services (SSS); and the Ronald E. McNair Post…

  10. Sulphur flux through the sulphate assimilation pathway is differently controlled by adenosine 5'-phosphosulphate reductase under stress and in transgenic poplar plants overexpressing gamma-ECS, SO, or APR.

    PubMed

    Scheerer, Ursula; Haensch, Robert; Mendel, Ralf R; Kopriva, Stanislav; Rennenberg, Heinz; Herschbach, Cornelia

    2010-01-01

    Sulphate assimilation provides reduced sulphur for the synthesis of cysteine, methionine, and numerous other essential metabolites and secondary compounds. The key step in the pathway is the reduction of activated sulphate, adenosine 5'-phosphosulphate (APS), to sulphite catalysed by APS reductase (APR). In the present study, [(35)S]sulphur flux from external sulphate into glutathione (GSH) and proteins was analysed to check whether APR controls the flux through the sulphate assimilation pathway in poplar roots under some stress conditions and in transgenic poplars. (i) O-Acetylserine (OAS) induced APR activity and the sulphur flux into GSH. (ii) The herbicide Acetochlor induced APR activity and results in a decline of GSH. Thereby the sulphur flux into GSH or protein remained unaffected. (iii) Cd treatment increased APR activity without any changes in sulphur flux but lowered sulphate uptake. Several transgenic poplar plants that were manipulated in sulphur metabolism were also analysed. (i) Transgenic poplar plants that overexpressed the gamma-glutamylcysteine synthetase (gamma-ECS) gene, the enzyme catalysing the key step in GSH formation, showed an increase in sulphur flux into GSH and sulphate uptake when gamma-ECS was targeted to the cytosol, while no changes in sulphur flux were observed when gamma-ECS was targeted to plastids. (ii) No effect on sulphur flux was observed when the sulphite oxidase (SO) gene from Arabidopsis thaliana, which catalyses the back reaction of APR, that is the reaction from sulphite to sulphate, was overexpressed. (iii) When Lemna minor APR was overexpressed in poplar, APR activity increased as expected, but no changes in sulphur flux were observed. For all of these experiments the flux control coefficient for APR was calculated. APR as a controlling step in sulphate assimilation seems obvious under OAS treatment, in gamma-ECS and SO overexpressing poplars. A possible loss of control under certain conditions, that is Cd treatment

  11. Suivi après le traitement du cancer du sein

    PubMed Central

    Sisler, Jeffrey; Chaput, Geneviève; Sussman, Jonathan; Ozokwelu, Emmanuel

    2016-01-01

    Résumé Objectif Offrir aux médecins de famille un résumé des recommandations fondées sur les données probantes pour guider les soins aux survivantes traitées pour le cancer du sein. Qualité des données Une recherche documentaire a été effectuée dans MEDLINE entre 2000 et 2016 à l’aide des mots-clés anglais suivants : breast cancer, survivorship, follow-up care, aftercare, guidelines et survivorship care plans, en se concentrant sur la revue des lignes directrices publiées récemment par les organismes nationaux de cancérologie. Les données étaient de niveaux I à III. Message principal Les soins aux survivantes comportent 4 facettes : surveillance et dépistage, prise en charge des effets à long terme, promotion de la santé et coordination des soins. La surveillance des récidives ne se traduit que par une mammographie annuelle, et le dépistage d’autres cancers doit suivre les lignes directrices basées sur la population. La prise en charge des effets à long terme du cancer et de son traitement aborde des problèmes courants tels la douleur, la fatigue, le lymphœdème, la détresse et les effets indésirables des médicaments, de même que les préoccupations à long terme comme la santé du cœur et des os. La promotion de la santé met en relief les bienfaits de l’activité chez les survivantes du cancer, avec l’accent mis sur l’activité physique. Les soins aux survivantes sont de meilleure qualité lorsque divers services et professionnels de la santé participent aux soins, et le médecin de famille joue un rôle important dans la coordination des soins. Conclusion Les médecins de famille sont de plus en plus souvent les principaux fournisseurs de soins de suivi après le traitement du cancer du sein. Le cancer du sein doit être considéré comme une affection médicale chronique, même chez les femmes en rémission, et les patientes profitent de la même approche que celle utilisée pour les autres affections chroniques en

  12. Simulation of the Universal-Time Diurnal Variation of the Global Electric Circuit Charging Rate

    NASA Technical Reports Server (NTRS)

    Mackerras, David; Darveniza, Mat; Orville, Richard E.; Williams, Earle R.; Goodman, Steven J.

    1999-01-01

    A global lightning model that includes diurnal and annual lightning variation, and total flash density versus latitude for each major land and ocean, has been used as the basis for simulating the global electric circuit charging rate. A particular objective has been to reconcile the difference in amplitude ratios [AR=(max-min)/mean] between global lightning diurnal variation (AR approximately equals 0.8) and the diurnal variation of typical atmospheric potential gradient curves (AR approximately equals 0.35). A constraint on the simulation is that the annual mean charging current should be about 1000 A. The global lightning model shows that negative ground flashes can contribute, at most, about 10-15% of the required current. For the purpose of the charging rate simulation, it was assumed that each ground flash contributes 5 C to the charging process. It was necessary to assume that all electrified clouds contribute to charging by means other than lightning, that the total flash rate can serve as an indirect indicator of the rate of charge transfer, and that oceanic electrified clouds contribute to charging even though they are relatively inefficient in producing lightning. It was also found necessary to add a diurnally invariant charging current component. By trial and error it was found that charging rate diurnal variation curves could be produced with amplitude ratios and general shapes similar to those of the potential gradient diurnal variation curves measured over ocean and arctic regions during voyages of the Carnegie Institute research vessels. The comparisons were made for the northern winter (Nov.-Feb.), the equinox (Mar., Apr., Sept., Oct.), the northern summer (May-Aug.), and the whole year.

  13. Complex regulation of AprA metalloprotease in Pseudomonas fluorescens M114: evidence for the involvement of iron, the ECF sigma factor, PbrA and pseudobactin M114 siderophore.

    PubMed

    Maunsell, Bláithín; Adams, Claire; O'Gara, Fergal

    2006-01-01

    In the soil bacterium Pseudomonas fluorescens M114, extracellular proteolytic activity and fluorescent siderophore (pseudobactin M114) production were previously shown to be co-ordinately negatively regulated in response to environmental iron levels. An iron-starvation extracytoplasmic function sigma factor, PbrA, required for the transcription of siderophore biosynthetic genes, was also implicated in M114 protease regulation. The current study centred on the characterization and genetic regulation of the gene(s) responsible for protease production in M114. A serralysin-type metalloprotease gene, aprA, was identified and found to encode the major, if not only, extracellular protease produced by this strain. The expression of aprA and its protein product were found to be subject to complex regulation. Transcription analysis confirmed that PbrA was required for full aprA transcription under low iron conditions, while the ferric uptake regulator, Fur, was implicated in aprA repression under high iron conditions. Interestingly, the iron regulation of AprA was dependent on culture conditions, with PbrA-independent AprA-mediated proteolytic activity observed on skim milk agar supplemented with yeast extract, when supplied with iron or purified pseudobactin M114. These effects were not observed on skim milk agar without yeast extract. PbrA-independent aprA expression was also observed from a truncated transcriptional fusion when grown in sucrose asparagine tryptone broth supplied with iron or purified pseudobactin M114. Thus, experimental evidence suggested that iron mediated its effects via transcriptional activation by PbrA under low iron conditions, while an as-yet-unidentified sigma factor(s) may be required for the PbrA-independent aprA expression and AprA proteolytic activity induced by siderophore and iron.

  14. Expression, purification, and characterization of the Necator americanus aspartic protease-1 (Na-APR-1 (M74)) antigen, a component of the bivalent human hookworm vaccine.

    PubMed

    Seid, Christopher A; Curti, Elena; Jones, R Mark; Hudspeth, Elissa; Rezende, Wanderson; Pollet, Jeroen; Center, Lori; Versteeg, Leroy; Pritchard, Sonya; Musiychuk, Konstantin; Yusibov, Vidadi; Hotez, Peter J; Bottazzi, Maria Elena

    2015-01-01

    Over 400 million people living in the world's poorest developing nations are infected with hookworms, mostly of the genus Necator americanus. A bivalent human hookworm vaccine composed of the Necator americanus Glutathione S-Transferase-1 (Na-GST-1) and the Necator americanus Aspartic Protease-1 (Na-APR-1 (M74)) is currently under development by the Sabin Vaccine Institute Product Development Partnership (Sabin PDP). Both monovalent vaccines are currently in Phase 1 trials. Both Na-GST-1 and Na-APR-1 antigens are expressed as recombinant proteins. While Na-GST-1 was found to express with high yields in Pichia pastoris, the level of expression of Na-APR-1 in this host was too low to be suitable for a manufacturing process. When the tobacco plant Nicotiana benthamiana was evaluated as an expression system, acceptable levels of solubility, yield, and stability were attained. Observed expression levels of Na-APR-1 (M74) using this system are ∼300 mg/kg. Here we describe the achievements and obstacles encountered during process development as well as characterization and stability of the purified Na-APR-1 (M74) protein and formulated vaccine. The expression, purification and analysis of purified Na-APR-1 (M74) protein obtained from representative 5 kg reproducibility runs performed to qualify the Na-APR-1 (M74) production process is also presented. This process has been successfully transferred to a pilot plant and a 50 kg scale manufacturing campaign under current Good Manufacturing Practice (cGMP) has been performed. The 50 kg run has provided a sufficient amount of protein to support the ongoing hookworm vaccine development program of the Sabin PDP.

  15. Using a Classroom Response System to Improve Multiple-Choice Performance in AP[R] Physics

    ERIC Educational Resources Information Center

    Bertrand, Peggy

    2009-01-01

    Participation in rigorous high school courses such as Advanced Placement (AP[R]) Physics increases the likelihood of college success, especially for students who are traditionally underserved. Tackling difficult multiple-choice exams should be part of any AP program because well-constructed multiple-choice questions, such as those on AP exams and…

  16. Advanced Design Features of APR1400 and Realization in Shin Kori Construction Project

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

    OH, S.J.; Park, K.C.; Kim, H.G.

    2006-07-01

    APR1400 adopted several advanced design features. To ensure their proper operation as a part of ShinKori 3,4 project, both experimental and analytical work are continuing. In this paper, work on the advanced design features related to enhanced safety is examined. APR1400 safety injection system consists of four independent trains which include four safety injection pump and tanks. A passive flow regulating device called fluidic device is installed in the safety injection tanks. Separate effect tests including a full scale fluidic device tests have been conducted. Integral system tests are in progress. Combination of these work with the analytical work usingmore » RELAP5/Mod3 would ensure the proper operation of the new safety injection systems. To mitigate severe accidents, hydrogen mitigation system using PARs and igniters is adopted. Also, active injection system and the streamlined insulation design are adopted to enhance the in-vessel retention capability with the external cooling of RPV strategy. Analytic work with supporting experiments is performed. We are certain that these preparatory work would help the successful adaptation of ADF in ShinKori project. (authors)« less

  17. 23. "GAFFTC 20 APR 60, H65A F106A; ESCAPE SYSTEM RUN ...

    Library of Congress Historic Buildings Survey, Historic Engineering Record, Historic Landscapes Survey

    23. "G-AFFTC 20 APR 60, H-6-5A F-106A; ESCAPE SYSTEM RUN 5A." Testing the ejection system on a Convair sled. - Edwards Air Force Base, South Base Sled Track, Edwards Air Force Base, North of Avenue B, between 100th & 140th Streets East, Lancaster, Los Angeles County, CA

  18. Processing of High Resolution, Multiparametric Radar Data for the Airborne Dual-Frequency Precipitation Radar APR-2

    NASA Technical Reports Server (NTRS)

    Tanelli, Simone; Meagher, Jonathan P.; Durden, Stephen L.; Im, Eastwood

    2004-01-01

    Following the successful Precipitation Radar (PR) of the Tropical Rainfall Measuring Mission, a new airborne, 14/35 GHz rain profiling radar, known as Airborne Precipitation Radar - 2 (APR-2), has been developed as a prototype for an advanced, dual-frequency spaceborne radar for a future spaceborne precipitation measurement mission. . This airborne instrument is capable of making simultaneous measurements of rainfall parameters, including co-pol and cross-pol rain reflectivities and vertical Doppler velocities, at 14 and 35 GHz. furthermore, it also features several advanced technologies for performance improvement, including real-time data processing, low-sidelobe dual-frequency pulse compression, and dual-frequency scanning antenna. Since August 2001, APR-2 has been deployed on the NASA P3 and DC8 aircrafts in four experiments including CAMEX-4 and the Wakasa Bay Experiment. Raw radar data are first processed to obtain reflectivity, LDR (linear depolarization ratio), and Doppler velocity measurements. The dataset is then processed iteratively to accurately estimate the true aircraft navigation parameters and to classify the surface return. These intermediate products are then used to refine reflectivity and LDR calibrations (by analyzing clear air ocean surface returns), and to correct Doppler measurements for the aircraft motion. Finally, the the melting layer of precipitation is detected and its boundaries and characteristics are identifIed at the APR-2 range resolution of 30m. The resulting 3D dataset will be used for validation of other airborne and spaceborne instruments, development of multiparametric rain/snow retrieval algorithms and melting layer characterization and statistics.

  19. Monitoring the impact of an aspartic protease (MpAPr1) on grape proteins and wine properties.

    PubMed

    Theron, Louwrens Wiid; Bely, Marina; Divol, Benoit

    2018-04-23

    The perception of haze in wine is brought about when pathogenesis-related proteins become unstable and aggregate, subsequently resulting in crosslinking until it develops into light-dispersing particles. Elimination of these proteins is usually achieved via bentonite fining, which, although effective, suffers from several drawbacks. The utilization of proteases has been proposed as an ideal alternative. In a previous study, an aspartic protease (MpAPr1) from the yeast Metschnikowia pulcherrima was purified and shown to be partially active against grape proteins in synthetic medium. In this study, the effects of pure MpAPr1 supplemented to Sauvignon Blanc juice on subsequent fermentation were investigated. The juice was incubated for 48 h and thereafter inoculated with Saccharomyces cerevisiae. Results revealed that the enzyme had no observable effects on fermentation performance and retained activity throughout. Protein degradation could be detected and resulted in a significant modification of the wine composition and an increase in the presence of certain volatile compounds, especially those linked to amino acid metabolism.

  20. Récidive après dix ans de tumeur de granulosa de l’ovaire: à propos de deux cas et revue de la littérature

    PubMed Central

    Majdoul, Soufya; Tawfiq, Nezha; Bourhaleb, Zouhour; Naqos, Nora; Taleb, Amina; Bouchbika, Zineb; Benchakroun, Nadia; Jouhadi, Hassan; Sahraoui, Souha; Benider, Abdelatif

    2016-01-01

    Les tumeurs à cellules de la granulosa (TG) de l’ovaire sont des tumeurs rares appartenant au groupe des tumeurs des cordons sexuels et du stroma. Elles représentent 0,6 à 3 % de l’ensemble des tumeurs de l’ovaire et 5 % des tumeurs malignes On distingue deux types: le type juvénile (TGJ) qui se caractérise par son agressivité et le type adulte (TGA) qui est le type le moins agressif et le plus fréquent. Les rechutes de TG de l'ovaire surviennent généralement dans les cinq ans, elles sont rarement sous forme de métastases péritonéales ou locales. Bien que, des options de traitement y compris la chirurgie avec ou sans chimiothérapie et ou radiothérapie ont été rapportés pour le traitement des récidives des TG, il n'y a aucune prise en charge standardisée de récidive de cette maladie. Ici, nous rapportons notre stratégie thérapeutique dans la prise en charge des récidives tardives, après dix ans, de la TG sous forme de carcinose péritonéale pour deux patientes avec une revue de la littérature. PMID:28154722

  1. New Estimates of Inferred Ionic Charge States for Solar Energetic Particle Events with ACE and STEREO

    NASA Astrophysics Data System (ADS)

    Labrador, A. W.; Sollitt, L. S.; Cohen, C. M.; Cummings, A. C.; Leske, R. A.; Mason, G. M.; Mewaldt, R. A.; Stone, E.; von Rosenvinge, T. T.; Wiedenbeck, M. E.

    2012-12-01

    Solar energetic particle (SEP) mean ionic charge states can depend on source temperatures and populations (e.g. seed populations) and conditions during acceleration and transport such as stripping. Multi-spacecraft observations of charge states from widely separated spacecraft may reveal evidence for seed populations that vary with longitude. In this presentation, we report new estimates of inferred high energy ionic charge states using the Sollitt et al. (2008) method that fits SEP energy-dependent decay times for SEP event elements to derive mean charge states. In the method, intensity decay times during SEP events are fitted for each element for various energies, and then the energy dependence of the decay times is fitted for each element. Finally, charge-to-mass ratios relative to that of a calibration element (carbon in this case) are obtained, and when Q(C)=5.9 is assumed for calibration, mean charge states for other elements can be inferred. Previously, ACE/SIS and ACE/ULEIS data were applied to three SEP events (Nov. 6, 1997; Nov. 4, 2001; Apr. 21, 2002) with this method, and last year, we reported new results for the Dec. 6, 2006 SEP event compatible with SAMPEX/MAST results. Additional work continues to generalize and extend the software to use publicly available online data from ACE and the two STEREO spacecraft. Energy ranges are those covered by the instruments on ACE (e.g. reference element C at <.1 MeV/nuc from ULEIS to ~64 MeV/nuc from SIS) and on STEREO (e.g. C at 3.2 - 33 MeV/nuc from LET). Initial candidate SEP events for multi-spacecraft charge state estimates are those of Mar. 8, 2011, Mar. 21, 2011, Jan. 24, 2012, and Mar. 4, 2012. Results from events observed by single spacecraft may also be reported.

  2. Outcomes of patients with abdominoperineal resection (APR) and low anterior resection (LAR) who had very low rectal cancer.

    PubMed

    Yeom, Seung-Seop; Park, In Ja; Jung, Sung Woo; Oh, Se Heon; Lee, Jong Lyul; Yoon, Yong Sik; Kim, Chan Wook; Lim, Seok-Byung; Kim, Nayoung; Yu, Chang Sik; Kim, Jin Cheon

    2017-10-01

    We compared the oncological outcomes of sphincter-saving resection (SSR) and abdominoperineal resection (APR) in 409 consecutive patients with very low rectal cancer (i.e., tumors within 3 cm from the anal verge); 335 (81.9%) patients underwent APR and 74 (18.1%) underwent SSR. The APR group comprised higher proportions of men (67.5% vs 55.4%, P = .049) and advanced-stage patients (P < .001). Preoperative chemoradiotherapy (PCRT) was more frequently administered in the SSR group (83.8% vs 52.8%, P < .001). Overall, the systemic and local recurrence rates were 29.1% and 6.1%, respectively. On stratification according to PCRT and pathologic stage, the mode of surgery did not affect the recurrence type. Moreover, recurrence-free survival (RFS) did not differ according to the mode of surgery in different cancer stages. RFS was associated with ypT and ypN stages in patients who received PCRT, while pN stage, lymphovascular invasion (LVI), and circumferential resection margin (CRM) involvement were risk factors for RFS in those who did not receive PCRT. Notably, SSR was not found to be a risk factor for RFS in either subgroup. Patients who were stratified according to cancer stage and PCRT also showed no differences in RFS according to the mode of surgery. Our results demonstrate that, regardless of PCRT administration, SSR is an effective treatment for very low rectal cancer, while CRM is an important prognostic factor for patients who did not receive PCRT.

  3. L'endométriose pariétale cicatricielle après césarienne: une entité rare

    PubMed Central

    El Fahssi, Mohammed; Lomdo, Massama; Bounaim, Ahmed; Ali, Abdelmounaim Ait; Sair, Khalid

    2016-01-01

    L'endométriose de la paroi est une entité clinique rare, dont la physiopathologie demeure imprécise. Elle survient le plus souvent après une intervention chirurgicale gynécologique ou obstétricale. Nous rapportons le cas d'une patiente présentant une douleur cyclique, au niveau de la cicatrice de césarienne, Avec à l'examen clinique une masse de 5cm localisée au niveau de la fosse iliaque droite. la tomodensitométrie montre une masse de densité tissulaire de 45mm de grand axe. D'où la décision d'excision large de la lésion dont l’étude anatomopathologique confirme le diagnostic d'endométriose pariétale. Les suites postopératoires étaient simples avec un recul de 20 mois sans récidive de la masse ni de la douleur. A travers notre cas, nous insisterons sur les caractéristiques de cette pathologie, ce qui permettra au praticien de comprendre l'intérêt du diagnostic et de la prise en charge précoce de cette affection ainsi que la possibilité de sa prévention au cours de chaque chirurgie gynécologique ou obstétricale. PMID:27642418

  4. A Bayesian inversion for slip distribution of 1 Apr 2007 Mw8.1 Solomon Islands Earthquake

    NASA Astrophysics Data System (ADS)

    Chen, T.; Luo, H.

    2013-12-01

    On 1 Apr 2007 the megathrust Mw8.1 Solomon Islands earthquake occurred in the southeast pacific along the New Britain subduction zone. 102 vertical displacement measurements over the southeastern end of the rupture zone from two field surveys after this event provide a unique constraint for slip distribution inversion. In conventional inversion method (such as bounded variable least squares) the smoothing parameter that determines the relative weight placed on fitting the data versus smoothing the slip distribution is often subjectively selected at the bend of the trade-off curve. Here a fully probabilistic inversion method[Fukuda,2008] is applied to estimate distributed slip and smoothing parameter objectively. The joint posterior probability density function of distributed slip and the smoothing parameter is formulated under a Bayesian framework and sampled with Markov chain Monte Carlo method. We estimate the spatial distribution of dip slip associated with the 1 Apr 2007 Solomon Islands earthquake with this method. Early results show a shallower dip angle than previous study and highly variable dip slip both along-strike and down-dip.

  5. The Experience of Staging Nijinsky's "L'Apres-Midi d'un Faune" in a Higher Education Dance Program

    ERIC Educational Resources Information Center

    Curran, Tina

    2010-01-01

    This study documented the experiences of staging Vaslav Nijinsky's "L'Apres-midi d'un Faune" in a higher education dance program. The ballet was staged from Labanotation. Research questions focused on teaching and learning pedagogy, characterization of the process over time, experiences of the participants and teaching approaches. The project…

  6. Anti-leukaemic effects induced by APR-246 are dependent on induction of oxidative stress and the NFE2L2/HMOX1 axis that can be targeted by PI3K and mTOR inhibitors in acute myeloid leukaemia cells.

    PubMed

    Ali, Dina; Mohammad, Dara K; Mujahed, Huthayfa; Jonson-Videsäter, Kerstin; Nore, Beston; Paul, Christer; Lehmann, Sören

    2016-07-01

    The small molecule APR-246 (PRIMA-1(MET) ) is a novel drug that restores the activity of mutated and unfolded TP53 protein. However, the mechanisms of action and potential off-target effects are not fully understood. Gene expression profiling in TP53 mutant KMB3 acute myeloid leukaemia (AML) cells showed that genes which protected cells from oxidative stress to be the most up-regulated. APR-246 exposure also induced reactive oxygen species (ROS) formation and depleted glutathione in AML cells. The genes most up-regulated by APR-246, confirmed by quantitative real time polymerase chain reaction, were heme oxygenase-1 (HMOX1, also termed HO-1), SLC7A11 and RIT1. Up-regulation of HMOX1, a key regulator of cellular response to ROS, was independent of TP53 mutational status. NFE2L2 (also termed Nrf2), a master regulator of HMOX1 expression, showed transcriptional up-regulation and nuclear translocation by APR-246. Down-regulation of NFE2L2 by siRNA in AML cells significantly increased the antitumoural effects of APR-246. The PI3K inhibitor wortmannin and the mTOR inhibitor rapamycin inhibited APR-246-induced nuclear translocation of NFE2L2 and counteracted the protective cellular responses to APR-246, resulting in synergistic cell killing together with APR-246. In conclusion, ROS induction is important for antileukaemic activities of APR-246 and inhibiting the protective response of the Nrf-2/HMOX1 axis using PI3K inhibitors, enhances the antileukaemic effects. © 2016 John Wiley & Sons Ltd.

  7. 75 FR 44847 - Proposed Collection; Comment Request for Forms 943, 943-PR, 943-A, and 943A-PR

    Federal Register 2010, 2011, 2012, 2013, 2014

    2010-07-29

    ... Para La Declarcion Anual De La Contribucion Federal Del Patrono De Empleados Agricolas, 943-A, Agricultural Employer's Record of Federal Tax Liability, and 943A-PR, Registro De La Obligacion Contributiva...: Employer's Annual Tax Return for Agricultural Employees (Form 943), Planilla Para La Declarcion Anual De La...

  8. 78 FR 47051 - Proposed Collection; Comment Request for Forms 943, 943-PR, 943-A, and 943A-PR

    Federal Register 2010, 2011, 2012, 2013, 2014

    2013-08-02

    ..., 943-PR, Planilla Para La Declarcion Anual De La Contribucion Federal Del Patrono De Empleados Agricolas, 943-A, Agricultural Employer's Record of Federal Tax Liability, and 943A-PR, Registro De La...: Employer's Annual Tax Return for Agricultural Employees (Form 943), Planilla Para La Declarcion Anual De La...

  9. A combination of p53-activating APR-246 and phosphatidylserine-targeting antibody potently inhibits tumor development in hormone-dependent mutant p53-expressing breast cancer xenografts

    PubMed Central

    Liang, Yayun; Mafuvadze, Benford; Besch-Williford, Cynthia; Hyder, Salman M

    2018-01-01

    Background Between 30 and 40% of human breast cancers express a defective tumor suppressor p53 gene. Wild-type p53 tumor suppressor protein promotes cell-cycle arrest and apoptosis and inhibits vascular endothelial growth factor–dependent angiogenesis, whereas mutant p53 protein (mtp53) lacks these functions, resulting in tumor cell survival and metastasis. Restoration of p53 function is therefore a promising drug-targeted strategy for combating mtp53-expressing breast cancer. Methods In this study, we sought to determine whether administration of APR-246, a small-molecule drug that restores p53 function, in combination with 2aG4, an antibody that targets phosphatidylserine residues on tumor blood vessels and disrupts tumor vasculature, effectively inhibits advanced hormone-dependent breast cancer tumor growth. Results APR-246 reduced cell viability in mtp53-expressing BT-474 and T47-D human breast cancer cells in vitro, and significantly induced apoptosis in a dose-dependent manner. However, APR-246 did not reduce cell viability in MCF-7 breast cancer cells, which express wild-type p53. We next examined APR-246’s anti-tumor effects in vivo using BT-474 and T47-D tumor xenografts established in female nude mice. Tumor-bearing mice were treated with APR-246 and/or 2aG4 and tumor volume followed over time. Tumor growth was more effectively suppressed by combination treatment than by either agent alone, and combination therapy completely eradicated some tumors. Immunohistochemistry analysis of tumor tissue sections demonstrated that combination therapy more effectively induced apoptosis and reduced cell proliferation in tumor xenografts than either agent alone. Importantly, combination therapy dramatically reduced the density of blood vessels, which serve as the major route for tumor metastasis, in tumor xenografts compared with either agent alone. Conclusion Based on our findings, we contend that breast tumor growth might effectively be controlled by simultaneous

  10. 78 FR 14155 - Special Conditions: Learjet Inc., Model LJ-200-1A10 Airplane; Use of Automatic Power Reserve (APR...

    Federal Register 2010, 2011, 2012, 2013, 2014

    2013-03-05

    ... Automatic Power Reserve (APR), an Automatic Takeoff Thrust Control System (ATTCS), for Go-Around Performance... airplane will have novel or unusual design features associated with utilizing go-around performance credit...: Federal eRegulations Portal: Go to http://www.regulations.gov/ and follow the online instructions for...

  11. 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

  12. Mimicking acute and chronic stress exposure in naive beef steers alters the acute phase response (APR) associated with vaccination

    USDA-ARS?s Scientific Manuscript database

    This study was designed to determine the effect of an acute versus chronic stress model on the APR associated with vaccination in naïve beef steers. Steers (n=32; 209 +/- 8 kg) were blocked by body weight and assigned to 1 of 3 treatments: 1) Chronic stress (CHR), 0.5 mg/kg body weight dexamethasone...

  13. 42 CFR 405.506 - Charges higher than customary or prevailing charges or lowest charge levels.

    Code of Federal Regulations, 2010 CFR

    2010-10-01

    ... 42 Public Health 2 2010-10-01 2010-10-01 false Charges higher than customary or prevailing charges... prevailing charges or lowest charge levels. A charge which exceeds the customary charge of the physician or other person who rendered the medical or other health service, or the prevailing charge in the locality...

  14. Use case driven approach to develop simulation model for PCS of APR1400 simulator

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

    Dong Wook, Kim; Hong Soo, Kim; Hyeon Tae, Kang

    2006-07-01

    The full-scope simulator is being developed to evaluate specific design feature and to support the iterative design and validation in the Man-Machine Interface System (MMIS) design of Advanced Power Reactor (APR) 1400. The simulator consists of process model, control logic model, and MMI for the APR1400 as well as the Power Control System (PCS). In this paper, a use case driven approach is proposed to develop a simulation model for PCS. In this approach, a system is considered from the point of view of its users. User's view of the system is based on interactions with the system and themore » resultant responses. In use case driven approach, we initially consider the system as a black box and look at its interactions with the users. From these interactions, use cases of the system are identified. Then the system is modeled using these use cases as functions. Lower levels expand the functionalities of each of these use cases. Hence, starting from the topmost level view of the system, we proceeded down to the lowest level (the internal view of the system). The model of the system thus developed is use case driven. This paper will introduce the functionality of the PCS simulation model, including a requirement analysis based on use case and the validation result of development of PCS model. The PCS simulation model using use case will be first used during the full-scope simulator development for nuclear power plant and will be supplied to Shin-Kori 3 and 4 plant. The use case based simulation model development can be useful for the design and implementation of simulation models. (authors)« less

  15. 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.

  16. Appraisal of the Psychiatric Diagnostic Screening Questionnaire in a perinatal cohort: The APrON study.

    PubMed

    Leung, Brenda; Letourneau, Nicole; Bright, Katherine; Giesbrecht, Gerald F; Ntanda, Henry; Gagnon, Lisa

    2017-08-01

    Depression and anxiety are routinely screened as part of perinatal care. However, other Axis 1 disorders and specific anxiety disorders are less likely to be screened or assessed as part of obstetric care. The objective of this study was to determine whether the Psychiatric Diagnostic Screening Questionnaire (PDSQ) is a potentially useful tool to screen for psychiatric conditions in pregnant and postpartum women in a community setting. We compared the prevalence of DSM Axis I disorders obtained on the PDSQ with: (1) the prevalence of these disorders reported in previous studies of pregnant and postpartum women, and (2) scores obtained on the Edinburgh Postpartum Depression Scale (EPDS) and the Symptom Checklist-90-Revised (SCL-90R) anxiety scale. Data were obtained from the Alberta Pregnancy Outcomes and Nutrition (APrON) study. The PDSQ was completed by 1575 women prenatally and 1481 postnatally. The three most prevalent PDSQ conditions were social phobia, somatic disorder, and obsessive-compulsive disorder (OCD). The prevalence of social phobia, alcohol disorder, OCD and psychosis were higher in the APrON cohort compared with statistics in the literature. The proportion of women meeting depression and anxiety cut-offs on the PDSQ were lower than for the EPDS and the SCL-90R. The Cohens Kappa index ( k) indicated poor to fair agreement between the measures in classifying pregnant women as depressed or anxious. The PDSQ subscales may not be appropriate for the pregnant population. Research into instruments more specific to pregnant and postpartum women are needed to determine the prevalence of psychiatric disorders in this population.

  17. 15 CFR 781.4 - U.S. Government requests for information needed to satisfy the requirements of the APR or the Act.

    Code of Federal Regulations, 2010 CFR

    2010-01-01

    ... 15 Commerce and Foreign Trade 2 2010-01-01 2010-01-01 false U.S. Government requests for information needed to satisfy the requirements of the APR or the Act. 781.4 Section 781.4 Commerce and Foreign Trade Regulations Relating to Commerce and Foreign Trade (Continued) BUREAU OF INDUSTRY AND SECURITY...

  18. Synthesis of Key Points from the OSEP Early Childhood Transition FAQ (SPP/APR Indicators C-8, B-11 and B-12)

    ERIC Educational Resources Information Center

    Diefendorf, M.; Henson, J.; Lucas, A.; Whaley, K.

    2010-01-01

    This document is a synthesis of the key points provided in the Office of Special Education Programs (OSEP) Early Childhood Transition FAQs: SPP/APR indicators C-8 and B-12 released on December 1, 2009. It was developed to assist states with the implementation of effective transition policies and practices. The following is included: (1) Transition…

  19. Charge states of ions, and mechanisms of charge ordering transitions

    NASA Astrophysics Data System (ADS)

    Pickett, Warren E.; Quan, Yundi; Pardo, Victor

    2014-07-01

    To gain insight into the mechanism of charge ordering transitions, which conventionally are pictured as a disproportionation of an ion M as 2Mn+→M(n+1)+ + M(n-1)+, we (1) review and reconsider the charge state (or oxidation number) picture itself, (2) introduce new results for the putative charge ordering compound AgNiO2 and the dual charge state insulator AgO, and (3) analyze the cationic occupations of the actual (not formal) charge, and work to reconcile the conundrums that arise. We establish that several of the clearest cases of charge ordering transitions involve no disproportion (no charge transfer between the cations, and hence no charge ordering), and that the experimental data used to support charge ordering can be accounted for within density functional-based calculations that contain no charge transfer between cations. We propose that the charge state picture retains meaning and importance, at least in many cases, if one focuses on Wannier functions rather than atomic orbitals. The challenge of modeling charge ordering transitions with model Hamiltonians isdiscussed.

  20. 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.

  1. Battery charging control methods, electric vehicle charging methods, battery charging apparatuses and rechargeable battery systems

    DOEpatents

    Tuffner, Francis K [Richland, WA; Kintner-Meyer, Michael C. W. [Richland, WA; Hammerstrom, Donald J [West Richland, WA; Pratt, Richard M [Richland, WA

    2012-05-22

    Battery charging control methods, electric vehicle charging methods, battery charging apparatuses and rechargeable battery systems. According to one aspect, a battery charging control method includes accessing information regarding a presence of at least one of a surplus and a deficiency of electrical energy upon an electrical power distribution system at a plurality of different moments in time, and using the information, controlling an adjustment of an amount of the electrical energy provided from the electrical power distribution system to a rechargeable battery to charge the rechargeable battery.

  2. Implementation of a Clinical Documentation Improvement Curriculum Improves Quality Metrics and Hospital Charges in an Academic Surgery Department.

    PubMed

    Reyes, Cynthia; Greenbaum, Alissa; Porto, Catherine; Russell, John C

    2017-03-01

    Accurate clinical documentation (CD) is necessary for many aspects of modern health care, including excellent communication, quality metrics reporting, and legal documentation. New requirements have mandated adoption of ICD-10-CM coding systems, adding another layer of complexity to CD. A clinical documentation improvement (CDI) and ICD-10 training program was created for health care providers in our academic surgery department. We aimed to assess the impact of our CDI curriculum by comparing quality metrics, coding, and reimbursement before and after implementation of our CDI program. A CDI/ICD-10 training curriculum was instituted in September 2014 for all members of our university surgery department. The curriculum consisted of didactic lectures, 1-on-1 provider training, case reviews, e-learning modules, and CD queries from nurse CDI staff and hospital coders. Outcomes parameters included monthly documentation completion rates, severity of illness (SOI), risk of mortality (ROM), case-mix index (CMI), all-payer refined diagnosis-related groups (APR-DRG), and Surgical Care Improvement Program (SCIP) metrics. Financial gain from responses to CDI queries was determined retrospectively. Surgery department delinquent documentation decreased by 85% after CDI implementation. Compliance with SCIP measures improved from 85% to 97%. Significant increases in surgical SOI, ROM, CMI, and APR-DRG (all p < 0.01) were found after CDI/ICD-10 training implementation. Provider responses to CDI queries resulted in an estimated $4,672,786 increase in charges. Clinical documentation improvement/ICD-10 training in an academic surgery department is an effective method to improve documentation rates, increase the hospital estimated reimbursement based on more accurate CD, and provide better compliance with surgical quality measures. Copyright © 2016 American College of Surgeons. All rights reserved.

  3. Charge migration and charge transfer in molecular systems

    PubMed Central

    Wörner, Hans Jakob; Arrell, Christopher A.; Banerji, Natalie; Cannizzo, Andrea; Chergui, Majed; Das, Akshaya K.; Hamm, Peter; Keller, Ursula; Kraus, Peter M.; Liberatore, Elisa; Lopez-Tarifa, Pablo; Lucchini, Matteo; Meuwly, Markus; Milne, Chris; Moser, Jacques-E.; Rothlisberger, Ursula; Smolentsev, Grigory; Teuscher, Joël; van Bokhoven, Jeroen A.; Wenger, Oliver

    2017-01-01

    The transfer of charge at the molecular level plays a fundamental role in many areas of chemistry, physics, biology and materials science. Today, more than 60 years after the seminal work of R. A. Marcus, charge transfer is still a very active field of research. An important recent impetus comes from the ability to resolve ever faster temporal events, down to the attosecond time scale. Such a high temporal resolution now offers the possibility to unravel the most elementary quantum dynamics of both electrons and nuclei that participate in the complex process of charge transfer. This review covers recent research that addresses the following questions. Can we reconstruct the migration of charge across a molecule on the atomic length and electronic time scales? Can we use strong laser fields to control charge migration? Can we temporally resolve and understand intramolecular charge transfer in dissociative ionization of small molecules, in transition-metal complexes and in conjugated polymers? Can we tailor molecular systems towards specific charge-transfer processes? What are the time scales of the elementary steps of charge transfer in liquids and nanoparticles? Important new insights into each of these topics, obtained from state-of-the-art ultrafast spectroscopy and/or theoretical methods, are summarized in this review. PMID:29333473

  4. Variability of nursing care by APR-DRG and by severity of illness in a sample of nine Belgian hospitals.

    PubMed

    Pirson, Magali; Delo, Caroline; Di Pierdomenico, Lionel; Laport, Nancy; Biloque, Veronique; Leclercq, Pol

    2013-10-10

    As soon as Diagnosis related Groups (DRG) were introduced in many hospital financing systems, most nursing research revealed that DRG were not very homogeneous with regard to nursing care. However, few studies are based on All Patient refined Diagnosis related Groups (APR-DRGs) and few of them use recent data. Objectives of this study are: (1) to evaluate if nursing activity is homogeneous by APR-DRG and by severity of illness (SOI) (2) to evaluate the outlier's rate associated with the nursing activity and (3) to compare nursing cost homogeneity per DRG and SOI. Study done in 9 Belgian hospitals on a selection of APR-DRG with more than 30 patients (7 638 inpatient stays). The evaluation of the homogeneity is based on coefficients of variation (CV). The 75th percentile + 1.5 × inter-quartile range was used to select high outliers. 25th percentile -1.5 × inter-quartile range was used to select low outliers. Nursing costs per ward were distributed on inpatient stays of each ward following two techniques (the LOS vs. the number of nursing care minutes per stay). The homogeneity of LOS by DRG and by SOI is relatively good (CV: 0.56). The homogeneity of the nursing activity by DRG is less good (CVs between 0.36 and 1.54) and is influenced by nursing activity outliers (high outliers' rate: 5.19%, low outliers' rate: 0.14%). The outlier's rate varies according to the studied variable. The high outliers' rate is higher for nursing activity than for LOS. The homogeneity of nursing costs is higher when costs are based on the LOS of patients than when based on minutes of nursing care (CVs between 0.26 and 1.46 for nursing costs based on LOS and between 0.49 and 2.04 for nursing costs based on minutes of nursing care). It is essential that the calculation of nursing cost by stay and by DRG for hospital financing purposes was based on nursing activity data, that more reflect resources used in wards, and not on LOS data. The only way to obtain this information is

  5. Variability of nursing care by APR-DRG and by severity of illness in a sample of nine Belgian hospitals

    PubMed Central

    2013-01-01

    Background As soon as Diagnosis related Groups (DRG) were introduced in many hospital financing systems, most nursing research revealed that DRG were not very homogeneous with regard to nursing care. However, few studies are based on All Patient refined Diagnosis related Groups (APR-DRGs) and few of them use recent data. Objectives of this study are: (1) to evaluate if nursing activity is homogeneous by APR-DRG and by severity of illness (SOI) (2) to evaluate the outlier’s rate associated with the nursing activity and (3) to compare nursing cost homogeneity per DRG and SOI. Methods Study done in 9 Belgian hospitals on a selection of APR-DRG with more than 30 patients (7 638 inpatient stays). The evaluation of the homogeneity is based on coefficients of variation (CV). The 75th percentile + 1.5 × inter-quartile range was used to select high outliers. 25th percentile −1.5 × inter-quartile range was used to select low outliers. Nursing costs per ward were distributed on inpatient stays of each ward following two techniques (the LOS vs. the number of nursing care minutes per stay). Results The homogeneity of LOS by DRG and by SOI is relatively good (CV: 0.56). The homogeneity of the nursing activity by DRG is less good (CVs between 0.36 and 1.54) and is influenced by nursing activity outliers (high outliers’ rate: 5.19%, low outliers’ rate: 0.14%). The outlier’s rate varies according to the studied variable. The high outliers’ rate is higher for nursing activity than for LOS. The homogeneity of nursing costs is higher when costs are based on the LOS of patients than when based on minutes of nursing care (CVs between 0.26 and 1.46 for nursing costs based on LOS and between 0.49 and 2.04 for nursing costs based on minutes of nursing care). Conclusions It is essential that the calculation of nursing cost by stay and by DRG for hospital financing purposes was based on nursing activity data, that more reflect resources used in wards, and not on LOS

  6. Space and surface charge behavior analysis of charge-eliminated polymer films

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

    Oda, Tetsuji; Takashima, Kazunori; Ichiyama, Shinichiro

    1995-12-31

    Charge behavior of corona-charged or charge eliminated polymer films being dipped in the city water were studied. They were polytetrafluoroethylene (PTFE teflon{trademark}), polypropylene (PP), low density or high density polyethylene (LDPE or HDPE) thin films which are as grown (native) or plasma-processed. The plasma processing at low pressure was tested as antistatic processing. Charge elimination was done by being dipped in alcohol or city water. TSDC analysis and surface charge profile measurement were done for both charged and charge eliminated polymer films. Surface charge density of plasma processed polymer films just after corona charging is roughly the same as thatmore » of an original film. There is little difference between surface charge density profile of a native film and that of a plasma processed film. A large hetero current peak of TSDC was observed at room temperature for a processed film. It was found that the hetero peak disappears after charge elimination process. A pressure pulse wave method by using a pulse-driven piezoelectric PVDF polymer film as a piezoelectric actuator was newly developed to observe real space charge distribution. A little difference of internal space charge distribution between the plasma processed film and the native one after corona charging is found.« less

  7. Response Time Analysis and Test of Protection System Instrument Channels for APR1400 and OPR1000

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

    Lee, Chang Jae; Han, Seung; Yun, Jae Hee

    2015-07-01

    Safety limits are required to maintain the integrity of physical barriers designed to prevent the uncontrolled release of radioactive materials in nuclear power plants. The safety analysis establishes two critical constraints that include an analytical limit in terms of a measured or calculated variable, and a specific time after the analytical limit is reached to begin protective action. Keeping with the nuclear regulations and industry standards, satisfying these two requirements will ensure that the safety limit will not be exceeded during the design basis event, either an anticipated operational occurrence or a postulated accident. Various studies on the setpoint determinationmore » methodology for the safety-related instrumentation have been actively performed to ensure that the requirement of the analytical limit is satisfied. In particular, the protection setpoint methodology for the advanced power reactor 1400 (APP1400) and the optimized power reactor 1000 (OPR1000) has been recently developed to cover both the design basis event and the beyond design basis event. The developed setpoint methodology has also been quantitatively validated using specific computer programs and setpoint calculations. However, the safety of nuclear power plants cannot be fully guaranteed by satisfying the requirement of the analytical limit. In spite of the response time verification requirements of nuclear regulations and industry standards, it is hard to find the studies on the systematically integrated methodology regarding the response time evaluation. In cases of APR1400 and OPR1000, the response time analysis for the plant protection system is partially included in the setpoint calculation and the response time test is separately performed via the specific plant procedure. The test technique has a drawback which is the difficulty to demonstrate completeness of timing test. The analysis technique has also a demerit of resulting in extreme times that not actually possible

  8. Electron-beam-charged dielectrics: Internal charge distribution

    NASA Technical Reports Server (NTRS)

    Beers, B. L.; Pine, V. W.

    1981-01-01

    Theoretical calculations of an electron transport model of the charging of dielectrics due to electron bombardment are compared to measurements of internal charge distributions. The emphasis is on the distribution of Teflon. The position of the charge centroid as a function of time is not monotonic. It first moves deeper into the material and then moves back near to the surface. In most time regimes of interest, the charge distribution is not unimodal, but instead has two peaks. The location of the centroid near saturation is a function of the incident current density. While the qualitative comparison of theory and experiment are reasonable, quantitative comparison shows discrepancies of as much as a factor of two.

  9. Effects of Discrete Charge Clustering in Simulations of Charged Interfaces.

    PubMed

    Grime, John M A; Khan, Malek O

    2010-10-12

    A system of counterions between charged surfaces is investigated, with the surfaces represented by uniform charged planes and three different arrangements of discrete surface charges - an equispaced grid and two different clustered arrangements. The behaviors of a series of systems with identical net surface charge density are examined, with particular emphasis placed on the long ranged corrections via the method of "charged slabs" and the effects of the simulation cell size. Marked differences are observed in counterion distributions and the osmotic pressure dependent on the particular representation of the charged surfaces; the uniformly charged surfaces and equispaced grids of discrete charge behave in a broadly similar manner, but the clustered systems display a pronounced decrease in osmotic pressure as the simulation size is increased. The influence of the long ranged correction is shown to be minimal for all but the very smallest of system sizes.

  10. Analysis and improvements of Adaptive Particle Refinement (APR) through CPU time, accuracy and robustness considerations

    NASA Astrophysics Data System (ADS)

    Chiron, L.; Oger, G.; de Leffe, M.; Le Touzé, D.

    2018-02-01

    While smoothed-particle hydrodynamics (SPH) simulations are usually performed using uniform particle distributions, local particle refinement techniques have been developed to concentrate fine spatial resolutions in identified areas of interest. Although the formalism of this method is relatively easy to implement, its robustness at coarse/fine interfaces can be problematic. Analysis performed in [16] shows that the radius of refined particles should be greater than half the radius of unrefined particles to ensure robustness. In this article, the basics of an Adaptive Particle Refinement (APR) technique, inspired by AMR in mesh-based methods, are presented. This approach ensures robustness with alleviated constraints. Simulations applying the new formalism proposed achieve accuracy comparable to fully refined spatial resolutions, together with robustness, low CPU times and maintained parallel efficiency.

  11. Policy Options for Sharing Activities between the Department of Veterans Affairs and the Department of Defense

    DTIC Science & Technology

    2007-06-14

    evidence - based medicine (Guideline [medicall, 2006). Those who adopt and execute the guidelines and operate within their requirements are said to...the populations of both Departments continues to rise. Similarly, as more evidence - based medicine is transformed into clinical practice guidelines and

  12. 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.

  13. 29 CFR 1626.8 - Contents of charge; amendment of charge.

    Code of Federal Regulations, 2013 CFR

    2013-07-01

    ... 29 Labor 4 2013-07-01 2013-07-01 false Contents of charge; amendment of charge. 1626.8 Section 1626.8 Labor Regulations Relating to Labor (Continued) EQUAL EMPLOYMENT OPPORTUNITY COMMISSION PROCEDURES-AGE DISCRIMINATION IN EMPLOYMENT ACT § 1626.8 Contents of charge; amendment of charge. (a) In...

  14. 29 CFR 1626.8 - Contents of charge; amendment of charge.

    Code of Federal Regulations, 2012 CFR

    2012-07-01

    ... 29 Labor 4 2012-07-01 2012-07-01 false Contents of charge; amendment of charge. 1626.8 Section 1626.8 Labor Regulations Relating to Labor (Continued) EQUAL EMPLOYMENT OPPORTUNITY COMMISSION PROCEDURES-AGE DISCRIMINATION IN EMPLOYMENT ACT § 1626.8 Contents of charge; amendment of charge. (a) In...

  15. 29 CFR 1626.8 - Contents of charge; amendment of charge.

    Code of Federal Regulations, 2011 CFR

    2011-07-01

    ... 29 Labor 4 2011-07-01 2011-07-01 false Contents of charge; amendment of charge. 1626.8 Section 1626.8 Labor Regulations Relating to Labor (Continued) EQUAL EMPLOYMENT OPPORTUNITY COMMISSION PROCEDURES-AGE DISCRIMINATION IN EMPLOYMENT ACT § 1626.8 Contents of charge; amendment of charge. (a) In...

  16. 29 CFR 1626.8 - Contents of charge; amendment of charge.

    Code of Federal Regulations, 2014 CFR

    2014-07-01

    ... 29 Labor 4 2014-07-01 2014-07-01 false Contents of charge; amendment of charge. 1626.8 Section 1626.8 Labor Regulations Relating to Labor (Continued) EQUAL EMPLOYMENT OPPORTUNITY COMMISSION PROCEDURES-AGE DISCRIMINATION IN EMPLOYMENT ACT § 1626.8 Contents of charge; amendment of charge. (a) In...

  17. 29 CFR 1626.8 - Contents of charge; amendment of charge.

    Code of Federal Regulations, 2010 CFR

    2010-07-01

    ... 29 Labor 4 2010-07-01 2010-07-01 false Contents of charge; amendment of charge. 1626.8 Section 1626.8 Labor Regulations Relating to Labor (Continued) EQUAL EMPLOYMENT OPPORTUNITY COMMISSION PROCEDURES-AGE DISCRIMINATION IN EMPLOYMENT ACT § 1626.8 Contents of charge; amendment of charge. (a) In...

  18. Understanding the Linkage between Charging Network Coverage and Charging Opportunity

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

    Liu, Changzheng; Lin, Zhenhong; Kontou, Eleftheria

    2016-01-01

    Using GPS-based travel survey data, this paper estimates the relationship between public charging network coverage and charging opportunity, defined as the probability of being able to access public charging for a driver at one of his/her stops or at one travel day. Understanding this relationship is of important interests to the electric vehicle industry and government in determining appropriate charging infrastructure deployment level and estimating the impact of public charging on market adoption of electric vehicles. The analysis finds that drivers trip destinations concentrate on a few popular places. If top 1% of most popular places are installed with publicmore » chargers, on average, drivers will be able to access public charging at 20% of all their stops and 1/3 of their travel days; If 20% of most popular places are installed with public chargers, drivers will be able to access public charging at 89% of all their stops and 94% of their travel days. These findings are encouraging, implying charging network can be efficiently designed by concentrating at a few popular places while still providing a high level of charging opportunity.« less

  19. Charging machine

    DOEpatents

    Medlin, John B.

    1976-05-25

    A charging machine for loading fuel slugs into the process tubes of a nuclear reactor includes a tubular housing connected to the process tube, a charging trough connected to the other end of the tubular housing, a device for loading the charging trough with a group of fuel slugs, means for equalizing the coolant pressure in the charging trough with the pressure in the process tubes, means for pushing the group of fuel slugs into the process tube and a latch and a seal engaging the last object in the group of fuel slugs to prevent the fuel slugs from being ejected from the process tube when the pusher is removed and to prevent pressure liquid from entering the charging machine.

  20. Point Charges Optimally Placed to Represent the Multipole Expansion of Charge Distributions

    PubMed Central

    Onufriev, Alexey V.

    2013-01-01

    We propose an approach for approximating electrostatic charge distributions with a small number of point charges to optimally represent the original charge distribution. By construction, the proposed optimal point charge approximation (OPCA) retains many of the useful properties of point multipole expansion, including the same far-field asymptotic behavior of the approximate potential. A general framework for numerically computing OPCA, for any given number of approximating charges, is described. We then derive a 2-charge practical point charge approximation, PPCA, which approximates the 2-charge OPCA via closed form analytical expressions, and test the PPCA on a set of charge distributions relevant to biomolecular modeling. We measure the accuracy of the new approximations as the RMS error in the electrostatic potential relative to that produced by the original charge distribution, at a distance the extent of the charge distribution–the mid-field. The error for the 2-charge PPCA is found to be on average 23% smaller than that of optimally placed point dipole approximation, and comparable to that of the point quadrupole approximation. The standard deviation in RMS error for the 2-charge PPCA is 53% lower than that of the optimal point dipole approximation, and comparable to that of the point quadrupole approximation. We also calculate the 3-charge OPCA for representing the gas phase quantum mechanical charge distribution of a water molecule. The electrostatic potential calculated by the 3-charge OPCA for water, in the mid-field (2.8 Å from the oxygen atom), is on average 33.3% more accurate than the potential due to the point multipole expansion up to the octupole order. Compared to a 3 point charge approximation in which the charges are placed on the atom centers, the 3-charge OPCA is seven times more accurate, by RMS error. The maximum error at the oxygen-Na distance (2.23 Å ) is half that of the point multipole expansion up to the octupole order. PMID

  1. Restoration of Verrallina to Generic Rank in Tribe Aedini (Diptera: Culicidae) and Descriptions of the Genus and Three Included Subgenera

    DTIC Science & Technology

    1999-01-01

    R. 1905. Les moustiques histoire naturelle et medicale. Paris, France, 673 pp, (in French). Bohart, R. M. 1945. A synopsis of the Philippine...L. Brug. 1937. Nederlandsch-Indische culicinen. Geneesk. Tijdschr. Ned.-Ind. 77:1-105. Borel, E. 1930. Les moustiques de la Cochinchine et du Sud

  2. Ion association at discretely-charged dielectric interfaces: Giant charge inversion

    NASA Astrophysics Data System (ADS)

    Wang, Zhi-Yong; Wu, Jianzhong

    2017-07-01

    Giant charge reversal has been identified for the first time by Monte Carlo simulation for a discretely charged surface in contact with a trivalent electrolyte solution. It takes place regardless of the surface charge density under study and the monovalent salt. In stark contrast to earlier predictions based on the 2-dimensional Wigner crystal model to describe strong correlation of counterions at the macroion surface, we find that giant charge reversal reflects an intricate interplay of ionic volume effects, electrostatic correlations, surface charge heterogeneity, and the dielectric response of the confined fluids. While the novel phenomenon is yet to be confirmed with experiment, the simulation results appear in excellent agreement with a wide range of existing observations in the subregime of charge inversion. Our findings may have far-reaching implications to understanding complex electrochemical phenomena entailing ionic fluids under dielectric confinements.

  3. Coulombic charge ice

    NASA Astrophysics Data System (ADS)

    McClarty, P. A.; O'Brien, A.; Pollmann, F.

    2014-05-01

    We consider a classical model of charges ±q on a pyrochlore lattice in the presence of long-range Coulomb interactions. This model first appeared in the early literature on charge 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 charge-charge 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 charge liquid within a temperature window in which the physics is well described as a liquid of screened charged defects. The structure factor in this phase, which has smeared pinch points at the reciprocal lattice points, may be used to detect charge ice experimentally. In addition, the model exhibits fractionally charged 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 charge ice model and the dipolar spin ice model on an equal footing by mapping both to a constrained charge 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 charge ice ground states as coming from a dipolar model on a diamond lattice. We study the properties of charge 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 charge ice in the correlated liquid phase.

  4. Modeling the Electric Potential and Surface Charge Density near Charged Thunderclouds

    ERIC Educational Resources Information Center

    Neel, Matthew Stephen

    2018-01-01

    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…

  5. 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.

  6. Validation of the All Patient Refined Diagnosis Related Group (APR-DRG) Risk of Mortality and Severity of Illness Modifiers as a Measure of Perioperative Risk.

    PubMed

    McCormick, Patrick J; Lin, Hung-Mo; Deiner, Stacie G; Levin, Matthew A

    2018-03-22

    The All Patient Refined Diagnosis Related Group (APR-DRG) is an inpatient visit classification system that assigns a diagnostic related group, a Risk of Mortality (ROM) subclass and a Severity of Illness (SOI) subclass. While extensively used for cost adjustment, no study has compared the APR-DRG subclass modifiers to the popular Charlson Comorbidity Index as a measure of comorbidity severity in models for perioperative in-hospital mortality. In this study we attempt to validate the use of these subclasses to predict mortality in a cohort of surgical patients. We analyzed all adult (age over 18 years) inpatient non-cardiac surgery at our institution between December 2005 and July 2013. After exclusions, we split the cohort into training and validation sets. We created prediction models of inpatient mortality using the Charlson Comorbidity Index, ROM only, SOI only, and ROM with SOI. Models were compared by receiver-operator characteristic (ROC) curve, area under the ROC curve (AUC), and Brier score. After exclusions, we analyzed 63,681 patient-visits. Overall in-hospital mortality was 1.3%. The median number of ICD-9-CM diagnosis codes was 6 (Q1-Q3 4-10). The median Charlson Comorbidity Index was 0 (Q1-Q3 0-2). When the model was applied to the validation set, the c-statistic for Charlson was 0.865, c-statistic for ROM was 0.975, and for ROM and SOI combined the c-statistic was 0.977. The scaled Brier score for Charlson was 0.044, Brier for ROM only was 0.230, and Brier for ROM and SOI was 0.257. The APR-DRG ROM or SOI subclasses are better predictors than the Charlson Comorbidity Index of in-hospital mortality among surgical patients.

  7. Charge collection kinetics on ferroelectric polymer surface using charge gradient microscopy

    DOE PAGES

    Choi, Yoon-Young; Tong, Sheng; Ducharme, Stephen P.; ...

    2016-05-03

    Here, a charge gradient microscopy (CGM) probe was used to collect surface screening charges on poly(vinylidene fluoride-trifluoroethylene) [P(VDF-TrFE)] thin films. These charges are naturally formed on unscreened ferroelectric domains in ambient condition. The CGM data were used to map the local electric current originating from the collected surface charges on the poled ferroelectric domains in the P(VDF-TrFE) thin films. Both the direction and amount of the collected current were controlled by changing the polarity and area of the poled domains. The endurance of charge collection by rubbing the CGM tip on the polymer film was limited to 20 scan cycles,more » after which the current reduced to almost zero. This degradation was attributed to the increase of the chemical bonding strength between the external screening charges and the polarization charges. Once this degradation mechanism is mitigated, the CGM technique can be applied to efficient energy harvesting devices using polymer ferroelectrics.« less

  8. Photoinduced ultrafast charge-order melting: Charge-order inversion and nonthermal effects

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

    van Veenendaal, Michel

    2016-09-01

    The effect of photoexcitation is studied for a system with checkerboard charge order induced by displacements of ligands around a metal site. The motion of the ligands is treated classically and the electronic charges are simplified to two-level molecular bond charges. The calculations are done for a checkerboard charge-ordered system with about 100 000 ligand oscillators coupled to a fixed-temperature bath. The initial photoexcitation is followed by a rapid decrease in the charge-order parameter within 50–100 femtoseconds while leaving the correlation length almost unchanged. Depending on the fluence, a complete melting of the charge order occurs in less than amore » picosecond. While for low fluences, the system returns to its original state, for full melting, it recovers to its broken-symmetry state leading to an inversion of the charge order. For small long-range interactions, recovery can be slow due to domain formation.« less

  9. Photoinduced ultrafast charge-order melting: Charge-order inversion and nonthermal effects

    DOE PAGES

    van Veenendaal, Michel

    2016-09-01

    The effect of photoexcitation is studied for a system with checkerboard charge order induced by displacements of ligands around a metal site. The motion of the ligands is treated classically and the electronic charges are simplified to two-level molecular bond charges. The calculations are done for a checkerboard charge-ordered system with about 100 000 ligand oscillators coupled to a fixed-temperature bath. The initial photoexcitation is followed by a rapid decrease in the charge-order parameter within 50–100 femtoseconds while leaving the correlation length almost unchanged. Depending on the fluence, a complete melting of the charge order occurs in less than amore » picosecond. While for low fluences, the system returns to its original state, for full melting, it recovers to its broken-symmetry state leading to an inversion of the charge order. Finally, for small long-range interactions, recovery can be slow due to domain formation.« less

  10. Fuel assembly design for APR1400 with low CBC

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

    Hah, Chang Joo, E-mail: changhah@kings.ac.kr

    2015-04-29

    APR 1400 is a PWR (Pressurized Water Reactor) with rated power of 3983 MWth and 241 assemblies. Recently, demand for extremely longer cycle up to 24 months is increasing with challenge of higher critical boron concentration (CBC). In this paper, assembly design method of selecting Gd-rods is introduced to reduce CBC. The purpose of the method is to lower the critical boron concentration of the preliminary core loading pattern (PLP), and consequently to achieve more negative or less positive moderator temperature coefficient (MTC). In this method, both the ratio of the number of low-Gd rod to the number of high-Gdmore » rod (r) and assembly average Gd wt% (w) are the decision variables. The target function is the amount of soluble boron concentration reduction, which can be converted to Δk{sub TARGET}. A set of new designed fuel assembly satisfies an objective function, min [f=∑{sub i}(Δk{sub FA}−Δk{sub i})], and enables a final loading pattern to reach a target CBC. The constraints required to determine a set of Δk are physically realizable pair, (r,w), and the sum of Δk of new designed assemblies as close to Δk{sub TARGET} as possible. New Gd-bearing assemblies selected based on valid pairs of (r,w) are replaced with existing assemblies in a PLP. This design methodology is applied to Shin-Kori Unit 3 Cycle 1 used as a reference model. CASMO-3/MASTER code is used for depletion calculation. CASMO-3/MASTER calculations with new designed assemblies produce lower CBC than the expected CBC, proving that the proposed method works successful.« less

  11. MOSFET Electric-Charge Sensor

    NASA Technical Reports Server (NTRS)

    Robinson, Paul A., Jr.

    1988-01-01

    Charged-particle probe compact and consumes little power. Proposed modification enables metal oxide/semiconductor field-effect transistor (MOSFET) to act as detector of static electric charges or energetic charged particles. Thickened gate insulation acts as control structure. During measurements metal gate allowed to "float" to potential of charge accumulated in insulation. Stack of modified MOSFET'S constitutes detector of energetic charged particles. Each gate "floats" to potential induced by charged-particle beam penetrating its layer.

  12. Rational design of viscosity reducing mutants of a monoclonal antibody: Hydrophobic versus electrostatic inter-molecular interactions

    PubMed Central

    Nichols, Pilarin; Li, Li; Kumar, Sandeep; Buck, Patrick M; Singh, Satish K; Goswami, Sumit; Balthazor, Bryan; Conley, Tami R; Sek, David; Allen, Martin J

    2015-01-01

    High viscosity of monoclonal antibody formulations at concentrations ≥100 mg/mL can impede their development as products suitable for subcutaneous delivery. The effects of hydrophobic and electrostatic intermolecular interactions on the solution behavior of MAB 1, which becomes unacceptably viscous at high concentrations, was studied by testing 5 single point mutants. The mutations were designed to reduce viscosity by disrupting either an aggregation prone region (APR), which also participates in 2 hydrophobic surface patches, or a negatively charged surface patch in the variable region. The disruption of an APR that lies at the interface of light and heavy chain variable domains, VH and VL, via L45K mutation destabilized MAB 1 and abolished antigen binding. However, mutation at the preceding residue (V44K), which also lies in the same APR, increased apparent solubility and reduced viscosity of MAB 1 without sacrificing antigen binding or thermal stability. Neutralizing the negatively charged surface patch (E59Y) also increased apparent solubility and reduced viscosity of MAB 1, but charge reversal at the same position (E59K/R) caused destabilization, decreased solubility and led to difficulties in sample manipulation that precluded their viscosity measurements at high concentrations. Both V44K and E59Y mutations showed similar increase in apparent solubility. However, the viscosity profile of E59Y was considerably better than that of the V44K, providing evidence that inter-molecular interactions in MAB 1 are electrostatically driven. In conclusion, neutralizing negatively charged surface patches may be more beneficial toward reducing viscosity of highly concentrated antibody solutions than charge reversal or aggregation prone motif disruption. PMID:25559441

  13. Rational design of viscosity reducing mutants of a monoclonal antibody: hydrophobic versus electrostatic inter-molecular interactions.

    PubMed

    Nichols, Pilarin; Li, Li; Kumar, Sandeep; Buck, Patrick M; Singh, Satish K; Goswami, Sumit; Balthazor, Bryan; Conley, Tami R; Sek, David; Allen, Martin J

    2015-01-01

    High viscosity of monoclonal antibody formulations at concentrations ≥100 mg/mL can impede their development as products suitable for subcutaneous delivery. The effects of hydrophobic and electrostatic intermolecular interactions on the solution behavior of MAB 1, which becomes unacceptably viscous at high concentrations, was studied by testing 5 single point mutants. The mutations were designed to reduce viscosity by disrupting either an aggregation prone region (APR), which also participates in 2 hydrophobic surface patches, or a negatively charged surface patch in the variable region. The disruption of an APR that lies at the interface of light and heavy chain variable domains, VH and VL, via L45K mutation destabilized MAB 1 and abolished antigen binding. However, mutation at the preceding residue (V44K), which also lies in the same APR, increased apparent solubility and reduced viscosity of MAB 1 without sacrificing antigen binding or thermal stability. Neutralizing the negatively charged surface patch (E59Y) also increased apparent solubility and reduced viscosity of MAB 1, but charge reversal at the same position (E59K/R) caused destabilization, decreased solubility and led to difficulties in sample manipulation that precluded their viscosity measurements at high concentrations. Both V44K and E59Y mutations showed similar increase in apparent solubility. However, the viscosity profile of E59Y was considerably better than that of the V44K, providing evidence that inter-molecular interactions in MAB 1 are electrostatically driven. In conclusion, neutralizing negatively charged surface patches may be more beneficial toward reducing viscosity of highly concentrated antibody solutions than charge reversal or aggregation prone motif disruption.

  14. 48 CFR 52.227-6 - Royalty Information.

    Code of Federal Regulations, 2011 CFR

    2011-10-01

    ... an identification of applicable claims of specific patents. (End of provision) Alternate I (APR 1984... construction or special assembly that contain costs or charges for royalties totaling more than $250, the...

  15. 48 CFR 52.227-6 - Royalty Information.

    Code of Federal Regulations, 2010 CFR

    2010-10-01

    ... an identification of applicable claims of specific patents. (End of provision) Alternate I (APR 1984... construction or special assembly that contain costs or charges for royalties totaling more than $250, the...

  16. Linear shaped charge

    DOEpatents

    Peterson, David; Stofleth, Jerome H.; Saul, Venner W.

    2017-07-11

    Linear shaped charges are described herein. In a general embodiment, the linear shaped charge has an explosive with an elongated arrowhead-shaped profile. The linear shaped charge also has and an elongated v-shaped liner that is inset into a recess of the explosive. Another linear shaped charge includes an explosive that is shaped as a star-shaped prism. Liners are inset into crevices of the explosive, where the explosive acts as a tamper.

  17. Internal Charging

    NASA Technical Reports Server (NTRS)

    Minow, Joseph I.

    2014-01-01

    (1) High energy (>100keV) electrons penetrate spacecraft walls and accumulate in dielectrics or isolated conductors; (2) Threat environment is energetic electrons with sufficient flux to charge circuit boards, cable insulation, and ungrounded metal faster than charge can dissipate; (3) Accumulating charge density generates electric fields in excess of material breakdown strenght resulting in electrostatic discharge; and (4) System impact is material damage, discharge currents inside of spacecraft Faraday cage on or near critical circuitry, and RF noise.

  18. Nickel-hydrogen battery state of charge during low rate trickle charging

    NASA Technical Reports Server (NTRS)

    Lurie, C.; Foroozan, S.; Brewer, J.; Jackson, L.

    1996-01-01

    The NASA AXAF-I program requires high battery state of charge at launch. Traditional approaches to providing high state of charge, during prelaunch operations, require significant battery cooling. The use of active cooling, in the AXAF-I prelaunch environment, was considered and proved to be difficult to implement and very expensive. Accordingly alternate approaches were considered. An approach utilizing adiabatic charging and low rate trickle charge, was investigated and proved successful.

  19. Electrostatic field and charge distribution in small charged dielectric droplets

    NASA Astrophysics Data System (ADS)

    Storozhev, V. B.

    2004-08-01

    The charge distribution in small dielectric droplets is calculated on the basis of continuum medium approximation. There are considered charged liquid spherical droplets of methanol in the range of nanometer sizes. The problem is solved by the following way. We find the free energy of some ion in dielectric droplet, which is a function of distribution of other ions in the droplet. The probability of location of the ion in some element of volume in the droplet is a function of its free energy in this element of volume. The same approach can be applied to other ions in the droplet. The obtained charge distribution differs considerably from the surface distribution. The curve of the charge distribution in the droplet as a function of radius has maximum near the surface. Relative concentration of charges in the vicinity of the center of the droplet does not equal to zero, and it is the higher, the less is the total charge of the droplet. According to the estimates the model is applicable if the droplet radius is larger than 10 nm.

  20. 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.

  1. The Gibbs Variational Method in Thermodynamics of Equilibrium Plasma: 1. General Conditions of Equilibrium and Stability for One-Component Charged Gas

    DTIC Science & Technology

    2018-04-01

    systems containing ionized gases. 2. Gibbs Method in the Integral Form As per the Gibbs general methodology , based on the concept of heterogeneous...ARL-TR-8348 ● APR 2018 US Army Research Laboratory The Gibbs Variational Method in Thermodynamics of Equilibrium Plasma: 1...ARL-TR-8348 ● APR 2018 US Army Research Laboratory The Gibbs Variational Method in Thermodynamics of Equilibrium Plasma: 1. General

  2. 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.

  3. Albuginosus, A New Subgenus of Aedes Meigen (Diptera: Culicidae) Described from the Afrotropical Region

    DTIC Science & Technology

    1986-01-01

    p. Blanchard , R. 1905. Les moustiques histoire naturelle et medicale. F. R. de Rudeval, Paris, 673 p. Brottes, I-I., A. Rickenbach, P. Bres, J-J...Salaun and L. Ferrara. 1966. Les arbovirus au Cameroun, isolements a partir de moustiques . Bull. Wld. I-Ilth. Org. 35: 811-825. Cordellie r, R

  4. Charged reflecting stars supporting charged massive scalar field configurations

    NASA Astrophysics Data System (ADS)

    Hod, Shahar

    2018-03-01

    The recently published no-hair theorems of Hod, Bhattacharjee, and Sarkar have revealed the intriguing fact that horizonless compact reflecting stars cannot support spatially regular configurations made of scalar, vector and tensor fields. In the present paper we explicitly prove that the interesting no-hair behavior observed in these studies is not a generic feature of compact reflecting stars. In particular, we shall prove that charged reflecting stars can support charged massive scalar field configurations in their exterior spacetime regions. To this end, we solve analytically the characteristic Klein-Gordon wave equation for a linearized charged scalar field of mass μ , charge coupling constant q, and spherical harmonic index l in the background of a spherically symmetric compact reflecting star of mass M, electric charge Q, and radius R_{ {s}}≫ M,Q. Interestingly, it is proved that the discrete set {R_{ {s}}(M,Q,μ ,q,l;n)}^{n=∞}_{n=1} of star radii that can support the charged massive scalar field configurations is determined by the characteristic zeroes of the confluent hypergeometric function. Following this simple observation, we derive a remarkably compact analytical formula for the discrete spectrum of star radii in the intermediate regime M≪ R_{ {s}}≪ 1/μ . The analytically derived resonance spectrum is confirmed by direct numerical computations.

  5. JPRS Report East Asia Southeast Asia

    DTIC Science & Technology

    1987-06-29

    Split UMNO Charged (NEW STRAITS TIMES, 7, 11 May 87) 44 ’Frustrated Millionaires’ Accused 44 Junid Sees No Security Threat 44 MCA Appeal to DAP ...SIN CHEW JIT POH MALAYSIA, 30 Apr 87) 50 Editorial on MCA- DAP Talks (NANYANG SIANG PAO, 30 Apr 87) 52 PBDS Chief on Remaining in Barisan... Ibrahim Hasan as factors "which must be taken into account." The "deflation" of the United Development Party also had its effect. Indonesianization

  6. Charge exchange system

    DOEpatents

    Anderson, Oscar A.

    1978-01-01

    An improved charge exchange system for substantially reducing pumping requirements of excess gas in a controlled thermonuclear reactor high energy neutral beam injector. The charge exchange system utilizes a jet-type blanket which acts simultaneously as the charge exchange medium and as a shield for reflecting excess gas.

  7. Portable refrigerant charge meter and method for determining the actual refrigerant charge in HVAC systems

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

    Gao, Zhiming; Abdelaziz, Omar; LaClair, Tim L.

    A refrigerant charge meter and a method for determining the actual refrigerant charge in HVAC systems are described. The meter includes means for determining an optimum refrigerant charge from system subcooling and system component parameters. The meter also includes means for determining the ratio of the actual refrigerant charge to the optimum refrigerant charge. Finally, the meter includes means for determining the actual refrigerant charge from the optimum refrigerant charge and the ratio of the actual refrigerant charge to the optimum refrigerant charge.

  8. The charging security study of electric vehicle charging spot based on automatic testing platform

    NASA Astrophysics Data System (ADS)

    Li, Yulan; Yang, Zhangli; Zhu, Bin; Ran, Shengyi

    2018-03-01

    With the increasing of charging spots, the testing of charging security and interoperability becomes more and more urgent and important. In this paper, an interface simulator for ac charging test is designed, the automatic testing platform for electric vehicle charging spots is set up and used to test and analyze the abnormal state during the charging process. On the platform, the charging security and interoperability of ac charging spots and IC-CPD can be checked efficiently, the test report can be generated automatically with No artificial reading error. From the test results, the main reason why the charging spot is not qualified is that the power supply cannot be cut off in the prescribed time when the charging anomaly occurs.

  9. Threshold-Based Random Charging Scheme for Decentralized PEV Charging Operation in a Smart Grid.

    PubMed

    Kwon, Ojin; Kim, Pilkee; Yoon, Yong-Jin

    2016-12-26

    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 charging, charging coordination techniques have become one of the most critical factors to optimize the PEV charging 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 charging (TBRC) operation for a decentralized charging system is proposed. Using PEV charging thresholds and random access rates, the PEVs themselves can participate in the charging requests. As PEVs with a high battery state do not transmit the charging requests to the central controller, the complexity of the central controller decreases due to the reduction of the charging requests. In addition, both the charging threshold and the random access rate are statistically calculated based on the average of supply power of the PEV charging system that do not require a real time update. By using the proposed TBRC with a tolerable PEV charging degradation, a 51% reduction of the PEV charging requests is achieved.

  10. Threshold-Based Random Charging Scheme for Decentralized PEV Charging Operation in a Smart Grid

    PubMed Central

    Kwon, Ojin; Kim, Pilkee; Yoon, Yong-Jin

    2016-01-01

    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 charging, charging coordination techniques have become one of the most critical factors to optimize the PEV charging 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 charging (TBRC) operation for a decentralized charging system is proposed. Using PEV charging thresholds and random access rates, the PEVs themselves can participate in the charging requests. As PEVs with a high battery state do not transmit the charging requests to the central controller, the complexity of the central controller decreases due to the reduction of the charging requests. In addition, both the charging threshold and the random access rate are statistically calculated based on the average of supply power of the PEV charging system that do not require a real time update. By using the proposed TBRC with a tolerable PEV charging degradation, a 51% reduction of the PEV charging requests is achieved. PMID:28035963

  11. Controlling charge on levitating drops.

    PubMed

    Hilger, Ryan T; Westphall, Michael S; Smith, Lloyd M

    2007-08-01

    Levitation technologies are used in containerless processing of materials, as microscale manipulators and reactors, and in the study of single drops and particles. Presented here is a method for controlling the amount and polarity of charge on a levitating drop. The method uses single-axis acoustic levitation to trap and levitate a single, initially neutral drop with a diameter between 400 microm and 2 mm. This drop is then charged in a controllable manner using discrete packets of charge in the form of charged drops produced by a piezoelectric drop-on-demand dispenser equipped with a charging electrode. The magnitude of the charge on the dispensed drops can be adjusted by varying the voltage applied to the charging electrode. The polarity of the charge on the added drops can be changed allowing removal of charge from the trapped drop (by neutralization) and polarity reversal. The maximum amount of added charge is limited by repulsion of like charges between the drops in the trap. This charging scheme can aid in micromanipulation and the study of charged drops and particles using levitation.

  12. Gated charged-particle trap

    DOEpatents

    Benner, W.H.

    1999-03-09

    The design and operation of a new type of charged-particle trap provides simultaneous measurements of mass, charge, and velocity of large electrospray ions. The trap consists of a detector tube mounted between two sets of center-bored trapping plates. Voltages applied to the trapping plates define symmetrically-opposing potential valleys which guide axially-injected ions to cycle back and forth through the charge-detection tube. A low noise charge-sensitive amplifier, connected to the tube, reproduces the image charge of individual ions as they pass through the detector tube. Ion mass is calculated from measurement of ion charge and velocity following each passage through the detector. 5 figs.

  13. Optimization of BEV Charging Strategy

    NASA Astrophysics Data System (ADS)

    Ji, Wei

    This paper presents different approaches to optimize fast charging and workplace charging strategy of battery electric vehicle (BEV) drivers. For the fast charging analysis, a rule-based model was built to simulate BEV charging behavior. Monte Carlo analysis was performed to explore to the potential range of congestion at fast charging stations which could be more than four hours at the most crowded stations. Genetic algorithm was performed to explore the theoretical minimum waiting time at fast charging stations, and it can decrease the waiting time at the most crowded stations to be shorter than one hour. A deterministic approach was proposed as a feasible suggestion that people should consider to take fast charging when the state of charge is approaching 40 miles. This suggestion is hoped to help to minimize potential congestion at fast charging stations. For the workplace charging analysis, scenario analysis was performed to simulate temporal distribution of charging demand under different workplace charging strategies. It was found that if BEV drivers charge as much as possible and as late as possible at workplace, it could increase the utility of solar-generated electricity while relieve grid stress of extra intensive electricity demand at night caused by charging electric vehicles at home.

  14. Spacecraft Charging Calculations: NASCAP-2K and SEE Spacecraft Charging Handbook

    NASA Technical Reports Server (NTRS)

    Davis, V. A.; Neergaard, L. F.; Mandell, M. J.; Katz, I.; Gardner, B. M.; Hilton, J. M.; Minor, J.

    2002-01-01

    For fifteen years NASA and the Air Force Charging Analyzer Program for Geosynchronous Orbits (NASCAP/GEO) has been the workhorse of spacecraft charging calculations. Two new tools, the Space Environment and Effects (SEE) Spacecraft Charging Handbook (recently released), and Nascap-2K (under development), use improved numeric techniques and modern user interfaces to tackle the same problem. The SEE Spacecraft Charging Handbook provides first-order, lower-resolution solutions while Nascap-2K provides higher resolution results appropriate for detailed analysis. This paper illustrates how the improvements in the numeric techniques affect the results.

  15. Determining the maximum charging currents of lithium-ion cells for small charge quantities

    NASA Astrophysics Data System (ADS)

    Grimsmann, F.; Gerbert, T.; Brauchle, F.; Gruhle, A.; Parisi, J.; Knipper, M.

    2017-10-01

    In order to optimize the operating parameters of battery management systems for electric and hybrid vehicles, great interest has been shown in achieving the maximum permissible charging currents during recuperation, without causing a cell damage due to lithium plating, in relation to the temperature, charge quantity and state of charge. One method for determining these recuperation currents is measuring the cell thickness, where excessively high charging currents can be detected by an irreversible increase in thickness. It is not possible to measure particularly small charge quantities by employing mechanic dial indicators, which have a limited resolution of 1 μm. This is why we developed a measuring setup that has a resolution limit of less than 10 nm using a high-resolution contactless inductance sensor. Our results show that the permissible charging current I can be approximated in relation to the charge quantity x by a correlating function I =a /√{(x) } which is compliant with the Arrhenius law. Small charge quantities therefore have an optimization potential for energy recovery during recuperation.

  16. Like-charged protein-polyelectrolyte complexation driven by charge patches

    NASA Astrophysics Data System (ADS)

    Yigit, Cemil; Heyda, Jan; Ballauff, Matthias; Dzubiella, Joachim

    2015-08-01

    We study the pair complexation of a single, highly charged polyelectrolyte (PE) chain (of 25 or 50 monomers) with like-charged patchy protein models (CPPMs) by means of implicit-solvent, explicit-salt Langevin dynamics computer simulations. Our previously introduced set of CPPMs embraces well-defined zero-, one-, and two-patched spherical globules each of the same net charge and (nanometer) size with mono- and multipole moments comparable to those of globular proteins with similar size. We observe large binding affinities between the CPPM and the like-charged PE in the tens of the thermal energy, kBT, that are favored by decreasing salt concentration and increasing charge of the patch(es). Our systematic analysis shows a clear correlation between the distance-resolved potentials of mean force, the number of ions released from the PE, and CPPM orientation effects. In particular, we find a novel two-site binding behavior for PEs in the case of two-patched CPPMs, where intermediate metastable complex structures are formed. In order to describe the salt-dependence of the binding affinity for mainly dipolar (one-patched) CPPMs, we introduce a combined counterion-release/Debye-Hückel model that quantitatively captures the essential physics of electrostatic complexation in our systems.

  17. Charge-pump voltage converter

    DOEpatents

    Brainard, John P [Albuquerque, NM; Christenson, Todd R [Albuquerque, NM

    2009-11-03

    A charge-pump voltage converter for converting a low voltage provided by a low-voltage source to a higher voltage. Charge is inductively generated on a transfer rotor electrode during its transit past an inductor stator electrode and subsequently transferred by the rotating rotor to a collector stator electrode for storage or use. Repetition of the charge transfer process leads to a build-up of voltage on a charge-receiving device. Connection of multiple charge-pump voltage converters in series can generate higher voltages, and connection of multiple charge-pump voltage converters in parallel can generate higher currents. Microelectromechanical (MEMS) embodiments of this invention provide a small and compact high-voltage (several hundred V) voltage source starting with a few-V initial voltage source. The microscale size of many embodiments of this invention make it ideally suited for MEMS- and other micro-applications where integration of the voltage or charge source in a small package is highly desirable.

  18. Charge instabilities due to local charge conjugation symmetry in /2+1 dimensions

    NASA Astrophysics Data System (ADS)

    Bais, F. A.; Striet, J.

    2003-08-01

    Alice electrodynamics (AED) is a theory of electrodynamics in which charge conjugation is a local gauge symmetry. In this paper we investigate a charge instability in alice electrodynamics in 2+1 dimensions due to this local charge conjugation. The instability manifests itself through the creation of a pair of alice fluxes. The final state is one in which the charge is completely delocalized, i.e., it is carried as cheshire charge by the flux pair that gets infinitely separated. We determine the decay rate in terms of the parameters of the model. The relation of this phenomenon with other salient features of 2-dimensional compact QED, such as linear confinement due to instantons/monopoles, is discussed.

  19. Quantum Theory of Atoms in Molecules Charge-Charge Transfer-Dipolar Polarization Classification of Infrared Intensities.

    PubMed

    Duarte, Leonardo J; Richter, Wagner E; Silva, Arnaldo F; Bruns, Roy E

    2017-10-26

    Fundamental infrared vibrational transition intensities of gas-phase molecules are sensitive probes of changes in electronic structure accompanying small molecular distortions. Models containing charge, charge transfer, and dipolar polarization effects are necessary for a successful classification of the C-H, C-F, and C-Cl stretching and bending intensities. C-H stretching and in-plane bending vibrations involving sp 3 carbon atoms have small equilibrium charge contributions and are accurately modeled by the charge transfer-counterpolarization contribution and its interaction with equilibrium charge movement. Large C-F and C═O stretching intensities have dominant equilibrium charge movement contributions compared to their charge transfer-dipolar polarization ones and are accurately estimated by equilibrium charge and the interaction contribution. The C-F and C-Cl bending modes have charge and charge transfer-dipolar polarization contribution sums that are of similar size but opposite sign to their interaction values resulting in small intensities. Experimental in-plane C-H bends have small average intensities of 12.6 ± 10.4 km mol -1 owing to negligible charge contributions and charge transfer-counterpolarization cancellations, whereas their average out-of-plane experimental intensities are much larger, 65.7 ± 20.0 km mol -1 , as charge transfer is zero and only dipolar polarization takes place. The C-F bending intensities have large charge contributions but very small intensities. Their average experimental out-of-plane intensity of 9.9 ± 12.6 km mol -1 arises from the cancellation of large charge contributions by dipolar polarization contributions. The experimental average in-plane C-F bending intensity, 5.8 ± 7.3 km mol -1 , is also small owing to charge and charge transfer-counterpolarization sums being canceled by their interaction contributions. Models containing only atomic charges and their fluxes are incapable of describing electronic structure

  20. Interaction of Charged Patchy Protein Models with Like-Charged Polyelectrolyte Brushes.

    PubMed

    Yigit, Cemil; Kanduč, Matej; Ballauff, Matthias; Dzubiella, Joachim

    2017-01-10

    We study the adsorption of charged patchy particle models (CPPMs) on a thin film of a like-charged and dense polyelectrolyte (PE) brush (of 50 monomers per chain) by means of implicit-solvent, explicit-salt Langevin dynamics computer simulations. Our previously introduced set of CPPMs embraces well-defined one- and two-patched spherical globules, each of the same net charge and (nanometer) size, with mono- and multipole moments comparable to those of small globular proteins. We focus on electrostatic effects on the adsorption far away from the isoelectric point of typical proteins, i.e., where charge regulation plays no role. Despite the same net charge of the brush and globule, we observe large binding affinities up to tens of the thermal energy, k B T, which are enhanced by decreasing salt concentration and increasing charge of the patch(es). Our analysis of the distance-resolved potentials of mean force together with a phenomenological description of all leading interaction contributions shows that the attraction is strongest at the brush surface, driven by multipolar, Born (self-energy), and counterion-release contributions, dominating locally over the monopolar and steric repulsions.

  1. Rain Drop Charge Sensor

    NASA Astrophysics Data System (ADS)

    S, Sreekanth T.

    begin{center} Large Large Rain Drop Charge Sensor Sreekanth T S*, Suby Symon*, G. Mohan Kumar (1) , S. Murali Das (2) *Atmospheric Sciences Division, Centre for Earth Science Studies, Thiruvananthapuram 695011 (1) D-330, Swathi Nagar, West Fort, Thiruvananthapuram 695023 (2) Kavyam, Manacaud, Thiruvananthapuram 695009 begin{center} ABSTRACT To study the inter-relations with precipitation electricity and precipitation microphysical parameters a rain drop charge sensor was designed and developed at CESS Electronics & Instrumentation Laboratory. Simultaneous measurement of electric charge and fall speed of rain drops could be done using this charge sensor. A cylindrical metal tube (sensor tube) of 30 cm length is placed inside another thick metal cover opened at top and bottom for electromagnetic shielding. Mouth of the sensor tube is exposed and bottom part is covered with metal net in the shielding cover. The instrument is designed in such a way that rain drops can pass only through unhindered inside the sensor tube. When electrically charged rain drops pass through the sensor tube, it is charged to the same magnitude of drop charge but with opposite polarity. The sensor tube is electrically connected the inverted input of a current to voltage converter operational amplifier using op-amp AD549. Since the sensor is electrically connected to the virtual ground of the op-amp, the charge flows to the ground and the generated current is converted to amplified voltage. This output voltage is recorded using a high frequency (1kHz) voltage recorder. From the recorded pulse, charge magnitude, polarity and fall speed of rain drop are calculated. From the fall speed drop diameter also can be calculated. The prototype is now under test running at CESS campus. As the magnitude of charge in rain drops is an indication of accumulated charge in clouds in lightning, this instrument has potential application in the field of risk and disaster management. By knowing the charge

  2. Particle-Charge Spectrometer

    NASA Technical Reports Server (NTRS)

    Fuerstenau, Stephen; Wilson, Gregory R.

    2008-01-01

    An instrument for rapidly measuring the electric charges and sizes (from approximately 1 to approximately 100 micrometers) of airborne particles is undergoing development. Conceived for monitoring atmospheric dust particles on Mars, instruments like this one could also be used on Earth to monitor natural and artificial aerosols in diverse indoor and outdoor settings for example, volcanic regions, clean rooms, powder-processing machinery, and spray-coating facilities. The instrument incorporates a commercially available, low-noise, ultrasensitive charge-sensing preamplifier circuit. The input terminal of this circuit--the gate of a field-effect transistor--is connected to a Faraday-cage cylindrical electrode. The charged particles of interest are suspended in air or other suitable gas that is made to flow along the axis of the cylindrical electrode without touching the electrode. The flow can be channeled and generated by any of several alternative means; in the prototype of this instrument, the gas is drawn along a glass capillary tube (see upper part of figure) coaxial with the electrode. The size of a particle affects its rate of acceleration in the flow and thus affects the timing and shape of the corresponding signal peak generated by the charge-sensing amplifier. The charge affects the magnitude (and thus also the shape) of the signal peak. Thus, the signal peak (see figure) conveys information on both the size and electric charge of a sensed particle. In experiments thus far, the instrument has been found to be capable of measuring individual aerosol particle charges of magnitude greater than 350 e (where e is the fundamental unit of electric charge) with a precision of +/- 150 e. The instrument can sample particles at a rate as high as several thousand per second.

  3. Quick spacecraft charging primer

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

    Larsen, Brian Arthur

    2014-03-12

    This is a presentation in PDF format which is a quick spacecraft charging primer, meant to be used for program training. It goes into detail about charging physics, RBSP examples, and how to identify charging.

  4. 23. 175 TON CAPACITY CHARGING LADLE ON THE CHARGING AISLE ...

    Library of Congress Historic Buildings Survey, Historic Engineering Record, Historic Landscapes Survey

    23. 175 TON CAPACITY CHARGING LADLE ON THE CHARGING AISLE OF THE BOP SHOP LOOKING SOUTH. HISTORIAN FOR SCALE. - U.S. Steel Duquesne Works, Basic Oxygen Steelmaking Plant, Along Monongahela River, Duquesne, Allegheny County, PA

  5. Benchmark Airport Charges

    NASA Technical Reports Server (NTRS)

    deWit, A.; Cohn, N.

    1999-01-01

    The Netherlands Directorate General of Civil Aviation (DGCA) commissioned Hague Consulting Group (HCG) to complete a benchmark study of airport charges at twenty eight airports in Europe and around the world, based on 1996 charges. This study followed previous DGCA research on the topic but included more airports in much more detail. The main purpose of this new benchmark study was to provide insight into the levels and types of airport charges worldwide and into recent changes in airport charge policy and structure, This paper describes the 1996 analysis. It is intended that this work be repeated every year in order to follow developing trends and provide the most up-to-date information possible.

  6. Benchmark Airport Charges

    NASA Technical Reports Server (NTRS)

    de Wit, A.; Cohn, N.

    1999-01-01

    The Netherlands Directorate General of Civil Aviation (DGCA) commissioned Hague Consulting Group (HCG) to complete a benchmark study of airport charges at twenty eight airports in Europe and around the world, based on 1996 charges. This study followed previous DGCA research on the topic but included more airports in much more detail. The main purpose of this new benchmark study was to provide insight into the levels and types of airport charges worldwide and into recent changes in airport charge policy and structure. This paper describes the 1996 analysis. It is intended that this work be repeated every year in order to follow developing trends and provide the most up-to-date information possible.

  7. Space-charge limited photocurrent.

    PubMed

    Mihailetchi, V D; Wildeman, J; Blom, P W M

    2005-04-01

    In 1971 Goodman and Rose predicted the occurrence of a fundamental electrostatic limit for the photocurrent in semiconductors at high light intensities. Blends of conjugated polymers and fullerenes are an ideal model system to observe this space-charge limit experimentally, since they combine an unbalanced charge transport, long lifetimes, high charge carrier generation efficiencies, and low mobility of the slowest charge carrier. The experimental photocurrents reveal all the characteristics of a space-charge limited photocurrent: a one-half power dependence on voltage, a three-quarter power dependence on light intensity, and a one-half power scaling of the voltage at which the photocurrent switches into full saturation with light intensity.

  8. Azimuthal angle dependence of the charge imbalance from charge conservation effects

    NASA Astrophysics Data System (ADS)

    BoŻek, Piotr

    2018-03-01

    The experimental search for the chiral magnetic effect in heavy-ion collisions is based on charge-dependent correlations between emitted particles. Recently, a sensitive observable comparing event-by-event distributions of the charge splitting projected on the directions along and perpendicular to the direction of the elliptic flow has been proposed. The results of a (3 + 1)-dimensional hydrodynamic model show that the preliminary experimental data of the STAR Collaboration can be explained as due to background effects, such as resonance decays and local charge conservation in the particle production. A related observable based on the third-order harmonic flow is proposed to further investigate such background effects in charge-dependent correlations.

  9. Modeling the Partial Atomic Charges in Inorganometallic Molecules and Solids and Charge Redistribution in Lithium-Ion Cathodes

    DOE PAGES

    Wang, Bo; Li, Shaohong L.; Truhlar, Donald G.

    2014-10-30

    Partial atomic charges are widely used for the description of charge distributions of molecules and solids. These charges are useful to indicate the extent of charge transfer and charge flow during chemical reactions in batteries, fuel cells, and catalysts and to characterize charge distributions in capacitors, liquid-phase electrolytes, and solids and at electrochemical interfaces. However, partial atomic charges given by various charge models differ significantly, especially for systems containing metal atoms. In the present study, we have compared various charge models on both molecular systems and extended systems, including Hirshfeld, CM5, MK, ChElPG, Mulliken, MBS, NPA, DDEC, LoProp, and Badermore » charges. Their merits and drawbacks are compared. The CM5 charge model is found to perform well on the molecular systems, with a mean unsigned percentage deviation of only 9% for the dipole moments. We therefore formulated it for extended systems and applied it to study charge flow during the delithiation process in lithium-containing oxides used as cathodes. Our calculations show that the charges given by the CM5 charge model are reasonable and that during the delithiation process, the charge flow can occur not only on the transition metal but also on the anions. The oxygen atoms can lose a significant density of electrons, especially for deeply delithiated materials. We also discuss other methods in current use to analyze the charge transfer and charge flow in batteries, in particular the use of formal charge, spin density, and orbital occupancy. Here, we conclude that CM5 charges provide useful information in describing charge distributions in various materials and are very promising for the study of charge transfer and charge flows in both molecules and solids.« less

  10. Modeling the Partial Atomic Charges in Inorganometallic Molecules and Solids and Charge Redistribution in Lithium-Ion Cathodes.

    PubMed

    Wang, Bo; Li, Shaohong L; Truhlar, Donald G

    2014-12-09

    Partial atomic charges are widely used for the description of charge distributions of molecules and solids. These charges are useful to indicate the extent of charge transfer and charge flow during chemical reactions in batteries, fuel cells, and catalysts and to characterize charge distributions in capacitors, liquid-phase electrolytes, and solids and at electrochemical interfaces. However, partial atomic charges given by various charge models differ significantly, especially for systems containing metal atoms. In the present study, we have compared various charge models on both molecular systems and extended systems, including Hirshfeld, CM5, MK, ChElPG, Mulliken, MBS, NPA, DDEC, LoProp, and Bader charges. Their merits and drawbacks are compared. The CM5 charge model is found to perform well on the molecular systems, with a mean unsigned percentage deviation of only 9% for the dipole moments. We therefore formulated it for extended systems and applied it to study charge flow during the delithiation process in lithium-containing oxides used as cathodes. Our calculations show that the charges given by the CM5 charge model are reasonable and that during the delithiation process, the charge flow can occur not only on the transition metal but also on the anions. The oxygen atoms can lose a significant density of electrons, especially for deeply delithiated materials. We also discuss other methods in current use to analyze the charge transfer and charge flow in batteries, in particular the use of formal charge, spin density, and orbital occupancy. We conclude that CM5 charges provide useful information in describing charge distributions in various materials and are very promising for the study of charge transfer and charge flows in both molecules and solids.

  11. ION PRODUCING MECHANISM (CHARGE CUPS)

    DOEpatents

    Brobeck, W.W.

    1959-04-21

    The problems of confining a charge material in a calutron and uniformly distributing heat to the charge is described. The charge is held in a cup of thermally conductive material removably disposed within the charge chamber of the ion source block. A central thermally conducting stem is incorporated within the cup for conducting heat to the central portion of the charge contained within the cup.

  12. Measuring momentum for charged particle tomography

    DOEpatents

    Morris, Christopher; Fraser, Andrew Mcleod; Schultz, Larry Joe; Borozdin, Konstantin N.; Klimenko, Alexei Vasilievich; Sossong, Michael James; Blanpied, Gary

    2010-11-23

    Methods, apparatus and systems for detecting charged particles and obtaining tomography of a volume by measuring charged particles including measuring the momentum of a charged particle passing through a charged particle detector. Sets of position sensitive detectors measure scattering of the charged particle. The position sensitive detectors having sufficient mass to cause the charged particle passing through the position sensitive detectors to scatter in the position sensitive detectors. A controller can be adapted and arranged to receive scattering measurements of the charged particle from the charged particle detector, determine at least one trajectory of the charged particle from the measured scattering; and determine at least one momentum measurement of the charged particle from the at least one trajectory. The charged particle can be a cosmic ray-produced charged particle, such as a cosmic ray-produced muon. The position sensitive detectors can be drift cells, such as gas-filled drift tubes.

  13. 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.

  14. Ion association at discretely-charged dielectric interfaces: Giant charge inversion [Dielectric response controlled ion association at physically heterogeneous surfaces: Giant charge reversal

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

    Wang, Zhi -Yong; Wu, Jianzhong

    2017-07-11

    Giant charge reversal has been identified for the first time by Monte Carlo simulation for a discretely charged surface in contact with a trivalent electrolyte solution. It takes place regardless of the surface charge density under study and the monovalent salt. In stark contrast to earlier predictions based on the 2-dimensional Wigner crystal model to describe strong correlation of counterions at the macroion surface, we find that giant charge reversal reflects an intricate interplay of ionic volume effects, electrostatic correlations, surface charge heterogeneity, and the dielectric response of the confined fluids. While the novel phenomenon is yet to be confirmedmore » with experiment, the simulation results appear in excellent agreement with a wide range of existing observations in the subregime of charge inversion. Lastly, our findings may have far-reaching implications to understanding complex electrochemical phenomena entailing ionic fluids under dielectric confinements.« less

  15. Spacecraft Charging Technology, 1980

    NASA Technical Reports Server (NTRS)

    1981-01-01

    The third Spacecraft Charging Technology Conference proceedings contain 66 papers on the geosynchronous plasma environment, spacecraft modeling, charged particle environment interactions with spacecraft, spacecraft materials characterization, and satellite design and testing. The proceedings is a compilation of the state of the art of spacecraft charging and environmental interaction phenomena.

  16. State-of-charge coulometer

    NASA Technical Reports Server (NTRS)

    Rowlette, J. J. (Inventor)

    1985-01-01

    A coulometer for accurately measuring the state-of-charge of an open-cell battery utilizing an aqueous electrolyte, includes a current meter for measuring the battery/discharge current and a flow meter for measuring the rate at which the battery produces gas during charge and discharge. Coupled to the flow meter is gas analyzer which measures the oxygen fraction of the battery gas. The outputs of the current meter, flow meter, and gas analyzer are coupled to a programmed microcomputer which includes a CPU and program and data memories. The microcomputer calculates that fraction of charge and discharge current consumed in the generation of gas so that the actual state-of-charge can be determined. The state-of-charge is then shown on a visual display.

  17. Influence of layer charge and charge distribution of smectites on the flow behaviour and swelling of bentonites

    USGS Publications Warehouse

    Christidis, G.E.; Blum, A.E.; Eberl, D.D.

    2006-01-01

    The influence of layer charge and charge distribution of dioctahedral smectites on the rheological and swelling properties of bentonites is examined. Layer charge and charge distribution were determined by XRD using the LayerCharge program [Christidis, G.E., Eberl, D.D., 2003. Determination of layer charge characteristics of smectites. Clays Clay Miner. 51, 644-655.]. The rheological properties were determined, after sodium exchange using the optimum amount of Na2CO3, from free swelling tests. Rheological properties were determined using 6.42% suspensions according to industrial practice. In smectites with layer charges of - 0.425 to - 0.470 per half formula unit (phfu), layer charge is inversely correlated with free swelling, viscosity, gel strength, yield strength and thixotropic behaviour. In these smectites, the rheological properties are directly associated with the proportion of low charge layers. By contrast, in low charge and high charge smectites there is no systematic relation between layer charge or the proportion of low charge layers and rheological properties. However, low charge smectites yield more viscous suspensions and swell more than high charge smectites. The rheological properties of bentonites also are affected by the proportion of tetrahedral charge (i.e. beidellitic charge), by the existence of fine-grained minerals having clay size, such as opal-CT and to a lesser degree by the ionic strength and the pH of the suspension. A new method for classification of smectites according to the layer charge based on the XRD characteristics of smecites is proposed, that also is consistent with variations in rheological properties. In this classification scheme the term smectites with intermediate layer charge is proposed. ?? 2006 Elsevier B.V. All rights reserved.

  18. Nickel-hydrogen battery state of charge during low rate trickle charging

    NASA Technical Reports Server (NTRS)

    Lurie, C.; Foroozan, S.; Brewer, J.; Jackson, L.

    1995-01-01

    Battery temperature increase, due to low rate trickle charging, has been determined experimentally, using a six cell battery module in a test setup simulating the anticipated AXAF-1 prelaunch environment. Test results indicate trickle charge rates less than or equal to the self discharge rate do not increase dissipation beyond that due to the self discharge. Significant trickle charge rates (approximately C/500) result in battery temperatures only a few degrees (F) higher than those observed during periods of open circuit stand.

  19. Experiments on Dust Grain Charging

    NASA Technical Reports Server (NTRS)

    Abbas, M. N.; Craven, P. D.; Spann, J. F.; Tankosic, D.; LeClair, A.; West, E. A.

    2004-01-01

    Dust particles in various astrophysical environments are charged by a variety of mechanisms generally involving collisional processes with other charged particles and photoelectric emission with UV radiation from nearby sources. The sign and the magnitude of the particle charge are determined by the competition between the charging processes by UV radiation and collisions with charged particles. Knowledge of the particle charges and equilibrium potentials is important for understanding of a number of physical processes. The charge of a dust grain is thus a fundamental parameter that influences the physics of dusty plasmas, processes in the interplanetary medium and interstellar medium, interstellar dust clouds, planetary rings, cometary and outer atmospheres of planets etc. In this paper we present some results of experiments on charging of dust grains carried out on a laboratory facility capable levitating micron size dust grains in an electrodynamic balance in simulated space environments. The charging/discharging experiments were carried out by exposing the dust grains to energetic electron beams and UV radiation. Photoelectric efficiencies and yields of micron size dust grains of SiO2, and lunar simulates obtained from NASA-JSC will be presented.

  20. Collisional charging of individual submillimeter particles: Using ultrasonic levitation to initiate and track charge transfer

    NASA Astrophysics Data System (ADS)

    Lee, Victor; James, Nicole M.; Waitukaitis, Scott R.; Jaeger, Heinrich M.

    2018-03-01

    Electrostatic charging of insulating fine particles can be responsible for numerous phenomena ranging from lightning in volcanic plumes to dust explosions. However, even basic aspects of how fine particles become charged are still unclear. Studying particle charging is challenging because it usually involves the complexities associated with many-particle collisions. To address these issues, we introduce a method based on acoustic levitation, which makes it possible to initiate sequences of repeated collisions of a single submillimeter particle with a flat plate, and to precisely measure the particle charge in situ after each collision. We show that collisional charge transfer between insulators is dependent on the hydrophobicity of the contacting surfaces. We use glass, which we modify by attaching nonpolar molecules to the particle, the plate, or both. We find that hydrophilic surfaces develop significant positive charges after contacting hydrophobic surfaces. Moreover, we demonstrate that charging between a hydrophilic and a hydrophobic surface is suppressed in an acidic environment and enhanced in a basic one. Application of an electric field during each collision is found to modify the charge transfer, again depending on surface hydrophobicity. We discuss these results within the context of contact charging due to ion transfer, and we show that they lend strong support to O H- ions as the charge carriers.

  1. 12 CFR 226.4 - Finance charge.

    Code of Federal Regulations, 2013 CFR

    2013-01-01

    ... 12 Banks and Banking 3 2013-01-01 2013-01-01 false Finance charge. 226.4 Section 226.4 Banks and...) TRUTH IN LENDING (REGULATION Z) General § 226.4 Finance charge. (a) Definition. The finance charge is... transaction. (1) Charges by third parties. The finance charge includes fees and amounts charged by someone...

  2. 12 CFR 226.4 - Finance charge.

    Code of Federal Regulations, 2014 CFR

    2014-01-01

    ... 12 Banks and Banking 3 2014-01-01 2014-01-01 false Finance charge. 226.4 Section 226.4 Banks and...) TRUTH IN LENDING (REGULATION Z) General § 226.4 Finance charge. (a) Definition. The finance charge is... transaction. (1) Charges by third parties. The finance charge includes fees and amounts charged by someone...

  3. Charge regulation circuit

    DOEpatents

    Ball, Don G.

    1992-01-01

    A charge regulation circuit provides regulation of an unregulated voltage supply in the range of 0.01%. The charge regulation circuit is utilized in a preferred embodiment in providing regulated voltage for controlling the operation of a laser.

  4. CHARGE-2 rocket observations of vehicle charging and charge neutralization

    NASA Astrophysics Data System (ADS)

    Banks, P. M.; Gilchrist, B. E.; Neubert, T.; Myers, N.; Raitt, W. J.; Williamson, P. R.; Fraser-Smith, A. C.; Sasaki, S.

    Observations of electrical charging and other phenomena have been made in the ionosphere with the CHARGE-2 tethered rocket system. In this experiment, two electrically connected payloads with a variety of plasma instruments measured effects associated with operation of a 1 keV, 40 mA electron gun and a 450-volt dc power supply. During electron beam operations, it was found that both mother and daughter payloads reached high positive potentials as a consequence of the restricted electron current collecting area of the payloads. During neutral gas thruster firings, the payload potentials were dramatically reduced, indicating that electrical discharges could effectively ground each payload to plasma potential. Other thruster-related effects were also seen, including substantial reductions of return current-associated electrical noise at HF and VLF and large increases in 3914 A light in the plasma sheath.

  5. 12 CFR 226.4 - Finance charge.

    Code of Federal Regulations, 2012 CFR

    2012-01-01

    ... 12 Banks and Banking 3 2012-01-01 2012-01-01 false Finance charge. 226.4 Section 226.4 Banks and... LENDING (REGULATION Z) General § 226.4 Finance charge. (a) Definition. The finance charge is the cost of...) Charges by third parties. The finance charge includes fees and amounts charged by someone other than the...

  6. Charge gradient microscopy

    DOEpatents

    Roelofs, Andreas; Hong, Seungbum

    2018-02-06

    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 addition, the method includes moving the tip across the surface of the material specimen while removing electrical charge therefrom, generating a signal produced by contact between the tip and the surface, and detecting, based on the data, the removed electrical charge induced through the tip during movement of the tip across the surface. The method further includes measuring the detected electrical charge.

  7. 25 CFR 143.4 - Charges.

    Code of Federal Regulations, 2010 CFR

    2010-04-01

    ... 25 Indians 1 2010-04-01 2010-04-01 false Charges. 143.4 Section 143.4 Indians BUREAU OF INDIAN AFFAIRS, DEPARTMENT OF THE INTERIOR FINANCIAL ACTIVITIES CHARGES FOR GOODS AND SERVICES PROVIDED TO NON-FEDERAL USERS § 143.4 Charges. (a) Charges shall be established by the Assistant Secretary and shall be...

  8. Charged-particle emission tomography

    PubMed Central

    Ding, Yijun; Caucci, Luca; Barrett, Harrison H.

    2018-01-01

    Purpose Conventional charged-particle imaging techniques —such as autoradiography —provide only two-dimensional (2D) black ex vivo images of thin tissue slices. In order to get volumetric information, images of multiple thin slices are stacked. This process is time consuming and prone to distortions, as registration of 2D images is required. We propose a direct three-dimensional (3D) autoradiography technique, which we call charged-particle emission tomography (CPET). This 3D imaging technique enables imaging of thick tissue sections, thus increasing laboratory throughput and eliminating distortions due to registration. CPET also has the potential to enable in vivo charged-particle imaging with a window chamber or an endoscope. Methods Our approach to charged-particle emission tomography uses particle-processing detectors (PPDs) to estimate attributes of each detected particle. The attributes we estimate include location, direction of propagation, and/or the energy deposited in the detector. Estimated attributes are then fed into a reconstruction algorithm to reconstruct the 3D distribution of charged-particle-emitting radionuclides. Several setups to realize PPDs are designed. Reconstruction algorithms for CPET are developed. Results Reconstruction results from simulated data showed that a PPD enables CPET if the PPD measures more attributes than just the position from each detected particle. Experiments showed that a two-foil charged-particle detector is able to measure the position and direction of incident alpha particles. Conclusions We proposed a new volumetric imaging technique for charged-particle-emitting radionuclides, which we have called charged-particle emission tomography (CPET). We also proposed a new class of charged-particle detectors, which we have called particle-processing detectors (PPDs). When a PPD is used to measure the direction and/or energy attributes along with the position attributes, CPET is feasible. PMID:28370094

  9. Charged-particle emission tomography.

    PubMed

    Ding, Yijun; Caucci, Luca; Barrett, Harrison H

    2017-06-01

    Conventional charged-particle imaging techniques - such as autoradiography - provide only two-dimensional (2D) black ex vivo images of thin tissue slices. In order to get volumetric information, images of multiple thin slices are stacked. This process is time consuming and prone to distortions, as registration of 2D images is required. We propose a direct three-dimensional (3D) autoradiography technique, which we call charged-particle emission tomography (CPET). This 3D imaging technique enables imaging of thick tissue sections, thus increasing laboratory throughput and eliminating distortions due to registration. CPET also has the potential to enable in vivo charged-particle imaging with a window chamber or an endoscope. Our approach to charged-particle emission tomography uses particle-processing detectors (PPDs) to estimate attributes of each detected particle. The attributes we estimate include location, direction of propagation, and/or the energy deposited in the detector. Estimated attributes are then fed into a reconstruction algorithm to reconstruct the 3D distribution of charged-particle-emitting radionuclides. Several setups to realize PPDs are designed. Reconstruction algorithms for CPET are developed. Reconstruction results from simulated data showed that a PPD enables CPET if the PPD measures more attributes than just the position from each detected particle. Experiments showed that a two-foil charged-particle detector is able to measure the position and direction of incident alpha particles. We proposed a new volumetric imaging technique for charged-particle-emitting radionuclides, which we have called charged-particle emission tomography (CPET). We also proposed a new class of charged-particle detectors, which we have called particle-processing detectors (PPDs). When a PPD is used to measure the direction and/or energy attributes along with the position attributes, CPET is feasible. © 2017 The Authors. Medical Physics published by Wiley Periodicals

  10. Charge-Dissipative Electrical Cables

    NASA Technical Reports Server (NTRS)

    Kolasinski, John R.; Wollack, Edward J.

    2004-01-01

    Electrical cables that dissipate spurious static electric charges, in addition 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 charges tend to accumulate within, and on the surfaces of, dielectric layers of cables. If the charging rate exceeds the dissipation rate, charges 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 charge-dissipative electrical cables is to drain spurious charges 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.

  11. Charged polymers in high dimensions

    NASA Technical Reports Server (NTRS)

    Kantor, Yacov

    1990-01-01

    A Monte Carlo study of charged polymers with either homogeneously distributed frozen charges or with mobile charges has been performed in four and five space dimensions. The results are consistent with the renormalization-group predictions and contradict the predictions of Flory-type theory. Introduction of charge mobility does not modify the behavior of the polymers.

  12. Charge transport in organic semiconductors.

    PubMed

    Bässler, Heinz; Köhler, Anna

    2012-01-01

    Modern optoelectronic devices, such as light-emitting diodes, field-effect transistors and organic solar cells require well controlled motion of charges for their efficient operation. The understanding of the processes that determine charge transport is therefore of paramount importance for designing materials with improved structure-property relationships. Before discussing different regimes of charge transport in organic semiconductors, we present a brief introduction into the conceptual framework in which we interpret the relevant photophysical processes. That is, we compare a molecular picture of electronic excitations against the Su-Schrieffer-Heeger semiconductor band model. After a brief description of experimental techniques needed to measure charge mobilities, we then elaborate on the parameters controlling charge transport in technologically relevant materials. Thus, we consider the influences of electronic coupling between molecular units, disorder, polaronic effects and space charge. A particular focus is given to the recent progress made in understanding charge transport on short time scales and short length scales. The mechanism for charge injection is briefly addressed towards the end of this chapter.

  13. Irrational Charge from Topological Order

    NASA Astrophysics Data System (ADS)

    Moessner, R.; Sondhi, S. L.

    2010-10-01

    Topological or deconfined phases of matter exhibit emergent gauge fields and quasiparticles that carry a corresponding gauge charge. In systems with an intrinsic conserved U(1) charge, such as all electronic systems where the Coulombic charge plays this role, these quasiparticles are also characterized by their intrinsic charge. We show that one can take advantage of the topological order fairly generally to produce periodic Hamiltonians which endow the quasiparticles with continuously variable, generically irrational, intrinsic charges. Examples include various topologically ordered lattice models, the three-dimensional resonating valence bond liquid on bipartite lattices as well as water and spin ice. By contrast, the gauge charges of the quasiparticles retain their quantized values.

  14. Two-phase charge-coupled device

    NASA Technical Reports Server (NTRS)

    Kosonocky, W. F.; Carnes, J. E.

    1973-01-01

    A charge-transfer efficiency of 99.99% per stage was achieved in the fat-zero mode of operation of 64- and 128-stage two-phase charge-coupled shift registers at 1.0-MHz clock frequency. The experimental two-phase charge-coupled shift registers were constructed in the form of polysilicon gates overlapped by aluminum gates. The unidirectional signal flow was accomplished by using n-type substrates with 0.5 to 1.0 ohm-cm resistivity in conjunction with a channel oxide thickness of 1000 A for the polysilicon gates and 3000 A for the aluminum gates. The operation of the tested shift registers with fat zero is in good agreement with the free-charge transfer characteristics expected for the tested structures. The charge-transfer losses observed when operating the experimental shift registers without the fat zero are attributed to fast interface state trapping. The analytical part of the report contains a review backed up by an extensive appendix of the free-charge transfer characteristics of CCD's in terms of thermal diffusion, self-induced drift, and fringing field drift. Also, a model was developed for the charge-transfer losses resulting from charge trapping by fast interface states. The proposed model was verified by the operation of the experimental two-phase charge-coupled shift registers.

  15. Protein adsorption at charged surfaces: the role of electrostatic interactions and interfacial charge regulation.

    PubMed

    Hartvig, Rune A; van de Weert, Marco; Østergaard, Jesper; Jorgensen, Lene; Jensen, Henrik

    2011-03-15

    The understanding of protein adsorption at charged surfaces is important for a wide range of scientific disciplines including surface engineering, separation sciences and pharmaceutical sciences. Compared to chemical entities having a permanent charge, the adsorption of small ampholytes and proteins is more complicated as the pH near a charged surface can be significantly different from the value in bulk solution. In this work, we have developed a phenomenological adsorption model which takes into account the combined role of interfacial ion distribution, interfacial charge regulation of amino acids in the proximity of the surface, electroneutrality, and mass balance. The model is straightforward to apply to a given set of experimental conditions as most model parameters are obtained from bulk properties and therefore easy to estimate or are directly measurable. The model provides a detailed understanding of the importance of surface charge on adsorption and in particular of how changes in surface charge, concentration, and surface area may affect adsorption behavior. The model is successfully used to explain the experimental adsorption behavior of the two model proteins lysozyme and α-lactalbumin. It is demonstrated that it is possible to predict the pH and surface charge dependent adsorption behavior from experimental or theoretical estimates of a preferred orientation of a protein at a solid charged interface.

  16. Charge-transfer modified embedded atom method dynamic charge potential for Li-Co-O system

    NASA Astrophysics Data System (ADS)

    Kong, Fantai; Longo, Roberto C.; Liang, Chaoping; Nie, Yifan; Zheng, Yongping; Zhang, Chenxi; Cho, Kyeongjae

    2017-11-01

    To overcome the limitation of conventional fixed charge potential methods for the study of Li-ion battery cathode materials, a dynamic charge potential method, charge-transfer modified embedded atom method (CT-MEAM), has been developed and applied to the Li-Co-O ternary system. The accuracy of the potential has been tested and validated by reproducing a variety of structural and electrochemical properties of LiCoO2. A detailed analysis on the local charge distribution confirmed the capability of this potential for dynamic charge modeling. The transferability of the potential is also demonstrated by its reliability in describing Li-rich Li2CoO2 and Li-deficient LiCo2O4 compounds, including their phase stability, equilibrium volume, charge states and cathode voltages. These results demonstrate that the CT-MEAM dynamic charge potential could help to overcome the challenge of modeling complex ternary transition metal oxides. This work can promote molecular dynamics studies of Li ion cathode materials and other important transition metal oxides systems that involve complex electrochemical and catalytic reactions.

  17. Charge-transfer modified embedded atom method dynamic charge potential for Li-Co-O system.

    PubMed

    Kong, Fantai; Longo, Roberto C; Liang, Chaoping; Nie, Yifan; Zheng, Yongping; Zhang, Chenxi; Cho, Kyeongjae

    2017-11-29

    To overcome the limitation of conventional fixed charge potential methods for the study of Li-ion battery cathode materials, a dynamic charge potential method, charge-transfer modified embedded atom method (CT-MEAM), has been developed and applied to the Li-Co-O ternary system. The accuracy of the potential has been tested and validated by reproducing a variety of structural and electrochemical properties of LiCoO 2 . A detailed analysis on the local charge distribution confirmed the capability of this potential for dynamic charge modeling. The transferability of the potential is also demonstrated by its reliability in describing Li-rich Li 2 CoO 2 and Li-deficient LiCo 2 O 4 compounds, including their phase stability, equilibrium volume, charge states and cathode voltages. These results demonstrate that the CT-MEAM dynamic charge potential could help to overcome the challenge of modeling complex ternary transition metal oxides. This work can promote molecular dynamics studies of Li ion cathode materials and other important transition metal oxides systems that involve complex electrochemical and catalytic reactions.

  18. Static Gas-Charging Plug

    NASA Technical Reports Server (NTRS)

    Indoe, William

    2012-01-01

    A gas-charging plug can be easily analyzed for random vibration. The design features two steeped O-rings in a radial configuration at two different diameters, with a 0.050-in. (.1.3-mm) diameter through-hole between the two O-rings. In the charging state, the top O-ring is engaged and sealing. The bottom O-ring outer diameter is not squeezed, and allows air to flow by it into the tank. The inner diameter is stretched to plug the gland diameter, and is restrained by the O-ring groove. The charging port bushing provides mechanical stop to restrain the plug during gas charge removal. It also prevents the plug from becoming a projectile when removing gas charge from the accumulator. The plug can easily be verified after installation to ensure leakage requirements are met.

  19. Effects of image charges, interfacial charge discreteness, and surface roughness on the zeta potential of spherical electric double layers.

    PubMed

    Gan, Zecheng; Xing, Xiangjun; Xu, Zhenli

    2012-07-21

    We investigate the effects of image charges, interfacial charge discreteness, and surface roughness on spherical electric double layer structures in electrolyte solutions with divalent counterions in the setting of the primitive model. By using Monte Carlo simulations and the image charge method, the zeta potential profile and the integrated charge distribution function are computed for varying surface charge strengths and salt concentrations. Systematic comparisons were carried out between three distinct models for interfacial charges: (1) SURF1 with uniform surface charges, (2) SURF2 with discrete point charges on the interface, and (3) SURF3 with discrete interfacial charges and finite excluded volume. By comparing the integrated charge distribution function and the zeta potential profile, we argue that the potential at the distance of one ion diameter from the macroion surface is a suitable location to define the zeta potential. In SURF2 model, we find that image charge effects strongly enhance charge inversion for monovalent interfacial charges, and strongly suppress charge inversion for multivalent interfacial charges. For SURF3, the image charge effect becomes much smaller. Finally, with image charges in action, we find that excluded volumes (in SURF3) suppress charge inversion for monovalent interfacial charges and enhance charge inversion for multivalent interfacial charges. Overall, our results demonstrate that all these aspects, i.e., image charges, interfacial charge discreteness, their excluding volumes, have significant impacts on zeta potentials of electric double layers.

  20. High resolution printing of charge

    DOEpatents

    Rogers, John; Park, Jang-Ung

    2015-06-16

    Provided are methods of printing a pattern of charge on a substrate surface, such as by electrohydrodynamic (e-jet) printing. The methods relate to providing a nozzle containing a printable fluid, providing a substrate having a substrate surface and generating from the nozzle an ejected printable fluid containing net charge. The ejected printable fluid containing net charge is directed to the substrate surface, wherein the net charge does not substantially degrade and the net charge retained on the substrate surface. Also provided are functional devices made by any of the disclosed methods.

  1. Effect of surface charge of immortalized mouse cerebral endothelial cell monolayer on transport of charged solutes.

    PubMed

    Yuan, Wei; Li, Guanglei; Gil, Eun Seok; Lowe, Tao Lu; Fu, Bingmei M

    2010-04-01

    Charge 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 charged 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 charge as that in the intact BBB and quantify this charge, which can be characterized by the SGL thickness (L(f)) and charge density (C(mf)), we measured the solute permeability of bEnd3 monolayer to neutral solutes and to solutes with similar size but opposite charges: negatively charged alpha-lactalbumin (-11) and positively charged 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 charge of the intact BBB, alters the charge of bEnd3 monolayer. We found that 1 mg/mL orosomucoid would increase SGL charge density of bEnd3 monolayer to approximately 2-fold of its control value.

  2. Charging of interplanetary grains

    NASA Technical Reports Server (NTRS)

    Baragiola, R. A.; Johnson, R. E.; Newcomb, John L.

    1995-01-01

    The objective of this program is to quantify, by laboratory experiments, the charging of ices and other insulators subject to irradiation with electrons, ions and ultraviolet photons and to model special conditions based on the data. The system and conditions to be studied are those relevant for charging of dust in magnetospheric plasmas. The measurements are supplemented by computer simulations of charging or grains under a variety of conditions. Our work for this period involved experiments on water ice, improved models of charging of ice grains for Saturn's E-ring, and the construction of apparatus for electron impact studies and measurements of electron energy distributions.

  3. 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/servlets/purl/1175280','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1175280"><span>Non-intrusive refrigerant <span class="hlt">charge</span> indicator</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Mei, Viung C.; Chen, Fang C.; Kweller, Esher</p> <p>2005-03-22</p> <p>A non-intrusive refrigerant <span class="hlt">charge</span> level indicator includes a structure for measuring at least one temperature at an outside surface of a two-phase refrigerant line section. The measured temperature can be used to determine the refrigerant <span class="hlt">charge</span> status of an HVAC system, and can be converted to a pressure of the refrigerant in the line section and compared to a recommended pressure range to determine whether the system is under-<span class="hlt">charged</span>, properly <span class="hlt">charged</span> or over-<span class="hlt">charged</span>. A non-intrusive method for assessing the refrigerant <span class="hlt">charge</span> level in a system containing a refrigerant fluid includes the step of measuring a temperature at least one outside surface of a two-phase region of a refrigerant containing refrigerant line, wherein the temperature measured can be converted to a refrigerant pressure within the line section.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016nova.pres.1393K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016nova.pres.1393K"><span>When <span class="hlt">Charged</span> Black Holes Merge</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kohler, Susanna</p> <p>2016-08-01</p> <p>Most theoretical models assume that black holes arent <span class="hlt">charged</span>. But a new study shows that mergers of <span class="hlt">charged</span> black holes could explain a variety of astrophysical phenomena, from fast radio bursts to gamma-ray bursts.No HairThe black hole no hair theorem states that all black holes can be described by just three things: their mass, their spin, and their <span class="hlt">charge</span>. Masses and spins have been observed and measured, but weve never measured the <span class="hlt">charge</span> of a black hole and its widely believed that real black holes dont actually have any <span class="hlt">charge</span>.That said, weve also never shown that black holes dont have <span class="hlt">charge</span>, or set any upper limits on the <span class="hlt">charge</span> that they might have. So lets suppose, for a moment, that its possible for a black hole to be <span class="hlt">charged</span>. How might that affect what we know about the merger of two black holes? A recent theoretical study by Bing Zhang (University of Nevada, Las Vegas) examines this question.Intensity profile of a fast radio burst, a sudden burst of radio emission that lasts only a few milliseconds. [Swinburne Astronomy Productions]Driving TransientsZhangs work envisions a pair of black holes in a binary system. He argues that if just one of the black holes carries <span class="hlt">charge</span> possibly retained by a rotating magnetosphere then it may be possible for the system to produce an electromagnetic signal that could accompany gravitational waves, such as a fast radio burst or a gamma-ray burst!In Zhangs model, the inspiral of the two black holes generates a global magnetic dipole thats perpendicular to the plane of the binarys orbit. The magnetic flux increases rapidly as the separation between the black holes decreases, generating an increasingly powerful magnetic wind. This wind, in turn, can give rise to a fast radio burst or a gamma-ray burst, depending on the value of the black holes <span class="hlt">charge</span>.Artists illustration of a short gamma-ray burst, thought to be caused by the merger of two compact objects. [ESO/A. Roquette]Zhang calculates lower limits on the <span class="hlt">charge</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JHEP...04..167C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JHEP...04..167C"><span><span class="hlt">Charged</span> black rings at large D</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chen, Bin; Li, Peng-Cheng; Wang, Zi-zhi</p> <p>2017-04-01</p> <p>We study the <span class="hlt">charged</span> slowly rotating black holes in the Einstein-Maxwell theory in the large dimensions ( D). By using the 1 /D expansion in the near regions of the black holes we obtain the effective equations for the <span class="hlt">charged</span> slowly rotating black holes. The effective equations capture the dynamics of various stationary solutions, including the <span class="hlt">charged</span> black ring, the <span class="hlt">charged</span> slowly rotating Myers-Perry black hole and the <span class="hlt">charged</span> slowly boosted black string. Via different embeddings we construct these stationary solutions explicitly. For the <span class="hlt">charged</span> black ring at large D, we find that the <span class="hlt">charge</span> lowers the angular momentum due to the regularity condition on the solution. By performing the perturbation analysis of the effective equations, we obtain the quasinormal modes of the <span class="hlt">charge</span> perturbation and the gravitational perturbation analytically. Like the neutral case the <span class="hlt">charged</span> thin black ring suffers from the Gregory-Laflamme-like instability under the non-axisymmetric perturbations, but the <span class="hlt">charge</span> weakens the instability. Besides, we find that the large D analysis always respects the cosmic censorship.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22053655-simulation-charge-breeding-rubidium-using-monte-carlo-charge-breeding-code-generalized-ecris-model','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22053655-simulation-charge-breeding-rubidium-using-monte-carlo-charge-breeding-code-generalized-ecris-model"><span>Simulation of <span class="hlt">charge</span> breeding of rubidium using Monte Carlo <span class="hlt">charge</span> breeding code and generalized ECRIS 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>Zhao, L.; Cluggish, B.; Kim, J. S.</p> <p>2010-02-15</p> <p>A Monte Carlo <span class="hlt">charge</span> breeding code (MCBC) is being developed by FAR-TECH, Inc. to model the capture and <span class="hlt">charge</span> breeding of 1+ ion beam in an electron cyclotron resonance ion source (ECRIS) device. The ECRIS plasma is simulated using the generalized ECRIS model which has two choices of boundary settings, free boundary condition and Bohm condition. The <span class="hlt">charge</span> state distribution of the extracted beam ions is calculated by solving the steady state ion continuity equations where the profiles of the captured ions are used as source terms. MCBC simulations of the <span class="hlt">charge</span> breeding of Rb+ showed good agreement with recentmore » <span class="hlt">charge</span> breeding experiments at Argonne National Laboratory (ANL). MCBC correctly predicted the peak of highly <span class="hlt">charged</span> ion state outputs under free boundary condition and similar <span class="hlt">charge</span> state distribution width but a lower peak <span class="hlt">charge</span> state under the Bohm condition. The comparisons between the simulation results and ANL experimental measurements are presented and discussed.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19870065191&hterms=scientific+collections&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dscientific%2Bcollections','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19870065191&hterms=scientific+collections&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dscientific%2Bcollections"><span>Scientific <span class="hlt">charge</span>-coupled devices</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Janesick, James R.; Elliott, Tom; Collins, Stewart; Blouke, Morley M.; Freeman, Jack</p> <p>1987-01-01</p> <p>The <span class="hlt">charge</span>-coupled device dominates an ever-increasing variety of scientific imaging and spectroscopy applications. Recent experience indicates, however, that the full potential of CCD performance lies well beyond that realized in devices currently available.Test data suggest that major improvements are feasible in spectral response, <span class="hlt">charge</span> collection, <span class="hlt">charge</span> transfer, and readout noise. These properties, their measurement in existing CCDs, and their potential for future improvement are discussed in this paper.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011AmJPh..79..217D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011AmJPh..79..217D"><span><span class="hlt">Charge</span> sniffer for electrostatics demonstrations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dinca, Mihai P.</p> <p>2011-02-01</p> <p>An electronic electroscope with a special design for demonstrations and experiments on static electricity is described. It operates as an electric <span class="hlt">charge</span> sniffer by detecting slightly <span class="hlt">charged</span> objects when they are brought to the front of its sensing electrode. The sniffer has the advantage of combining high directional sensitivity with a logarithmic bar display. It allows for the identification of electric <span class="hlt">charge</span> polarity during <span class="hlt">charge</span> separation by friction, peeling, electrostatic induction, batteries, or secondary coils of power transformers. Other experiments in electrostatics, such as observing the electric field of an oscillating dipole and the distance dependence of the electric field generated by simple <span class="hlt">charge</span> configurations, are also described.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvP...9d4017R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvP...9d4017R"><span><span class="hlt">Charge</span> Transport in Spiro-OMeTAD Investigated through Space-<span class="hlt">Charge</span>-Limited Current Measurements</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Röhr, Jason A.; Shi, Xingyuan; Haque, Saif A.; Kirchartz, Thomas; Nelson, Jenny</p> <p>2018-04-01</p> <p>Extracting <span class="hlt">charge</span>-carrier mobilities for organic semiconductors from space-<span class="hlt">charge</span>-limited conduction measurements is complicated in practice by nonideal factors such as trapping in defects and injection barriers. Here, we show that by allowing the bandlike <span class="hlt">charge</span>-carrier mobility, trap characteristics, injection barrier heights, and the shunt resistance to vary in a multiple-trapping drift-diffusion model, a numerical fit can be obtained to the entire current density-voltage curve from experimental space-<span class="hlt">charge</span>-limited current measurements on both symmetric and asymmetric 2 ,2',7 ,7' -tetrakis(N ,N -di-4-methoxyphenylamine)-9 ,9' -spirobifluorene (spiro-OMeTAD) single-carrier devices. This approach yields a bandlike mobility that is more than an order of magnitude higher than the effective mobility obtained using analytical approximations, such as the Mott-Gurney law and the moving-electrode equation. It is also shown that where these analytical approximations require a temperature-dependent effective mobility to achieve fits, the numerical model can yield a temperature-, electric-field-, and <span class="hlt">charge</span>-carrier-density-independent mobility. Finally, we present an analytical model describing trap-limited current flow through a semiconductor in a symmetric single-carrier device. We compare the obtained <span class="hlt">charge</span>-carrier mobility and trap characteristics from this analytical model to the results from the numerical model, showing excellent agreement. This work shows the importance of accounting for traps and injection barriers explicitly when analyzing current density-voltage curves from space-<span class="hlt">charge</span>-limited current measurements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22486953','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22486953"><span>Penetration and release studies of positively and negatively <span class="hlt">charged</span> nanoemulsions--is there a benefit of the positive <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>Baspinar, Yücel; Borchert, Hans-Hubert</p> <p>2012-07-01</p> <p>The surface of all tissues, including the stratum corneum, carries a negative <span class="hlt">charge</span>. Following that fact it is assumed that a positively <span class="hlt">charged</span> topical formulation could lead to an enhanced penetration because of an increased interaction with the negative <span class="hlt">charge</span> of the membrane. The intention of this study is to prove an enhanced penetration of a positively <span class="hlt">charged</span> nanoemulsion compared to a negatively <span class="hlt">charged</span> 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 <span class="hlt">charged</span> formulation is higher compared to the positively <span class="hlt">charged</span> nanoemulsion, while the penetration of the positively <span class="hlt">charged</span> nanoemulsion is enhanced compared to the negatively <span class="hlt">charged</span> formulation. The results of the investigated positively <span class="hlt">charged</span> 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 <span class="hlt">charge</span>. Copyright © 2012 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA612156','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA612156"><span>Diplomats in the Foxhole: The Evolution of the State Department During Irregular Conflicts</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2014-05-22</p> <p>transitioning of Iraq,” and the Project and Contracting Office ( PCO ) which was a DOD-led organization <span class="hlt">charged</span> with contract acquisition and project...JUL - DOS S/CRS established • IRMO established • PCO established • SETs introduced • <span class="hlt">APR</span>. Battle of Fallujah • Central Revolutionary</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19800017283','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19800017283"><span>Pulse <span class="hlt">charging</span> of lead-acid traction cells</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Smithrick, J. J.</p> <p>1980-01-01</p> <p>Pulse <span class="hlt">charging</span>, as a method of rapidly and efficiently <span class="hlt">charging</span> 300 amp-hour lead-acid traction cells for an electric vehicle application was investigated. A wide range of <span class="hlt">charge</span> pulse current square waveforms were investigated and the results were compared to constant current <span class="hlt">charging</span> at the time averaged pulse current values. Representative pulse current waveforms were: (1) positive waveform-peak <span class="hlt">charge</span> pulse current of 300 amperes (amps), discharge pulse-current of zero amps, and a duty cycle of about 50%; (2) Romanov waveform-peak <span class="hlt">charge</span> pulse current of 300 amps, peak discharge pulse current of 15 amps, and a duty of 50%; and (3) McCulloch waveform peak <span class="hlt">charge</span> pulse current of 193 amps, peak discharge pulse current of about 575 amps, and a duty cycle of 94%. Experimental results indicate that on the basis of amp-hour efficiency, pulse <span class="hlt">charging</span> offered no significant advantage as a method of rapidly <span class="hlt">charging</span> 300 amp-hour lead-acid traction cells when compared to constant current <span class="hlt">charging</span> at the time average pulse current value. There were, however, some disadvantages of pulse <span class="hlt">charging</span> in particular a decrease in <span class="hlt">charge</span> amp-hour and energy efficiencies and an increase in cell electrolyte temperature. The constant current <span class="hlt">charge</span> method resulted in the best energy efficiency with no significant sacrifice of <span class="hlt">charge</span> time or amp-hour output. Whether or not pulse <span class="hlt">charging</span> offers an advantage over constant current <span class="hlt">charging</span> with regard to the cell <span class="hlt">charge</span>/discharge cycle life is unknown at this time.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19950057055&hterms=grain+dust&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dgrain%2Bdust','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19950057055&hterms=grain+dust&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dgrain%2Bdust"><span><span class="hlt">Charged</span> dust in planetary magnetospheres: Hamiltonian dynamics and numerical simulations for highly <span class="hlt">charged</span> grains</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Schaffer, L.; Burns, J. A.</p> <p>1994-01-01</p> <p>We use a combination of analytical and numerical methods to investigate the dynamics of <span class="hlt">charged</span> dust grains in planetary magnetospheres. Our emphasis is on obtaining results valid for particles that are not necessarily dominated either by gravitational or electromagnetic forces. A Hamiltonian formulation of the problem yields exact results, for all values of <span class="hlt">charge</span>-to-mass ratio, when we introduce two constraints: particles remain in the equatorial plane and the magnetic field is taken as axially symmetric. In particular, we obtain locations of equilibrium points, the frequencies of stable periodic orbits, the topology of separatrices in phase space, and the rate of longitudinal drift. These results are significant for specific applications: motion in the nearly aligned dipolar field of Saturn, and the trajectories of arbitrarily <span class="hlt">charged</span> particles in complex magnetic fields for limited periods of time after ejection from parent bodies. Since the model is restrictive, we also use numerical integrations of the full three-dimensional equations of motion and illustrate under what conditions the constrained problem yields reasonable results. We show that a large fraction of the intermediately <span class="hlt">charged</span> and highly <span class="hlt">charged</span> (gyrating) particles will always be lost to a planet's atmosphere within a few hundred hours, for motion through tilted-dipole magnetic fields. We find that grains must have a very high <span class="hlt">charge</span>-to-mass ratio in order to be mirrored back to the ring plane. Thus, except perhaps at Saturn where the dipole tilt is very small, the likely inhabitants of the dusty ring systems are those particles that are either nearly Keplerian (weakly <span class="hlt">charged</span>) grains or grains whose <span class="hlt">charges</span> place them in the lower end of the intermediate <span class="hlt">charge</span> zone. Fianlly, we demonstrate the effect of plasma drag on the orbits of gyrating particles to be a rapid decrease in gyroradius followed by a slow radial evolution of the guiding center.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20070014070','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20070014070"><span>Spacecraft <span class="hlt">Charging</span> in Low Temperature Environments</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Parker, Linda N.</p> <p>2007-01-01</p> <p>Spacecraft <span class="hlt">charging</span> in plasma and radiation environments is a temperature dependent phenomenon due to the reduction of electrical conductivity in dielectric materials at low temperatures. <span class="hlt">Charging</span> time constants are proportional to l/conductivity may become very large (on the order of days to years) at low temperatures and accumulation of <span class="hlt">charge</span> densities in insulators in <span class="hlt">charging</span> environments traditionally considered benign at ambient temperatures may be sufficient to produce <span class="hlt">charge</span> densities and electric fields of concern in insulators at low temperatures. Low temperature <span class="hlt">charging</span> is of interest because a number of spacecraft-primarily infrared astronomy and microwave cosmology observatories-are currently being design, built, and or operated at very cold temperatures on the order of 40K to 100K. This paper reviews the temperature dependence of spacecraft <span class="hlt">charging</span> processes and material parameters important to <span class="hlt">charging</span> as a function of temperature with an emphasis on low temperatures regimes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19655844','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19655844"><span><span class="hlt">Charge</span> conservation in electronegativity equalization and its implications for the electrostatic properties of fluctuating-<span class="hlt">charge</span> models.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Chen, Jiahao; Martínez, Todd J</p> <p>2009-07-28</p> <p>An analytical solution of fluctuating-<span class="hlt">charge</span> models using Gaussian elimination allows us to isolate the contribution of <span class="hlt">charge</span> conservation effects in determining the <span class="hlt">charge</span> distribution. We use this analytical solution to calculate dipole moments and polarizabilities and show that <span class="hlt">charge</span> conservation plays a critical role in maintaining the correct translational invariance of the electrostatic properties predicted by these models.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20020038756','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20020038756"><span><span class="hlt">Charge</span> Islands Through Tunneling</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Robinson, Daryl C.</p> <p>2002-01-01</p> <p>It has been recently reported that the electrical <span class="hlt">charge</span> in a semiconductive carbon nanotube is not evenly distributed, but rather it is divided into <span class="hlt">charge</span> "islands." This paper links the aforementioned phenomenon to tunneling and provides further insight into the higher rate of tunneling processes, which makes tunneling devices attractive. This paper also provides a basis for calculating the <span class="hlt">charge</span> profile over the length of the tube so that nanoscale devices' conductive properties may be fully exploited.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1078282','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1078282"><span>High dynamic range <span class="hlt">charge</span> measurements</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>De Geronimo, Gianluigi</p> <p>2012-09-04</p> <p>A <span class="hlt">charge</span> amplifier for use in radiation sensing includes an amplifier, at least one switch, and at least one capacitor. The switch selectively couples the input of the switch to one of at least two voltages. The capacitor is electrically coupled in series between the input of the amplifier and the input of the switch. The capacitor is electrically coupled to the input of the amplifier without a switch coupled therebetween. A method of measuring <span class="hlt">charge</span> in radiation sensing includes selectively diverting <span class="hlt">charge</span> from an input of an amplifier to an input of at least one capacitor by selectively coupling an output of the at least one capacitor to one of at least two voltages. The input of the at least one capacitor is operatively coupled to the input of the amplifier without a switch coupled therebetween. The method also includes calculating a total <span class="hlt">charge</span> based on a sum of the amplified <span class="hlt">charge</span> and the diverted <span class="hlt">charge</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title7-vol12/pdf/CFR-2012-title7-vol12-sec1767-23.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title7-vol12/pdf/CFR-2012-title7-vol12-sec1767-23.pdf"><span>7 CFR 1767.23 - Interest <span class="hlt">charges</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-01-01</p> <p>.... Interest <span class="hlt">Charges</span> 427Interest on Long-Term Debt 427.3Interest <span class="hlt">Charged</span> to Construction—Credit 428Amortization... Companies 431Other Interest Expense 432Allowance for Borrowed Funds Used During Construction—Credit Interest....3Interest <span class="hlt">Charged</span> to Construction—Credit This account shall include concurrent credits for interest <span class="hlt">charged</span>...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title7-vol12/pdf/CFR-2010-title7-vol12-sec1767-23.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title7-vol12/pdf/CFR-2010-title7-vol12-sec1767-23.pdf"><span>7 CFR 1767.23 - Interest <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>2010-01-01</p> <p>.... Interest <span class="hlt">Charges</span> 427Interest on Long-Term Debt 427.3Interest <span class="hlt">Charged</span> to Construction—Credit 428Amortization... Companies 431Other Interest Expense 432Allowance for Borrowed Funds Used During Construction—Credit Interest....3Interest <span class="hlt">Charged</span> to Construction—Credit This account shall include concurrent credits for interest <span class="hlt">charged</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.gpo.gov/fdsys/pkg/CFR-2013-title7-vol12/pdf/CFR-2013-title7-vol12-sec1767-23.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title7-vol12/pdf/CFR-2013-title7-vol12-sec1767-23.pdf"><span>7 CFR 1767.23 - Interest <span class="hlt">charges</span>.</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>.... Interest <span class="hlt">Charges</span> 427Interest on Long-Term Debt 427.3Interest <span class="hlt">Charged</span> to Construction—Credit 428Amortization... Companies 431Other Interest Expense 432Allowance for Borrowed Funds Used During Construction—Credit Interest....3Interest <span class="hlt">Charged</span> to Construction—Credit This account shall include concurrent credits for interest <span class="hlt">charged</span>...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010SSRv..157...57D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010SSRv..157...57D"><span><span class="hlt">Charge</span> Transfer Reactions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dennerl, Konrad</p> <p>2010-12-01</p> <p><span class="hlt">Charge</span> transfer, or <span class="hlt">charge</span> exchange, describes a process in which an ion takes one or more electrons from another atom. Investigations of this fundamental process have accompanied atomic physics from its very beginning, and have been extended to astrophysical scenarios already many decades ago. Yet one important aspect of this process, i.e. its high efficiency in generating X-rays, was only revealed in 1996, when comets were discovered as a new class of X-ray sources. This finding has opened up an entirely new field of X-ray studies, with great impact due to the richness of the underlying atomic physics, as the X-rays are not generated by hot electrons, but by ions picking up electrons from cold gas. While comets still represent the best astrophysical laboratory for investigating the physics of <span class="hlt">charge</span> transfer, various studies have already spotted a variety of other astrophysical locations, within and beyond our solar system, where X-rays may be generated by this process. They range from planetary atmospheres, the heliosphere, the interstellar medium and stars to galaxies and clusters of galaxies, where <span class="hlt">charge</span> transfer may even be observationally linked to dark matter. This review attempts to put the various aspects of the study of <span class="hlt">charge</span> transfer reactions into a broader historical context, with special emphasis on X-ray astrophysics, where the discovery of cometary X-ray emission may have stimulated a novel look at our universe.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/4206675','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/biblio/4206675"><span><span class="hlt">CHARGE</span> BOTTLE FOR A MASS SEPARATOR</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Davidson, P.H.</p> <p>1959-07-01</p> <p>Improved mass separator <span class="hlt">charge</span> bottles are described for containing a dense <span class="hlt">charge</span> of a chemical compound of copper, nickel, lead or other useful substance which is to be vaporized, and to the method of utilizing such improvcd <span class="hlt">charge</span> bottles so that the chemical compound is vaporized from the under surface of the <span class="hlt">charge</span> and thus permits the non-volatile portion thereof to fall to the bottom of the <span class="hlt">charge</span> bottle where it does not form an obstacle to further evaporation. The <span class="hlt">charge</span> bottle comprises a vertically disposed cylindrical portion, an inner re-entrant cylindrical portion extending axially and downwardly into the same from the upper end thereof, and evaporative source material in the form of a chemical compound compacted within the upper annular pontion of the <span class="hlt">charge</span> bottle formed by the re-entrant cylindrical portion, whereby vapor from the chemical compound will pass outwardly from the <span class="hlt">charge</span> bottle through an apertured closure.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADP011087','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADP011087"><span>Respiratory Changes and Consequences for Treatment of Decompression Bubbles Following Severe Decompression Accidents</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2001-06-01</p> <p>conditions hypobares ou hyperbares ] To order the complete compilation report, use: ADA395680 The component part is provided here to allow users access to...the following report: TITLE: Operational Medical Issues in Hypo-and Hyperbaric Conditions [les Questions <span class="hlt">medicales</span> a caractere oprationel liees aux...anaesthetised animals subjected to controlled primary and treatment hyperbaric procedures; the range of bubble counts was from zero to fatal. Treatment</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADP011064','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADP011064"><span>Pharmacological Correction of the Human Functional State in High Altitude Conditions</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2001-06-01</p> <p>Operational Medical Issues in Hypo-and Hyperbaric Conditions [les Questions <span class="hlt">medicales</span> a caractere oprationel liees aux conditions hypobares ou hyperbares ...Cholesterol, Adaptation Paper presented at the RTO HFM Symposium on "Operational Medical Issues in Hypo- and Hyperbaric Conditions", held in Toronto...T.D., 1986, Recovery after Extreme Hypobaric Hypoxia as a Method of Study of Antihypoxic Activity of Chemical Compounds. In: Farmakologicheskaya</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADP011077','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADP011077"><span>Severe Decompression Illness Following Simulated Rescue from a Pressurized Distressed Submarine</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2001-06-01</p> <p>TITLE: Operational Medical Issues in Hypo-and Hyperbaric Conditions [les Questions <span class="hlt">medicales</span> a caractere oprationel liees aux conditions hypobares ou... hyperbares ] To order the complete compilation report, use: ADA395680 The component part is provided here to allow users access to individually authored...upon the relationship between pressure exposure and risk of a bad outcome, which needs to be elucidated. Additionally, any non- hyperbaric methods of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADP011084','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADP011084"><span>Incidence of Decompression Illness and Other Diving Related Medical Problems Amongst Royal Navy Divers 1995-1999</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>1999-01-01</p> <p>conditions hypobares ou hyperbares ] To order the complete compilation report, use: ADA395680 The component part is provided here to allow users access to...following report: TITLE: Operational Medical Issues in Hypo-and Hyperbaric Conditions [les Questions <span class="hlt">medicales</span> a caractere oprationel liees aux...Navy diving accidents, and with the assistance of the British Hyperbaric Association (BHA) all civilian cases of decompression illness treated by member</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JHEP...05..050R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JHEP...05..050R"><span>Abelian F-theory models with <span class="hlt">charge</span>-3 and <span class="hlt">charge</span>-4 matter</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Raghuram, Nikhil</p> <p>2018-05-01</p> <p>This paper analyzes U(1) F-theory models admitting matter with <span class="hlt">charges</span> q = 3 and 4. First, we systematically derive a q = 3 construction that generalizes the previous q = 3 examples. We argue that U(1) symmetries can be tuned through a procedure reminiscent of the SU( N ) and Sp( N ) tuning process. For models with q = 3 matter, the components of the generating section vanish to orders higher than 1 at the <span class="hlt">charge</span>-3 matter loci. As a result, the Weierstrass models can contain non-UFD structure and thereby deviate from the standard Morrison-Park form. Techniques used to tune SU( N ) models on singular divisors allow us to determine the non-UFD structures and derive the q = 3 tuning from scratch. We also obtain a class of a q=4 models by deforming a prior U(1) × U(1) construction. To the author's knowledge, this is the first published F-theory example with <span class="hlt">charge</span>-4 matter. Finally, we discuss some conjectures regarding models with <span class="hlt">charges</span> larger than 4.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title40-vol33/pdf/CFR-2011-title40-vol33-sec1515-14.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title40-vol33/pdf/CFR-2011-title40-vol33-sec1515-14.pdf"><span>40 CFR 1515.14 - Other <span class="hlt">charges</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-07-01</p> <p>... 40 Protection of Environment 33 2011-07-01 2011-07-01 false Other <span class="hlt">charges</span>. 1515.14 Section 1515.14 Protection of Environment COUNCIL ON ENVIRONMENTAL QUALITY FREEDOM OF INFORMATION ACT PROCEDURES Costs § 1515.14 Other <span class="hlt">charges</span>. CEQ may apply other <span class="hlt">charges</span>, including the following: (a) Special <span class="hlt">charges</span>. CEQ...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title40-vol34/pdf/CFR-2013-title40-vol34-sec1515-14.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title40-vol34/pdf/CFR-2013-title40-vol34-sec1515-14.pdf"><span>40 CFR 1515.14 - Other <span class="hlt">charges</span>.</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>2013-07-01</p> <p>... 40 Protection of Environment 34 2013-07-01 2013-07-01 false Other <span class="hlt">charges</span>. 1515.14 Section 1515.14 Protection of Environment COUNCIL ON ENVIRONMENTAL QUALITY FREEDOM OF INFORMATION ACT PROCEDURES Costs § 1515.14 Other <span class="hlt">charges</span>. CEQ may apply other <span class="hlt">charges</span>, including the following: (a) Special <span class="hlt">charges</span>. CEQ...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title40-vol33/pdf/CFR-2014-title40-vol33-sec1515-14.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title40-vol33/pdf/CFR-2014-title40-vol33-sec1515-14.pdf"><span>40 CFR 1515.14 - Other <span class="hlt">charges</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-07-01</p> <p>... 40 Protection of Environment 33 2014-07-01 2014-07-01 false Other <span class="hlt">charges</span>. 1515.14 Section 1515.14 Protection of Environment COUNCIL ON ENVIRONMENTAL QUALITY FREEDOM OF INFORMATION ACT PROCEDURES Costs § 1515.14 Other <span class="hlt">charges</span>. CEQ may apply other <span class="hlt">charges</span>, including the following: (a) Special <span class="hlt">charges</span>. CEQ...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title40-vol34/pdf/CFR-2012-title40-vol34-sec1515-14.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title40-vol34/pdf/CFR-2012-title40-vol34-sec1515-14.pdf"><span>40 CFR 1515.14 - Other <span class="hlt">charges</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-07-01</p> <p>... 40 Protection of Environment 34 2012-07-01 2012-07-01 false Other <span class="hlt">charges</span>. 1515.14 Section 1515.14 Protection of Environment COUNCIL ON ENVIRONMENTAL QUALITY FREEDOM OF INFORMATION ACT PROCEDURES Costs § 1515.14 Other <span class="hlt">charges</span>. CEQ may apply other <span class="hlt">charges</span>, including the following: (a) Special <span class="hlt">charges</span>. CEQ...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016APS..MARA33006R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016APS..MARA33006R"><span>Effect of <span class="hlt">Charge</span> Patterning on the Phase Behavior of Polymer Coacervates for <span class="hlt">Charge</span> Driven Self Assembly</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Radhakrishna, Mithun; Sing, Charles E.</p> <p></p> <p>Oppositely <span class="hlt">charged</span> polymers can undergo associative liquid-liquid phase separation when mixed under suitable conditions of ionic strength, temperature and pH to form what are known as `polymeric complex coacervates'. Polymer coacervates find use in diverse array of applications like microencapsulation, drug delivery, membrane filtration and underwater adhesives. The similarity between complex coacervate environments and those in biological systems has also found relevance in areas of bio-mimicry. Our previous works have demonstrated how local <span class="hlt">charge</span> correlations and molecular connectivity can drastically affect the phase behavior of coacervates. The precise location of <span class="hlt">charges</span> along the chain therefore dramatically influences the local <span class="hlt">charge</span> correlations, which consequently influences the phase behavior of coacervates. We investigate the effect of <span class="hlt">charge</span> patterning along the polymer chain on the phase behavior of coacervates in the framework of the Restricted Primitive Model using Gibbs Ensemble Monte Carlo simulations. Our results show that <span class="hlt">charge</span> patterning dramatically changes the phase behavior of polymer coacervates, which contrasts with the predictions of the classical Voorn-Overbeek theory. This provides the basis for designing new materials through <span class="hlt">charge</span> driven self assembly by controlling the positioning of the <span class="hlt">charged</span> monomers along the chain.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title44-vol1/pdf/CFR-2013-title44-vol1-sec6-83.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title44-vol1/pdf/CFR-2013-title44-vol1-sec6-83.pdf"><span>44 CFR 6.83 - Prepayment of fees.</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>2013-10-01</p> <p>... (a) or (b). [52 FR 13679, <span class="hlt">Apr</span>. 24, 1987] ... before continuing to process the request. (b) When a requester has previously failed to pay a fee <span class="hlt">charged</span>... or a pending request from that requester. (c) When FEMA acts under § 5.44 (a) or (b), the...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title44-vol1/pdf/CFR-2012-title44-vol1-sec6-83.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title44-vol1/pdf/CFR-2012-title44-vol1-sec6-83.pdf"><span>44 CFR 6.83 - Prepayment of fees.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-10-01</p> <p>... (a) or (b). [52 FR 13679, <span class="hlt">Apr</span>. 24, 1987] ... before continuing to process the request. (b) When a requester has previously failed to pay a fee <span class="hlt">charged</span>... or a pending request from that requester. (c) When FEMA acts under § 5.44 (a) or (b), the...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title44-vol1/pdf/CFR-2014-title44-vol1-sec6-83.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title44-vol1/pdf/CFR-2014-title44-vol1-sec6-83.pdf"><span>44 CFR 6.83 - Prepayment of fees.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-10-01</p> <p>... (a) or (b). [52 FR 13679, <span class="hlt">Apr</span>. 24, 1987] ... before continuing to process the request. (b) When a requester has previously failed to pay a fee <span class="hlt">charged</span>... or a pending request from that requester. (c) When FEMA acts under § 5.44 (a) or (b), the...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title44-vol1/pdf/CFR-2010-title44-vol1-sec6-83.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title44-vol1/pdf/CFR-2010-title44-vol1-sec6-83.pdf"><span>44 CFR 6.83 - Prepayment of fees.</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>... (a) or (b). [52 FR 13679, <span class="hlt">Apr</span>. 24, 1987] ... before continuing to process the request. (b) When a requester has previously failed to pay a fee <span class="hlt">charged</span>... or a pending request from that requester. (c) When FEMA acts under § 5.44 (a) or (b), the...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title44-vol1/pdf/CFR-2011-title44-vol1-sec6-83.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title44-vol1/pdf/CFR-2011-title44-vol1-sec6-83.pdf"><span>44 CFR 6.83 - Prepayment of fees.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-10-01</p> <p>... (a) or (b). [52 FR 13679, <span class="hlt">Apr</span>. 24, 1987] ... before continuing to process the request. (b) When a requester has previously failed to pay a fee <span class="hlt">charged</span>... or a pending request from that requester. (c) When FEMA acts under § 5.44 (a) or (b), the...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title12-vol1/pdf/CFR-2010-title12-vol1-sec7-4001.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title12-vol1/pdf/CFR-2010-title12-vol1-sec7-4001.pdf"><span>12 CFR 7.4001 - <span class="hlt">Charging</span> interest at rates permitted competing institutions; <span class="hlt">charging</span> interest to corporate...</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>... 12 Banks and Banking 1 2010-01-01 2010-01-01 false <span class="hlt">Charging</span> interest at rates permitted competing... interest at rates permitted competing institutions; <span class="hlt">charging</span> interest to corporate borrowers. (a... <span class="hlt">charge</span> interest at the maximum rate permitted to any state-chartered or licensed lending institution by...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title31-vol2/pdf/CFR-2011-title31-vol2-sec206-9.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title31-vol2/pdf/CFR-2011-title31-vol2-sec206-9.pdf"><span>31 CFR 206.9 - <span class="hlt">Charges</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-07-01</p> <p>... OF THE CASH MANAGEMENT IMPROVEMENTS FUND § 206.9 <span class="hlt">Charges</span>. (a) Within 30 days of the effective date of... noncompliance. In the case of cash management collection noncompliance, an agency will absorb the <span class="hlt">charge</span> from.... <span class="hlt">Charges</span> collected from an executive agency in the case of cash management collection noncompliance will be...</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('http://adsabs.harvard.edu/abs/2015JPS...273..413V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015JPS...273..413V"><span>New <span class="hlt">charging</span> strategy for lithium-ion batteries based on the integration of Taguchi method and state of <span class="hlt">charge</span> estimation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vo, Thanh Tu; Chen, Xiaopeng; Shen, Weixiang; Kapoor, Ajay</p> <p>2015-01-01</p> <p>In this paper, a new <span class="hlt">charging</span> strategy of lithium-polymer batteries (LiPBs) has been proposed based on the integration of Taguchi method (TM) and state of <span class="hlt">charge</span> estimation. The TM is applied to search an optimal <span class="hlt">charging</span> current pattern. An adaptive switching gain sliding mode observer (ASGSMO) is adopted to estimate the SOC which controls and terminates the <span class="hlt">charging</span> process. The experimental results demonstrate that the proposed <span class="hlt">charging</span> strategy can successfully <span class="hlt">charge</span> the same types of LiPBs with different capacities and cycle life. The proposed <span class="hlt">charging</span> strategy also provides much shorter <span class="hlt">charging</span> time, narrower temperature variation and slightly higher energy efficiency than the equivalent constant current constant voltage <span class="hlt">charging</span> method.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26510600','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26510600"><span>[Probabilistic calculations of biomolecule <span class="hlt">charge</span> states that generate mass spectra of multiply <span class="hlt">charged</span> ions].</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Raznikova, M O; Raznikov, V V</p> <p>2015-01-01</p> <p>In this work, information relating to <span class="hlt">charge</span> states of biomolecule ions in solution obtained using the electrospray ionization mass spectrometry of different biopolymers is analyzed. The data analyses have mainly been carried out by solving an inverse problem of calculating the probabilities of retention of protons and other <span class="hlt">charge</span> carriers by ionogenic groups of biomolecules with known primary structures. The approach is a new one and has no known to us analogues. A program titled "Decomposition" was developed and used to analyze the <span class="hlt">charge</span> distribution of ions of native and denatured cytochrome c mass spectra. The possibility of splitting of the <span class="hlt">charge</span>-state distribution of albumin into normal components, which likely corresponds to various conformational states of the biomolecule, has been demonstrated. The applicability criterion for using previously described method of decomposition of multidimensional <span class="hlt">charge</span>-state distributions with two <span class="hlt">charge</span> carriers, e.g., a proton and a sodium ion, to characterize the spatial structure of biopolymers in solution has been formulated. In contrast to known mass-spectrometric approaches, this method does not require the use of enzymatic hydrolysis or collision-induced dissociation of the biopolymers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013JHEP...12..059B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013JHEP...12..059B"><span>Holographic <span class="hlt">charged</span> Rényi entropies</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Belin, Alexandre; Hung, Ling-Yan; Maloney, Alexander; Matsuura, Shunji; Myers, Robert C.; Sierens, Todd</p> <p>2013-12-01</p> <p>We construct a new class of entanglement measures by extending the usual definition of Rényi entropy to include a chemical potential. These <span class="hlt">charged</span> Rényi entropies measure the degree of entanglement in different <span class="hlt">charge</span> sectors of the theory and are given by Euclidean path integrals with the insertion of a Wilson line encircling the entangling surface. We compute these entropies for a spherical entangling surface in CFT's with holographic duals, where they are related to entropies of <span class="hlt">charged</span> black holes with hyperbolic horizons. We also compute <span class="hlt">charged</span> Rényi entropies in free field theories.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title10-vol4/pdf/CFR-2013-title10-vol4-sec904-7.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title10-vol4/pdf/CFR-2013-title10-vol4-sec904-7.pdf"><span>10 CFR 904.7 - Base <span class="hlt">charge</span>.</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>... 10 Energy 4 2013-01-01 2013-01-01 false Base <span class="hlt">charge</span>. 904.7 Section 904.7 Energy DEPARTMENT OF... Marketing § 904.7 Base <span class="hlt">charge</span>. (a) The Base <span class="hlt">Charge</span> shall be developed by the Administrator and promulgated in accordance with appropriate DOE regulations. The Base <span class="hlt">Charge</span> shall be composed of a capacity...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title10-vol4/pdf/CFR-2011-title10-vol4-sec904-7.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title10-vol4/pdf/CFR-2011-title10-vol4-sec904-7.pdf"><span>10 CFR 904.7 - Base <span class="hlt">charge</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-01-01</p> <p>... 10 Energy 4 2011-01-01 2011-01-01 false Base <span class="hlt">charge</span>. 904.7 Section 904.7 Energy DEPARTMENT OF... Marketing § 904.7 Base <span class="hlt">charge</span>. (a) The Base <span class="hlt">Charge</span> shall be developed by the Administrator and promulgated in accordance with appropriate DOE regulations. The Base <span class="hlt">Charge</span> shall be composed of a capacity...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title10-vol4/pdf/CFR-2012-title10-vol4-sec904-7.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title10-vol4/pdf/CFR-2012-title10-vol4-sec904-7.pdf"><span>10 CFR 904.7 - Base <span class="hlt">charge</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-01-01</p> <p>... 10 Energy 4 2012-01-01 2012-01-01 false Base <span class="hlt">charge</span>. 904.7 Section 904.7 Energy DEPARTMENT OF... Marketing § 904.7 Base <span class="hlt">charge</span>. (a) The Base <span class="hlt">Charge</span> shall be developed by the Administrator and promulgated in accordance with appropriate DOE regulations. The Base <span class="hlt">Charge</span> shall be composed of a capacity...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title10-vol4/pdf/CFR-2010-title10-vol4-sec904-7.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title10-vol4/pdf/CFR-2010-title10-vol4-sec904-7.pdf"><span>10 CFR 904.7 - Base <span class="hlt">charge</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>2010-01-01</p> <p>... 10 Energy 4 2010-01-01 2010-01-01 false Base <span class="hlt">charge</span>. 904.7 Section 904.7 Energy DEPARTMENT OF... Marketing § 904.7 Base <span class="hlt">charge</span>. (a) The Base <span class="hlt">Charge</span> shall be developed by the Administrator and promulgated in accordance with appropriate DOE regulations. The Base <span class="hlt">Charge</span> shall be composed of a capacity...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=goods+AND+service+AND+tax&pg=6&id=EJ196524','ERIC'); return false;" href="https://eric.ed.gov/?q=goods+AND+service+AND+tax&pg=6&id=EJ196524"><span><span class="hlt">Charging</span> Users for Library Service.</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>Cooper, Michael D.</p> <p>1978-01-01</p> <p>Examines the question of instituting direct <span class="hlt">charges</span> for library service, using on-line bibliographic searching as an example, and contrasts this with the current indirect <span class="hlt">charging</span> system where services are paid for by taxes. Information, as a merit good, should be supplied with or without direct <span class="hlt">charges</span>, depending upon user status. (CWM)</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013JChPh.139d4110M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013JChPh.139d4110M"><span>Coupled electron-nuclear dynamics: <span class="hlt">Charge</span> migration and <span class="hlt">charge</span> transfer initiated near a conical intersection</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mendive-Tapia, David; Vacher, Morgane; Bearpark, Michael J.; Robb, Michael A.</p> <p>2013-07-01</p> <p>Coupled electron-nuclear dynamics, implemented using the Ehrenfest method, has been used to study <span class="hlt">charge</span> migration with fixed nuclei, together with <span class="hlt">charge</span> transfer when nuclei are allowed to move. Simulations were initiated at reference geometries of neutral benzene and 2-phenylethylamine (PEA), and at geometries close to potential energy surface crossings in the cations. Cationic eigenstates, and the so-called sudden approximation, involving removal of an electron from a correlated ground-state wavefunction for the neutral species, were used as initial conditions. <span class="hlt">Charge</span> migration without coupled nuclear motion could be observed if the Ehrenfest simulation, using the sudden approximation, was started near a conical intersection where the states were both strongly coupled and quasi-degenerate. Further, the main features associated with <span class="hlt">charge</span> migration were still recognizable when the nuclear motion was allowed to couple. In the benzene radical cation, starting from the reference neutral geometry with the sudden approximation, one could observe sub-femtosecond <span class="hlt">charge</span> migration with a small amplitude, which results from weak interaction with higher electronic states. However, we were able to engineer large amplitude <span class="hlt">charge</span> migration, with a period between 10 and 100 fs, corresponding to oscillation of the electronic structure between the quinoid and anti-quinoid cationic electronic configurations, by distorting the geometry along the derivative coupling vector from the D6h Jahn-Teller crossing to lower symmetry where the states are not degenerate. When the nuclear motion becomes coupled, the period changes only slightly. In PEA, in an Ehrenfest trajectory starting from the D2 eigenstate and reference geometry, a partial <span class="hlt">charge</span> transfer occurs after about 12 fs near the first crossing between D1, D2 (N+-Phenyl, N-Phenyl+). If the Ehrenfest propagation is started near this point, using the sudden approximation without coupled nuclear motion, one observes an</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 additions 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.gpo.gov/fdsys/pkg/CFR-2010-title30-vol1/pdf/CFR-2010-title30-vol1-sec56-4502.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title30-vol1/pdf/CFR-2010-title30-vol1-sec56-4502.pdf"><span>30 CFR 56.4502 - Battery-<span class="hlt">charging</span> stations.</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>2010-07-01</p> <p>... 30 Mineral Resources 1 2010-07-01 2010-07-01 false Battery-<span class="hlt">charging</span> stations. 56.4502 Section 56... Control Installation/construction/maintenance § 56.4502 Battery-<span class="hlt">charging</span> stations. (a) Battery-<span class="hlt">charging</span>... prohibited at the battery <span class="hlt">charging</span> station during battery <span class="hlt">charging</span>. (c) Readily visible signs prohibiting...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title30-vol1/pdf/CFR-2014-title30-vol1-sec56-4502.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title30-vol1/pdf/CFR-2014-title30-vol1-sec56-4502.pdf"><span>30 CFR 56.4502 - Battery-<span class="hlt">charging</span> stations.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-07-01</p> <p>... 30 Mineral Resources 1 2014-07-01 2014-07-01 false Battery-<span class="hlt">charging</span> stations. 56.4502 Section 56... Control Installation/construction/maintenance § 56.4502 Battery-<span class="hlt">charging</span> stations. (a) Battery-<span class="hlt">charging</span>... prohibited at the battery <span class="hlt">charging</span> station during battery <span class="hlt">charging</span>. (c) Readily visible signs prohibiting...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title30-vol1/pdf/CFR-2012-title30-vol1-sec56-4502.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title30-vol1/pdf/CFR-2012-title30-vol1-sec56-4502.pdf"><span>30 CFR 56.4502 - Battery-<span class="hlt">charging</span> stations.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-07-01</p> <p>... 30 Mineral Resources 1 2012-07-01 2012-07-01 false Battery-<span class="hlt">charging</span> stations. 56.4502 Section 56... Control Installation/construction/maintenance § 56.4502 Battery-<span class="hlt">charging</span> stations. (a) Battery-<span class="hlt">charging</span>... prohibited at the battery <span class="hlt">charging</span> station during battery <span class="hlt">charging</span>. (c) Readily visible signs prohibiting...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title30-vol1/pdf/CFR-2013-title30-vol1-sec56-4502.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title30-vol1/pdf/CFR-2013-title30-vol1-sec56-4502.pdf"><span>30 CFR 56.4502 - Battery-<span class="hlt">charging</span> stations.</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>2013-07-01</p> <p>... 30 Mineral Resources 1 2013-07-01 2013-07-01 false Battery-<span class="hlt">charging</span> stations. 56.4502 Section 56... Control Installation/construction/maintenance § 56.4502 Battery-<span class="hlt">charging</span> stations. (a) Battery-<span class="hlt">charging</span>... prohibited at the battery <span class="hlt">charging</span> station during battery <span class="hlt">charging</span>. (c) Readily visible signs prohibiting...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title30-vol1/pdf/CFR-2011-title30-vol1-sec56-4502.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title30-vol1/pdf/CFR-2011-title30-vol1-sec56-4502.pdf"><span>30 CFR 56.4502 - Battery-<span class="hlt">charging</span> stations.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-07-01</p> <p>... 30 Mineral Resources 1 2011-07-01 2011-07-01 false Battery-<span class="hlt">charging</span> stations. 56.4502 Section 56... Control Installation/construction/maintenance § 56.4502 Battery-<span class="hlt">charging</span> stations. (a) Battery-<span class="hlt">charging</span>... prohibited at the battery <span class="hlt">charging</span> station during battery <span class="hlt">charging</span>. (c) Readily visible signs prohibiting...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title12-vol1/pdf/CFR-2011-title12-vol1-sec7-4001.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title12-vol1/pdf/CFR-2011-title12-vol1-sec7-4001.pdf"><span>12 CFR 7.4001 - <span class="hlt">Charging</span> interest at rates permitted competing institutions; <span class="hlt">charging</span> interest to corporate...</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-01-01</p> <p>... bank may lawfully <span class="hlt">charge</span> the highest rate permitted to be <span class="hlt">charged</span> by a state-licensed small loan... small loan companies. (c) Effect on state definitions of interest. The Federal definition of the term... the law of that state. If state law permits different interest <span class="hlt">charges</span> on specified classes of loans...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title12-vol1/pdf/CFR-2014-title12-vol1-sec7-4001.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title12-vol1/pdf/CFR-2014-title12-vol1-sec7-4001.pdf"><span>12 CFR 7.4001 - <span class="hlt">Charging</span> interest at rates permitted competing institutions; <span class="hlt">charging</span> interest to corporate...</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-01-01</p> <p>... bank may lawfully <span class="hlt">charge</span> the highest rate permitted to be <span class="hlt">charged</span> by a state-licensed small loan... small loan companies. (c) Effect on state definitions of interest. The Federal definition of the term... the law of that state. If state law permits different interest <span class="hlt">charges</span> on specified classes of loans...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title12-vol1/pdf/CFR-2013-title12-vol1-sec7-4001.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title12-vol1/pdf/CFR-2013-title12-vol1-sec7-4001.pdf"><span>12 CFR 7.4001 - <span class="hlt">Charging</span> interest at rates permitted competing institutions; <span class="hlt">charging</span> interest to corporate...</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>... bank may lawfully <span class="hlt">charge</span> the highest rate permitted to be <span class="hlt">charged</span> by a state-licensed small loan... small loan companies. (c) Effect on state definitions of interest. The Federal definition of the term... the law of that state. If state law permits different interest <span class="hlt">charges</span> on specified classes of loans...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title12-vol1/pdf/CFR-2012-title12-vol1-sec7-4001.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title12-vol1/pdf/CFR-2012-title12-vol1-sec7-4001.pdf"><span>12 CFR 7.4001 - <span class="hlt">Charging</span> interest at rates permitted competing institutions; <span class="hlt">charging</span> interest to corporate...</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-01-01</p> <p>... bank may lawfully <span class="hlt">charge</span> the highest rate permitted to be <span class="hlt">charged</span> by a state-licensed small loan... small loan companies. (c) Effect on state definitions of interest. The Federal definition of the term... the law of that state. If state law permits different interest <span class="hlt">charges</span> on specified classes of loans...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016PhRvC..94f4315B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016PhRvC..94f4315B"><span>Predictions of nuclear <span class="hlt">charge</span> radii</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bao, M.; Lu, Y.; Zhao, Y. M.; Arima, A.</p> <p>2016-12-01</p> <p>The nuclear <span class="hlt">charge</span> radius is a fundamental property of an atomic nucleus. In this article we study the predictive power of empirical relations for experimental nuclear <span class="hlt">charge</span> radii of neighboring nuclei and predict the unknown <span class="hlt">charge</span> radii of 1085 nuclei based on the experimental CR2013 database within an uncertainty of 0.03 fm.</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('https://www.osti.gov/biblio/22415881-complexation-behavior-oppositely-charged-polyelectrolytes-effect-charge-distribution','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22415881-complexation-behavior-oppositely-charged-polyelectrolytes-effect-charge-distribution"><span>Complexation behavior of oppositely <span class="hlt">charged</span> polyelectrolytes: Effect of <span class="hlt">charge</span> distribution</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>Zhao, Mingtian; Li, Baohui, E-mail: dliang@pku.edu.cn, E-mail: baohui@nankai.edu.cn; Zhou, Jihan</p> <p></p> <p>Complexation behavior of oppositely <span class="hlt">charged</span> polyelectrolytes in a solution is investigated using a combination of computer simulations and experiments, focusing on the influence of polyelectrolyte <span class="hlt">charge</span> distributions along the chains on the structure of the polyelectrolyte complexes. The simulations are performed using Monte Carlo with the replica-exchange algorithm for three model systems where each system is composed of a mixture of two types of oppositely <span class="hlt">charged</span> model polyelectrolyte chains (EGEG){sub 5}/(KGKG){sub 5}, (EEGG){sub 5}/(KKGG){sub 5}, and (EEGG){sub 5}/(KGKG){sub 5}, in a solution including explicit solvent molecules. Among the three model systems, only the <span class="hlt">charge</span> distributions along the chains are notmore » identical. Thermodynamic quantities are calculated as a function of temperature (or ionic strength), and the microscopic structures of complexes are examined. It is found that the three systems have different transition temperatures, and form complexes with different sizes, structures, and densities at a given temperature. Complex microscopic structures with an alternating arrangement of one monolayer of E/K monomers and one monolayer of G monomers, with one bilayer of E and K monomers and one bilayer of G monomers, and with a mixture of monolayer and bilayer of E/K monomers in a box shape and a trilayer of G monomers inside the box are obtained for the three mixture systems, respectively. The experiments are carried out for three systems where each is composed of a mixture of two types of oppositely <span class="hlt">charged</span> peptide chains. Each peptide chain is composed of Lysine (K) and glycine (G) or glutamate (E) and G, in solution, and the chain length and amino acid sequences, and hence the <span class="hlt">charge</span> distribution, are precisely controlled, and all of them are identical with those for the corresponding model chain. The complexation behavior and complex structures are characterized through laser light scattering and atomic force microscopy measurements. The</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20130014143','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20130014143"><span>Battery <span class="hlt">Charge</span> Equalizer with Transformer Array</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Davies, Francis</p> <p>2013-01-01</p> <p>High-power batteries generally consist of a series connection of many cells or cell banks. In order to maintain high performance over battery life, it is desirable to keep the state of <span class="hlt">charge</span> of all the cell banks equal. A method provides individual <span class="hlt">charging</span> for battery cells in a large, high-voltage battery array with a minimum number of transformers while maintaining reasonable efficiency. This is designed to augment a simple highcurrent charger that supplies the main <span class="hlt">charge</span> energy. The innovation will form part of a larger battery <span class="hlt">charge</span> system. It consists of a transformer array connected to the battery array through rectification and filtering circuits. The transformer array is connected to a drive circuit and a timing and control circuit that allow individual battery cells or cell banks to be <span class="hlt">charged</span>. The timing circuit and control circuit connect to a <span class="hlt">charge</span> controller that uses battery instrumentation to determine which battery bank to <span class="hlt">charge</span>. It is important to note that the innovation can <span class="hlt">charge</span> an individual cell bank at the same time that the main battery charger is <span class="hlt">charging</span> the high-voltage battery. The fact that the battery cell banks are at a non-zero voltage, and that they are all at similar voltages, can be used to allow <span class="hlt">charging</span> of individual cell banks. A set of transformers can be connected with secondary windings in series to make weighted sums of the voltages on the primaries.</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 addition, 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 additional 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://www.osti.gov/servlets/purl/1174352','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1174352"><span><span class="hlt">Charge</span> exchange molecular ion source</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Vella, Michael C.</p> <p>2003-06-03</p> <p>Ions, particularly molecular ions with multiple dopant nucleons per ion, are produced by <span class="hlt">charge</span> exchange. An ion source contains a minimum of two regions separated by a physical barrier and utilizes <span class="hlt">charge</span> exchange to enhance production of a desired ion species. The essential elements are a plasma chamber for production of ions of a first species, a physical separator, and a <span class="hlt">charge</span> transfer chamber where ions of the first species from the plasma chamber undergo <span class="hlt">charge</span> exchange or transfer with the reactant atom or molecules to produce ions of a second species. Molecular ions may be produced which are useful for ion implantation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23898800','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23898800"><span>Electrophoresis of a <span class="hlt">charged</span> soft particle in a <span class="hlt">charged</span> cavity with arbitrary double-layer thickness.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Chen, Wei J; Keh, Huan J</p> <p>2013-08-22</p> <p>An analysis for the quasi-steady electrophoretic motion of a soft particle composed of a <span class="hlt">charged</span> spherical rigid core and an adsorbed porous layer positioned at the center of a <span class="hlt">charged</span> spherical cavity filled with an arbitrary electrolyte solution is presented. Within the porous layer, frictional segments with fixed <span class="hlt">charges</span> are assumed to distribute uniformly. Through the use of the linearized Poisson-Boltzmann equation and the Laplace equation, the equilibrium double-layer potential distribution and its perturbation caused by the applied electric field are separately determined. The modified Stokes and Brinkman equations governing the fluid flow fields outside and inside the porous layer, respectively, are solved subsequently. An explicit formula for the electrokinetic migration velocity of the soft particle in terms of the fixed <span class="hlt">charge</span> densities on the rigid core surface, in the porous layer, and on the cavity wall is obtained from a balance between its electrostatic and hydrodynamic forces. This formula is valid for arbitrary values of κa, λa, r0/a, and a/b, where κ is the Debye screening parameter, λ is the reciprocal of the length characterizing the extent of flow penetration inside the porous layer, a is the radius of the soft particle, r0 is the radius of the rigid core of the particle, and b is the radius of the cavity. In the limiting cases of r0 = a and r0 = 0, the migration velocity for the <span class="hlt">charged</span> soft sphere reduces to that for a <span class="hlt">charged</span> impermeable sphere and that for a <span class="hlt">charged</span> porous sphere, respectively, in the <span class="hlt">charged</span> cavity. The effect of the surface <span class="hlt">charge</span> at the cavity wall on the particle migration can be significant, and the particle may reverse the direction of its migration.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMAE33B0442B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMAE33B0442B"><span>Thunderstorm <span class="hlt">Charge</span> Structures Producing Negative Gigantic Jets</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Boggs, L.; Liu, N.; Riousset, J. A.; Shi, F.; Rassoul, H.</p> <p>2016-12-01</p> <p>Here we present observational and modeling results that provide insight into thunderstorm <span class="hlt">charge</span> 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, <span class="hlt">charge</span> structures, and lightning activity when the gigantic jets emerged from the parent thunderstorms. A detailed investigation of the evolution of one of the <span class="hlt">charge</span> structures by analyzing the VHF data is also presented. The newly found <span class="hlt">charge</span> 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 <span class="hlt">charge</span> structures feature a narrow upper positive <span class="hlt">charge</span> region over a wide middle negative <span class="hlt">charge</span> region. There also likely exists a `ring' of negative screening <span class="hlt">charge</span> located around the perimeter of the upper positive <span class="hlt">charge</span>. This is different from previously thought <span class="hlt">charge</span> structures of the storms producing gigantic jets, which had a very wide upper positive <span class="hlt">charge</span> region over a wide middle negative <span class="hlt">charge</span> region, with a very small negative screening layer covering the cloud top. The newly found <span class="hlt">charge</span> 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 <span class="hlt">charge</span> structures, while vital to the understanding of gigantic jet initiation and the role of <span class="hlt">charge</span> imbalances inside the cloud, do not produce leader discharge trees that agree with observed gigantic jet discharges.Finally, the newly discovered gigantic jet <span class="hlt">charge</span> structures are formed near the end of a convective pulse [Meyer et al., JGR, 118</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013ISPAr.XL4a..77E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013ISPAr.XL4a..77E"><span>a Movable <span class="hlt">Charging</span> Unit for Green Mobility</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>ElBanhawy, E. Y.; Nassar, K.</p> <p>2013-05-01</p> <p>Battery swapping of electric vehicles (EVs) matter appears to be the swiftest and most convenient to users. The existence of swapping stations increases the feasibility of distributed energy storage via the electric grid. However, it is a cost-prohibitive way of <span class="hlt">charging</span>. Early adaptors' preferences of /perceptions about EV system in general, has its inflectional effects on potential users hence the market penetration level. Yet, the <span class="hlt">charging</span> matter of electric batteries worries the users and puts more pressure on them with the more rigorous planning-ahead they have to make prior to any trip. This paper presents a distinctive way of <span class="hlt">charging</span>. It aims at making the overall <span class="hlt">charging</span> process at ease. From a closer look into the literature, most of EVs' populations depend on domestic <span class="hlt">charge</span>. Domestic <span class="hlt">charging</span> gives them more confidence and increases the usability factor of the EV system. Nevertheless, they still need to count on the publically available <span class="hlt">charging</span> points to reach their destination(s). And when it comes to multifamily residences, it becomes a thorny problem as these apartments do not have a room for <span class="hlt">charging</span> outlets. Having said the irritating <span class="hlt">charging</span> time needed to fatten the batteries over the day and the minimal average mileage drove daily, hypothetically, home delivery <span class="hlt">charging</span> (Movable <span class="hlt">Charging</span> Unit-MCU) would be a stupendous solution. The paper discusses the integration of shortest path algorithm problem with the information about EV users within a metropolitan area, developing an optimal route for a <span class="hlt">charging</span> unit. This MCU delivers <span class="hlt">charging</span> till homes whether by swapping batteries or by fast <span class="hlt">charging</span> facility. Information about users is to be provided by the service provider of the neighbourhood, which includes <span class="hlt">charging</span> patterns (timing, power capacity). This problem lies under the shortest path algorithms problem. It provides optimal route of <span class="hlt">charging</span> that in return shall add more reliability and usability values and alleviate the <span class="hlt">charging</span></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 negative <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('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 additional 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/2060/19960001539','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19960001539"><span>Failures and anomalies attributed to spacecraft <span class="hlt">charging</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Leach, R. D.; Alexander, M. B. (Editor)</p> <p>1995-01-01</p> <p>The effects of spacecraft <span class="hlt">charging</span> can be very detrimental to electronic systems utilized in space missions. Assuring that subsystems and systems are protected against <span class="hlt">charging</span> is an important engineering function necessary to assure mission success. Spacecraft <span class="hlt">charging</span> is expected to have a significant role in future space activities and programs. Objectives of this reference publication are to present a brief overview of spacecraft <span class="hlt">charging</span>, to acquaint the reader with <span class="hlt">charging</span> history, including illustrative cases of <span class="hlt">charging</span> anomalies, and to introduce current spacecraft <span class="hlt">charging</span> prevention activities of the Electromagnetics and Environments Branch, Marshall Space Flight Center (MSFC), National Aeronautics and Space Administration (NASA).</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 addition, 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>, additional control over delivery of <span class="hlt">charged</span> species can be achieved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19990014049','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19990014049"><span>Electrostatic <span class="hlt">Charging</span> of the Pathfinder Rover</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Siebert, Mark W.; Kolecki, Joseph C.</p> <p>1996-01-01</p> <p>The Mars Pathfinder mission will send a lander and a rover to the martian surface. Because of the extremely dry conditions on Mars, electrostatic <span class="hlt">charging</span> of the rover is expected to occur as it moves about. <span class="hlt">Charge</span> accumulation may result in high electrical potentials and discharge through the martian atmosphere. Such discharge could interfere with the operation of electrical elements on the rover. A strategy was sought to mitigate this <span class="hlt">charge</span> accumulation as a precautionary measure. Ground tests were performed to demonstrate <span class="hlt">charging</span> in laboratory conditions simulating the surface conditions expected at Mars. Tests showed that a rover wheel, driven at typical rover speeds, will accumulate electrical <span class="hlt">charge</span> and develop significant electrical potentials (average observed, 110 volts). Measurements were made of wheel electrical potential, and wheel capacitance. From these quantities, the amount of absolute <span class="hlt">charge</span> was estimated. An engineering solution was developed and recommended to mitigate <span class="hlt">charge</span> accumulation. That solution has been implemented on the actual rover.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title48-vol2/pdf/CFR-2014-title48-vol2-sec52-227-6.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title48-vol2/pdf/CFR-2014-title48-vol2-sec52-227-6.pdf"><span>48 CFR 52.227-6 - Royalty Information.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-10-01</p> <p>... 48 Federal Acquisition Regulations System 2 2014-10-01 2014-10-01 false Royalty Information. 52....227-6 Royalty Information. As prescribed in 27.202-5(a)(1), insert the following provision: Royalty Information (<span class="hlt">APR</span> 1984) (a) Cost or <span class="hlt">charges</span> for royalties. When the response to this solicitation contains...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.fs.usda.gov/treesearch/pubs/27662','TREESEARCH'); return false;" href="https://www.fs.usda.gov/treesearch/pubs/27662"><span><span class="hlt">Charge</span>Out! : determining machine and capital equipment <span class="hlt">charge</span>-out rates using discounted cash-flow analysis</span></a></p> <p><a target="_blank" href="http://www.fs.usda.gov/treesearch/">Treesearch</a></p> <p>E.M. (Ted) Bilek</p> <p>2007-01-01</p> <p>The model <span class="hlt">Charge</span>Out! was developed to determine <span class="hlt">charge</span>-out rates or rates of return for machines and capital equipment. This paper introduces a costing methodology and applies it to a piece of capital equipment. Although designed for the forest industry, the methodology is readily transferable to other sectors. Based on discounted cash-flow analysis, <span class="hlt">Charge</span>Out!...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010JPS...195.3928G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010JPS...195.3928G"><span>Solar photovoltaic <span class="hlt">charging</span> of lithium-ion batteries</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gibson, Thomas L.; Kelly, Nelson A.</p> <p></p> <p>Solar photovoltaic (PV) <span class="hlt">charging</span> of batteries was tested by using high efficiency crystalline and amorphous silicon PV modules to recharge lithium-ion battery modules. This testing was performed as a proof of concept for solar PV <span class="hlt">charging</span> of batteries for electrically powered vehicles. The iron phosphate type lithium-ion batteries were safely <span class="hlt">charged</span> to their maximum capacity and the thermal hazards associated with overcharging were avoided by the self-regulating design of the solar <span class="hlt">charging</span> system. The solar energy to battery <span class="hlt">charge</span> conversion efficiency reached 14.5%, including a PV system efficiency of nearly 15%, and a battery <span class="hlt">charging</span> efficiency of approximately 100%. This high system efficiency was achieved by directly <span class="hlt">charging</span> the battery from the PV system with no intervening electronics, and matching the PV maximum power point voltage to the battery <span class="hlt">charging</span> voltage at the desired maximum state of <span class="hlt">charge</span> for the battery. It is envisioned that individual homeowners could <span class="hlt">charge</span> electric and extended-range electric vehicles from residential, roof-mounted solar arrays, and thus power their daily commuting with clean, renewable solar energy.</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 additional 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('https://www.gpo.gov/fdsys/pkg/CFR-2010-title12-vol6/pdf/CFR-2010-title12-vol6-sec706-4.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title12-vol6/pdf/CFR-2010-title12-vol6-sec706-4.pdf"><span>12 CFR 706.4 - Late <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>2010-01-01</p> <p>... indirectly, to levy or collect any delinquency <span class="hlt">charge</span> on a payment, which payment is otherwise a full payment... only delinquency is attributable to late fee(s) or delinquency <span class="hlt">charge(s</span>) assessed on earlier...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA106032','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA106032"><span>A Spacecraft <span class="hlt">Charging</span> Capability for SXTF.</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>1979-01-17</p> <p>surfaces can <span class="hlt">charge</span> up. ’Iiiis differential <span class="hlt">charging</span> of satellite surfaces can cause vacutum sparks , and dielectric breakdowns, and wi 11 effect the S...times required to reach steady <span class="hlt">charge</span> state in the spacecraft internal dielectrics upon electron irradiation. In space , typical times (order of magni...WORDS (Continue on reverse side it necessary end Identify by block nunmber) Spacecraft <span class="hlt">charging</span> Dielectric breakdown SGEMP Electron accelerators</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JHEP...05..012E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JHEP...05..012E"><span><span class="hlt">Charged</span> fermions below 100 GeV</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Egana-Ugrinovic, Daniel; Low, Matthew; Ruderman, Joshua T.</p> <p>2018-05-01</p> <p>How light can a fermion be if it has unit electric <span class="hlt">charge</span>? We revisit the lore that LEP robustly excludes <span class="hlt">charged</span> fermions lighter than about 100 GeV. We review LEP chargino searches, and find them to exclude <span class="hlt">charged</span> fermions lighter than 90 GeV, assuming a higgsino-like cross section. However, if the <span class="hlt">charged</span> fermion couples to a new scalar, destructive interference among production channels can lower the LEP cross section by a factor of 3. In this case, we find that <span class="hlt">charged</span> fermions as light as 75 GeV can evade LEP bounds, while remaining consistent with constraints from the LHC. As the LHC collects more data, <span class="hlt">charged</span> fermions in the 75-100 GeV mass range serve as a target for future monojet and disappearing track searches.</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('http://adsabs.harvard.edu/abs/2016PhRvB..93p1108H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016PhRvB..93p1108H"><span>Engineering <span class="hlt">charge</span> ordering into multiferroicity</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>He, Xu; Jin, Kui-juan</p> <p>2016-04-01</p> <p>Multiferroic materials have attracted great interest but are rare in nature. In many transition-metal oxides, <span class="hlt">charge</span> ordering and magnetic ordering coexist, so that a method of engineering <span class="hlt">charge</span>-ordered materials into ferroelectric materials would lead to a large class of multiferroic materials. We propose a strategy for designing new ferroelectric or even multiferroic materials by inserting a spacing layer into each two layers of <span class="hlt">charge</span>-ordered materials and artificially making a superlattice. One example of the model demonstrated here is the perovskite (LaFeO3)2/LaTiO3 (111) superlattice, in which the LaTiO3 layer acts as the donor and the spacing layer, and the LaFeO3 layer is half doped and performs <span class="hlt">charge</span> ordering. The collaboration of the <span class="hlt">charge</span> ordering and the spacing layer breaks the space inversion symmetry, resulting in a large ferroelectric polarization. As the <span class="hlt">charge</span> ordering also leads to a ferrimagnetic structure, (LaFeO3)2/LaTiO3 is multiferroic. It is expected that this work can encourage the designing and experimental implementation of a large class of multiferroic structures with novel properties.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018E%26ES..113a2117S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018E%26ES..113a2117S"><span>A Novel Methodology for <span class="hlt">Charging</span> Station Deployment</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sun, Zhonghao; Zhao, Yunwei; He, Yueying; Li, Mingzhe</p> <p>2018-02-01</p> <p>Lack of <span class="hlt">charging</span> stations has been a main obstacle to the promotion of electric vehicles. This paper studies deploying <span class="hlt">charging</span> stations in traffic networks considering grid constraints to balance the <span class="hlt">charging</span> demand and grid stability. First, we propose a statistical model for <span class="hlt">charging</span> demand. Then we combine the <span class="hlt">charging</span> demand model with power grid constraints and give the formulation of the <span class="hlt">charging</span> station deployment problem. Finally, we propose a theoretical solution for the problem by transforming it to a Markov Decision Process.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018NatNa..13..316S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018NatNa..13..316S"><span><span class="hlt">Charge</span> splitters and <span class="hlt">charge</span> transport junctions based on guanine quadruplexes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sha, Ruojie; Xiang, Limin; Liu, Chaoren; Balaeff, Alexander; Zhang, Yuqi; Zhang, Peng; Li, Yueqi; Beratan, David N.; Tao, Nongjian; Seeman, Nadrian C.</p> <p>2018-04-01</p> <p>Self-assembling circuit elements, such as current splitters or combiners at the molecular scale, require the design of building blocks with three or more terminals. A promising material for such building blocks is DNA, wherein multiple strands can self-assemble into multi-ended junctions, and nucleobase stacks can transport <span class="hlt">charge</span> over long distances. However, nucleobase stacking is often disrupted at junction points, hindering electric <span class="hlt">charge</span> transport between the two terminals of the junction. Here, we show that a guanine-quadruplex (G4) motif can be used as a connector element for a multi-ended DNA junction. By attaching specific terminal groups to the motif, we demonstrate that <span class="hlt">charges</span> can enter the structure from one terminal at one end of a three-way G4 motif, and can exit from one of two terminals at the other end with minimal carrier transport attenuation. Moreover, we study four-way G4 junction structures by performing theoretical calculations to assist in the design and optimization of these connectors.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018SPIE10585E..18A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018SPIE10585E..18A"><span>Model improvements to simulate <span class="hlt">charging</span> in SEM</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Arat, K. T.; Klimpel, T.; Hagen, C. W.</p> <p>2018-03-01</p> <p><span class="hlt">Charging</span> of insulators is a complex phenomenon to simulate since the accuracy of the simulations is very sensitive to the interaction of electrons with matter and electric fields. In this study, we report model improvements for a previously developed Monte-Carlo simulator to more accurately simulate samples that <span class="hlt">charge</span>. The improvements include both modelling of low energy electron scattering and <span class="hlt">charging</span> of insulators. The new first-principle scattering models provide a more realistic <span class="hlt">charge</span> distribution cloud in the material, and a better match between non-<span class="hlt">charging</span> simulations and experimental results. Improvements on <span class="hlt">charging</span> models mainly focus on redistribution of the <span class="hlt">charge</span> carriers in the material with an induced conductivity (EBIC) and a breakdown model, leading to a smoother distribution of the <span class="hlt">charges</span>. Combined with a more accurate tracing of low energy electrons in the electric field, we managed to reproduce the dynamically changing <span class="hlt">charging</span> contrast due to an induced positive surface potential.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22224178-coupled-electron-nuclear-dynamics-charge-migration-charge-transfer-initiated-near-conical-intersection','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22224178-coupled-electron-nuclear-dynamics-charge-migration-charge-transfer-initiated-near-conical-intersection"><span>Coupled electron-nuclear dynamics: <span class="hlt">Charge</span> migration and <span class="hlt">charge</span> transfer initiated near a conical intersection</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>Mendive-Tapia, David; Vacher, Morgane; Bearpark, Michael J.</p> <p></p> <p>Coupled electron-nuclear dynamics, implemented using the Ehrenfest method, has been used to study <span class="hlt">charge</span> migration with fixed nuclei, together with <span class="hlt">charge</span> transfer when nuclei are allowed to move. Simulations were initiated at reference geometries of neutral benzene and 2-phenylethylamine (PEA), and at geometries close to potential energy surface crossings in the cations. Cationic eigenstates, and the so-called sudden approximation, involving removal of an electron from a correlated ground-state wavefunction for the neutral species, were used as initial conditions. <span class="hlt">Charge</span> migration without coupled nuclear motion could be observed if the Ehrenfest simulation, using the sudden approximation, was started near a conicalmore » intersection where the states were both strongly coupled and quasi-degenerate. Further, the main features associated with <span class="hlt">charge</span> migration were still recognizable when the nuclear motion was allowed to couple. In the benzene radical cation, starting from the reference neutral geometry with the sudden approximation, one could observe sub-femtosecond <span class="hlt">charge</span> migration with a small amplitude, which results from weak interaction with higher electronic states. However, we were able to engineer large amplitude <span class="hlt">charge</span> migration, with a period between 10 and 100 fs, corresponding to oscillation of the electronic structure between the quinoid and anti-quinoid cationic electronic configurations, by distorting the geometry along the derivative coupling vector from the D{sub 6h} Jahn-Teller crossing to lower symmetry where the states are not degenerate. When the nuclear motion becomes coupled, the period changes only slightly. In PEA, in an Ehrenfest trajectory starting from the D{sub 2} eigenstate and reference geometry, a partial <span class="hlt">charge</span> transfer occurs after about 12 fs near the first crossing between D{sub 1}, D{sub 2} (N{sup +}-Phenyl, N-Phenyl{sup +}). If the Ehrenfest propagation is started near this point, using the sudden approximation without</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 addition, 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.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 additive 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('http://www.dtic.mil/docs/citations/ADP011097','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADP011097"><span>Decompression Sickness, Extravehicular Activities, and Nitrogen Induced Osmosis: Brian Hills Revisited</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2001-06-01</p> <p>hypobares ou hyperbares ] To order the complete compilation report, use: ADA395680 The component part is provided here to allow users access to individually...report: TITLE: Operational Medical Issues in Hypo-and Hyperbaric Conditions [les Questions <span class="hlt">medicales</span> a caractere oprationel liees aux conditions...Hypo- and Hyperbaric Conditions ", held in Toronto, Canada, 16-19 October 2000, and published in RTO MP-062. 45-2 upon the local pressure differential</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADP011074','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADP011074"><span>The Role of PWC in Declaring a Diver Fit</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2001-06-01</p> <p>Conditions [les Questions <span class="hlt">medicales</span> a caractere oprationel liees aux conditions hypobares ou hyperbares ] To order the complete compilation report...Approved for public release, distribution unlimited This paper is part of the following report: TITLE: Operational Medical Issues in Hypo-and Hyperbaric ...on "Operational Medical Issues in Hypo- and Hyperbaric Conditions", held in Toronto, Canada, 16-19 October 2000, and published in RTO MP-062. 18-2</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADP011091','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADP011091"><span>Altitude Decompression Illness - The Operational Risk at Sustained Altitudes up to 35,000 ft.</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2001-06-01</p> <p>TITLE: Operational Medical Issues in Hypo-and Hyperbaric Conditions [les Questions <span class="hlt">medicales</span> a caractere oprationel liees aux conditions hypobares ou... hyperbares ] To order the complete compilation report, use: ADA395680 The component part is provided here to allow users access to individually authored... Hyperbaric Conditions", held in Toronto, Canada, 16-19 October 2000, and published in RTO MP-062. 37-2 by a tissue response to the presence of bubbles</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADP011071','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADP011071"><span>Designing Efficient and Effective, Operationally Relevant, High Altitude Training Profiles</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2001-06-01</p> <p>Operational Medical Issues in Hypo-and Hyperbaric Conditions [les Questions <span class="hlt">medicales</span> a caractere oprationel liees aux conditions hypobares ou... hyperbares ] To order the complete compilation report, use: ADA395680 The component part is provided here to allow users access to individually authored...Airforce was felt to meet this need and was recommended. Paper presented at the RTO HFM Symposium on "Operational Medical Issues in Hypo- and Hyperbaric</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADP011094','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADP011094"><span>Modeling Approach for Oxygen Exchange in the Human Lung under Hypobaric Conditions</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2001-06-01</p> <p>Operational Medical Issues in Hypo-and Hyperbaric Conditions [les Questions <span class="hlt">medicales</span> a caractere oprationel liees aux conditions hypobares ou hyperbares ] To...under Hypobaric Conditions DISTRIBUTION: Approved for public release, distribution unlimited This paper is part of the following report: TITLE...Approach for Oxygen Exchange in the Human Lung under Hypobaric Conditions Ing J.P.F. Lindhout*, Drs M. van de Graaff*, Ir Drs R.C. van de Graaff*, Dr</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADP011067','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADP011067"><span>Neuropsychometric Test in Royal Netherlands Navy Mine-Clearance Divers</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2001-06-01</p> <p>Issues in Hypo-and Hyperbaric Conditions [les Questions <span class="hlt">medicales</span> a caractere oprationel liees aux conditions hypobares ou hyperbares ] To order the...Digit Memo Sjan Test (F/B DMST-F/B Learnin /memoie Paper presented at the RTO HFM Symposium on "Operational Medical Issues in Hypo- and Hyperbaric ... Hyperbaric Medicine Annual Meeting 1995, Florida, USA. Abstract 46: 35. 6. Baker EL, R Letz, A Fidler. A computer-administered Neurobehavioural Evaluation</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19700000179','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19700000179"><span>Nondissipative optimum <span class="hlt">charge</span> regulator</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Rosen, R.; Vitebsky, J. N.</p> <p>1970-01-01</p> <p>Optimum <span class="hlt">charge</span> regulator provides constant level <span class="hlt">charge</span>/discharge control of storage batteries. Basic power transfer and control is performed by solar panel coupled to battery through power switching circuit. Optimum controller senses battery current and modifies duty cycle of switching circuit to maximize current available to battery.</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 addition 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 addition 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('https://www.osti.gov/servlets/purl/1369380','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1369380"><span>EV <span class="hlt">Charging</span> Infrastructure Roadmap</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>Karner, Donald; Garetson, Thomas; Francfort, Jim</p> <p>2016-08-01</p> <p>As highlighted in the U.S. Department of Energy’s EV Everywhere Grand Challenge, vehicle technology is advancing toward an objective to “… produce plug-in electric vehicles that are as affordable and convenient for the average American family as today’s gasoline-powered vehicles …” [1] by developing more efficient drivetrains, greater battery energy storage per dollar, and lighter-weight vehicle components and construction. With this technology advancement and improved vehicle performance, the objective for <span class="hlt">charging</span> infrastructure is to promote vehicle adoption and maximize the number of electric miles driven. The EV Everywhere <span class="hlt">Charging</span> Infrastructure Roadmap (hereafter referred to as Roadmap) looks forward and assumesmore » that the technical challenges and vehicle performance improvements set forth in the EV Everywhere Grand Challenge will be met. The Roadmap identifies and prioritizes deployment of <span class="hlt">charging</span> infrastructure in support of this <span class="hlt">charging</span> infrastructure objective for the EV Everywhere Grand Challenge« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140011369','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140011369"><span>Spacecraft <span class="hlt">Charging</span> Issues for Launch Vehicles</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Buhler, Janessa L.; Minow, Joseph I.; Trout, Dawn H.</p> <p>2014-01-01</p> <p>Spacecraft <span class="hlt">charging</span> is well known threat to successful long term spacecraft operations and instrument reliability in orbits that spend significant time in hot electron environments. In recent years, spacecraft <span class="hlt">charging</span> has increasingly been recognized as a potentially significant engineering issue for launch vehicles used to deploy spacecraft using (a) low Earth orbit (LEO), high inclination flight trajectories that pass through the auroral zone, (b) geostationary transfer orbits that require exposures to the hot electron environments in the Earths outer radiation belts, and (c) LEO escape trajectories using multiple phasing orbits through the Earths radiation belts while raising apogee towards a final Earth escape geometry. <span class="hlt">Charging</span> becomes an issue when significant areas of exposed insulating materials or ungrounded conductors are used in the launch vehicle design or the payload is designed for use in a benign <span class="hlt">charging</span> region beyond the Earths magnetosphere but must survive passage through the strong <span class="hlt">charging</span> regimes of the Earths radiation belts. This presentation will first outline the <span class="hlt">charging</span> risks encountered on typical launch trajectories used to deploy spacecraft into Earth orbit and Earth escape trajectories. We then describe the process used by NASAs Launch Services Program to evaluate when surface and internal <span class="hlt">charging</span> is a potential risk to a NASA mission. Finally, we describe the options for mitigating <span class="hlt">charging</span> risks including modification of the launch vehicle andor payload design and controlling the risk through operational launch constraints to avoid significant <span class="hlt">charging</span> environments.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/5030546-charge-control-microcomputer-device-vehicles','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/5030546-charge-control-microcomputer-device-vehicles"><span><span class="hlt">Charge</span> control microcomputer device for vehicles</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>Morishita, M.; Kouge, S.</p> <p>1986-10-14</p> <p>This patent describes a <span class="hlt">charge</span> control microcomputer device for a vehicle, comprising: speed changing means for transmitting the output torque of an engine. The speed changing means includes a slip clutch means having an output with a variable slippage amount with respect to its input and controlled in accordance with an operating instruction. The speed changing means further includes a speed change gear for changing the rotational speed input thereto at an output thereto, the speed change gear receiving the output of the slip clutch means; a <span class="hlt">charging</span> generator driven by the output of the speed change gear; a batterymore » <span class="hlt">charged</span> by an output voltage of the <span class="hlt">charging</span> generator; a voltage regulator for controlling the output voltage of the <span class="hlt">charging</span> generator to a predetermined value; an engine controlling microcomputer for receiving data from the engine, to control the engine, the engine data comprising at least an engine speed signal; a <span class="hlt">charge</span> control microcomputer for processing engine data from the engine controlling microcomputer and <span class="hlt">charge</span> system data including terminal voltage data from the battery and generated voltage data from the changing generator; and a display unit for displaying detection data, including fault detection data, form the <span class="hlt">charge</span> control microcomputer.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23030920','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23030920"><span>Spatial inhomogeneities in ionic liquids, <span class="hlt">charged</span> proteins, and <span class="hlt">charge</span> stabilized colloids from collective variables theory.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Patsahan, O; Ciach, A</p> <p>2012-09-01</p> <p>Effects of size and <span class="hlt">charge</span> asymmetry between oppositely <span class="hlt">charged</span> ions or particles on spatial inhomogeneities are studied for a large range of <span class="hlt">charge</span> and size ratios. We perform a stability analysis of the primitive model of ionic systems with respect to periodic ordering using the collective variables-based theory. We extend previous studies [Ciach et al., Phys. Rev. E 75, 051505 (2007)] in several ways. First, we employ a nonlocal approximation for the reference hard-sphere fluid which leads to the Percus-Yevick pair direct correlation functions for the uniform case. Second, we use the Weeks-Chandler-Anderson regularization scheme for the Coulomb potential inside the hard core. We determine the relevant order parameter connected with the periodic ordering and analyze the character of the dominant fluctuations along the λ lines. We show that the above-mentioned modifications produce large quantitative and partly qualitative changes in the phase diagrams obtained previously. We discuss possible scenarios of the periodic ordering for the whole range of size and <span class="hlt">charge</span> ratios of the two ionic species, covering electrolytes, ionic liquids, <span class="hlt">charged</span> globular proteins or nanoparticles in aqueous solutions, and <span class="hlt">charge</span>-stabilized colloids.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015APS..DFDA36003B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015APS..DFDA36003B"><span>Interaction between electrically <span class="hlt">charged</span> droplets in microgravity</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Brandenbourger, Martin; Caps, Herve; Hardouin, Jerome; Vitry, Youen; Boigelot, Bernard; Dorbolo, Stephane; Grasp Team; Beams Collaboration</p> <p>2015-11-01</p> <p>The past ten years, electrically <span class="hlt">charged</span> droplets have been studied tremendously for their applications in industry (electrospray, electrowetting,...). However, <span class="hlt">charged</span> droplets are also present in nature. Indeed, it has been shown that the droplets falling from thunderclouds possess an excess of electric <span class="hlt">charges</span>. Moreover, some research groups try to use the electrical interaction between drops in order to control the coalescence between cloud droplets and control rain generation. The common way to study this kind of system is to make hypothesis on the interaction between two <span class="hlt">charged</span> drops. Then, these hypothesis are extended to a system of thousands of <span class="hlt">charged</span> droplets. Thanks to microgravity conditions, we were able to study the interaction between two electrically <span class="hlt">charged</span> droplets. In practice, the <span class="hlt">charged</span> droplets were propelled one in front of the other at low speed (less than 1 m/s). The droplets trajectory is studied for various <span class="hlt">charges</span> and volumes. The repulsion between two <span class="hlt">charged</span> drops is correctly fitted by a simple Coulomb repulsion law. In the case of attractive interactions, we discuss the collisions observed as a function of the droplets speed, volume and electric <span class="hlt">charges</span>. Thanks to FNRS for financial support.</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.ncbi.nlm.nih.gov/pubmed/29410440','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29410440"><span>The <span class="hlt">Charging</span> Events in Contact-Separation Electrification.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Musa, Umar G; Cezan, S Doruk; Baytekin, Bilge; Baytekin, H Tarik</p> <p>2018-02-06</p> <p>Contact electrification (CE)-<span class="hlt">charging</span> of surfaces that are contacted and separated, is a common phenomenon, however it is not completely understood yet. Recent studies using surface imaging techniques and chemical analysis revealed a 'spatial' bipolar distribution of <span class="hlt">charges</span> at the nano dimension, which made a paradigm shift in the field. However, such analyses can only provide information about the <span class="hlt">charges</span> that remained on the surface after the separation, providing limited information about the actual course of the CE event. Tapping common polymers and metal surfaces to each other and detecting the electrical potential produced on these surfaces 'in-situ' in individual events of contact and separation, we show that, <span class="hlt">charges</span> are generated and transferred between the surfaces in both events; the measured potential is bipolar in contact and unipolar in separation. We show, the 'contact-<span class="hlt">charges</span>' on the surfaces are indeed the net <span class="hlt">charges</span> that results after the separation process, and a large contribution to tribocharge harvesting comes, in fact, from the electrostatic induction resulting from the generated CE <span class="hlt">charges</span>. Our results refine the mechanism of CE providing information for rethinking the conventional ranking of materials' <span class="hlt">charging</span> abilities, <span class="hlt">charge</span> harvesting, and <span class="hlt">charge</span> prevention.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JPhB...51a4003P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JPhB...51a4003P"><span>Impact of <span class="hlt">charge</span>-transfer excitons in regioregular polythiophene on the <span class="hlt">charge</span> separation at polythiophene-fullerene heterojunctions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Polkehn, M.; Tamura, H.; Burghardt, I.</p> <p>2018-01-01</p> <p>This study addresses the mechanism of ultrafast <span class="hlt">charge</span> separation in regioregular oligothiophene-fullerene assemblies representative of poly-3-hexylthiophene (P3HT)-[6,6]-phenyl-C61 butyric acid methyl ester (PCBM) heterojunctions, with special emphasis on the inclusion of <span class="hlt">charge</span> transfer excitons in the oligothiophene phase. The formation of polaronic inter-chain <span class="hlt">charge</span> separated species in highly ordered oligothiophene has been demonstrated in recent experiments and could have a significant impact on the net <span class="hlt">charge</span> transfer to the fullerene acceptor. The present approach combines a first-principles parametrized multi-site Hamiltonian, based on time-dependent density functional theory calculations, with accurate quantum dynamics simulations using the multi-layer multi-configuration time-dependent Hartree method. Quantum dynamical studies are carried out for up to 182 electronic states and 112 phonon modes. The present analysis follows up on our previous study of (Huix-Rotllant et al 2015 J. Phys. Chem. Lett. 6 1702) and significantly expands the scope of this analysis by including the dynamical role of <span class="hlt">charge</span> transfer excitons. Our investigation highlights the pronounced mixing of photogenerated Frenkel excitons with <span class="hlt">charge</span> transfer excitons in the oligothiophene domain, and the opening of new transfer channels due the creation of such <span class="hlt">charge</span>-separated species. As a result, it turns out that the interfacial donor/acceptor <span class="hlt">charge</span> transfer state can be largely circumvented due to the presence of <span class="hlt">charge</span> transfer excitons. However, the latter states in turn act as a trap, such that the free carrier yield observed on ultrafast time scales is tangibly reduced. The present analysis underscores the complexity of the transfer pathways at P3HT-PCBM type junctions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1992ZPhyC..54...45J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1992ZPhyC..54...45J"><span>Multiplicity distributions of <span class="hlt">charged</span> hadrons in vp and <span class="hlt">charged</span> current interactions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jones, G. T.; Jones, R. W. L.; Kennedy, B. W.; Morrison, D. R. O.; Mobayyen, M. M.; Wainstein, S.; Aderholz, M.; Hantke, D.; Katz, U. F.; Kern, J.; Schmitz, N.; Wittek, W.; Borner, H. P.; Myatt, G.; Radojicic, D.; Burke, S.</p> <p>1992-03-01</p> <p>Using data on vp andbar vp <span class="hlt">charged</span> current interactions from a bubble chamber experiment with BEBC at CERN, the multiplicity distributions of <span class="hlt">charged</span> hadrons are investigated. The analysis is based on ˜20000 events with incident v and ˜10000 events with incidentbar v. The invariant mass W of the total hadronic system ranges from 3 GeV to ˜14 GeV. The experimental multiplicity distributions are fitted by the binomial function (for different intervals of W and in different intervals of the rapidity y), by the Levy function and the lognormal function. All three parametrizations give acceptable values for X 2. For fixed W, forward and backward multiplicities are found to be uncorrelated. The normalized moments of the <span class="hlt">charged</span> multiplicity distributions are measured as a function of W. They show a violation of KNO scaling.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JGP...125...12B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JGP...125...12B"><span>Dynamics of <span class="hlt">charges</span> and solitons</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Barros, Manuel; Ferrández, Ángel; Garay, Óscar J.</p> <p>2018-02-01</p> <p>We first show that trajectories traced by <span class="hlt">charges</span> moving in rotational magnetic fields are, basically, the non-parallel geodesics of surfaces of revolution with coincident axis. Thus, people living in a surface of revolution are not able to sense the magnetic Hall effect induced by the surrounding magnetic field and perceive <span class="hlt">charges</span> as influenced, exclusively, by the gravity action on the surface of revolution. Secondly, the extended Hasimoto transformations are introduced and then used to identify trajectories of <span class="hlt">charges</span> moving through a Killing rotational magnetic field in terms of non-circular elastic curves. As a consequence, we see that in this case <span class="hlt">charges</span> evolve along trajectories which are obtained as extended Hasimoto transforms of solitons of the filament equation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23215112','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23215112"><span>Radio frequency <span class="hlt">charge</span> parity meter.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Schroer, M D; Jung, M; Petersson, K D; Petta, J R</p> <p>2012-10-19</p> <p>We demonstrate a total <span class="hlt">charge</span> parity measurement by detecting the radio frequency signal that is reflected by a lumped-element resonator coupled to a single InAs nanowire double quantum dot. The high frequency response of the circuit is used to probe the effects of the Pauli exclusion principle at interdot <span class="hlt">charge</span> transitions. Even parity <span class="hlt">charge</span> transitions show a striking magnetic field dependence that is due to a singlet-triplet transition, while odd parity transitions are relatively insensitive to a magnetic field. The measured response agrees well with cavity input-output theory, allowing accurate measurements of the interdot tunnel coupling and the resonator-<span class="hlt">charge</span> coupling rate g(c)/2π~17 MHz.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JPS...367..216M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JPS...367..216M"><span>Enabling fast <span class="hlt">charging</span> - Vehicle considerations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Meintz, Andrew; Zhang, Jiucai; Vijayagopal, Ram; Kreutzer, Cory; Ahmed, Shabbir; Bloom, Ira; Burnham, Andrew; Carlson, Richard B.; Dias, Fernando; Dufek, Eric J.; Francfort, James; Hardy, Keith; Jansen, Andrew N.; Keyser, Matthew; Markel, Anthony; Michelbacher, Christopher; Mohanpurkar, Manish; Pesaran, Ahmad; Scoffield, Don; Shirk, Matthew; Stephens, Thomas; Tanim, Tanvir</p> <p>2017-11-01</p> <p>To achieve a successful increase in the plug-in battery electric vehicle (BEV) market, it is anticipated that a significant improvement in battery performance is required to increase the range that BEVs can travel and the rate at which they can be recharged. While the range that BEVs can travel on a single recharge is improving, the recharge rate is still much slower than the refueling rate of conventional internal combustion engine vehicles. To achieve comparable recharge times, we explore the vehicle considerations of <span class="hlt">charge</span> rates of at least 400 kW. Faster recharge is expected to significantly mitigate the perceived deficiencies for long-distance transportation, to provide alternative <span class="hlt">charging</span> in densely populated areas where overnight <span class="hlt">charging</span> at home may not be possible, and to reduce range anxiety for travel within a city when unplanned <span class="hlt">charging</span> may be required. This substantial increase in <span class="hlt">charging</span> rate is expected to create technical issues in the design of the battery system and the vehicle's electrical architecture that must be resolved. This work focuses on vehicle system design and total recharge time to meet the goals of implementing improved <span class="hlt">charge</span> rates and the impacts of these expected increases on system voltage and vehicle components.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19850000058&hterms=battery+fuel&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dbattery%2Bfuel','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19850000058&hterms=battery+fuel&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dbattery%2Bfuel"><span>Battery-<span class="hlt">Charge</span>-State Model</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Vivian, H. C.</p> <p>1985-01-01</p> <p><span class="hlt">Charge</span>-state model for lead/acid batteries proposed as part of effort to make equivalent of fuel gage for battery-powered vehicles. Models based on equations that approximate observable characteristics of battery electrochemistry. Uses linear equations, easier to simulate on computer, and gives smooth transitions between <span class="hlt">charge</span>, discharge, and recuperation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1069158','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1069158"><span>Review of Variable Generation Integration <span class="hlt">Charges</span></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>Porter, K.; Fink, S.; Buckley, M.</p> <p>2013-03-01</p> <p>The growth of wind and solar generation in the United States, and the expectation of continued growth of these technologies, dictates that the future power system will be operated in a somewhat different manner because of increased variability and uncertainty. A small number of balancing authorities have attempted to determine an 'integration cost' to account for these changes to their current operating practices. Some balancing authorities directly <span class="hlt">charge</span> wind and solar generators for integration <span class="hlt">charges</span>, whereas others add integration <span class="hlt">charges</span> to projected costs of wind and solar in integrated resource plans or in competitive solicitations for generation. This report reviewsmore » the balancing authorities that have calculated variable generation integration <span class="hlt">charges</span> and broadly compares and contrasts the methodologies they used to determine their specific integration <span class="hlt">charges</span>. The report also profiles each balancing authority and how they derived wind and solar integration <span class="hlt">charges</span>.« less</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 negatively <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/2018AIPC.1928b0010M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AIPC.1928b0010M"><span>Highly <span class="hlt">charged</span> ion beams and their applications</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Marler, Joan</p> <p>2018-01-01</p> <p>While much previous work with highly <span class="hlt">charged</span> ions has been performed with the ions in the plasma state in which they were formed, beams of highly <span class="hlt">charged</span> ions hold promise for exciting new experiments. Specifically low energy beams with a high degree of <span class="hlt">charge</span> state purity are a prerequisite for momentum resolved cross section measurements and for efficient loading of highly <span class="hlt">charged</span> ions into UHV traps for spectroscopy. The Clemson University facility is optimized for the delivery of such beams of highly <span class="hlt">charged</span> ions with low kinetic energies. Near term experiments include energy resolved <span class="hlt">charge</span> exchange with neutral targets.</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 negatively <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('https://www.osti.gov/servlets/purl/1393636','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1393636"><span>Exploring Demand <span class="hlt">Charge</span> Savings from Commercial Solar</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>Darghouth, Naim; Barbose, Galen; Mills, Andrew</p> <p></p> <p>Commercial retail electricity rates commonly include a demand <span class="hlt">charge</span> component, based on some measure of the customer’s peak demand. Customer-sited solar PV can potentially reduce demand <span class="hlt">charges</span>, but the magnitude of these savings can be difficult to predict, given variations in demand <span class="hlt">charge</span> designs, customer loads, and PV generation profiles. Moreover, depending on the circumstances, demand <span class="hlt">charges</span> from solar may or may not align well with associated utility cost savings. Lawrence Berkeley National Laboratory (Berkeley Lab) and the National Renewable Energy Laboratory (NREL) are collaborating in a series of studies to understand how solar PV can reduce demand <span class="hlt">charge</span> levelsmore » for a variety of customer types and demand <span class="hlt">charges</span> designs. Previous work focused on residential customs with solar. This study, instead, focuses on commercial customers and seeks to understand the extent and conditions under which rooftop can solar reduce commercial demand <span class="hlt">charges</span>. To answer these questions, we simulate demand <span class="hlt">charge</span> savings for a broad range of commercial customer types, demand <span class="hlt">charge</span> designs, locations, and PV system characteristics. This particular analysis does not include storage, but a subsequent analysis in this series will evaluate demand <span class="hlt">charge</span> savings for commercial customers with solar and storage.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22680073-cracking-charged-anisotropic-polytropes','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22680073-cracking-charged-anisotropic-polytropes"><span>On cracking of <span class="hlt">charged</span> anisotropic polytropes</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>Azam, M.; Mardan, S.A., E-mail: azam.math@ue.edu.pk, E-mail: syedalimardanazmi@yahoo.com</p> <p>2017-01-01</p> <p>Recently in [1], the role of electromagnetic field on the cracking of spherical polytropes has been investigated without perturbing <span class="hlt">charge</span> parameter explicitly. In this study, we have examined the occurrence of cracking of anisotropic spherical polytropes through perturbing parameters like anisotropic pressure, energy density and <span class="hlt">charge</span>. We consider two different types of polytropes in this study. We discuss the occurrence of cracking in two different ways ( i ) by perturbing polytropic constant, anisotropy and <span class="hlt">charge</span> parameter ( ii ) by perturbing polytropic index, anisotropy and <span class="hlt">charge</span> parameter for each case. We conclude that cracking appears for a wide rangemore » of parameters in both cases. Also, our results are reduced to [2] in the absence of <span class="hlt">charge</span>.« less</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 addition, 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://eric.ed.gov/?q=Electricity&pg=4&id=EJ984094','ERIC'); return false;" href="https://eric.ed.gov/?q=Electricity&pg=4&id=EJ984094"><span>Can Like <span class="hlt">Charges</span> Attract Each Other?</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>Balta, Nuri</p> <p>2012-01-01</p> <p>Electroscopes are sensitive instruments useful for investigations of static electricity. They are devices that are used for detecting whether an object is <span class="hlt">charged</span> or uncharged. They also determine the type of <span class="hlt">charge</span>. Their operation is based on the principle of like sign <span class="hlt">charge</span> repulsion.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JASMS..28..498K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JASMS..28..498K"><span>Spontaneous Mass and <span class="hlt">Charge</span> Losses from Single Multi-Megadalton Ions Studied by <span class="hlt">Charge</span> Detection Mass Spectrometry</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Keifer, David Z.; Alexander, Andrew W.; Jarrold, Martin F.</p> <p>2017-03-01</p> <p>Spontaneous mass and <span class="hlt">charge</span> losses from individual multi-megadalton ions have been observed with <span class="hlt">charge</span> detection mass spectrometry (CDMS) by trapping single hepatitis B virus (HBV) capsids for 3 s. Gradual increases in the oscillation frequency of single ions in the ion trap are attributed mainly to mass loss (probably solvent, water, and/or salt). The total mass lost during the 3 s trapping period peaks at around 20 kDa for 4 MDa HBV T = 4 capsids. Discrete frequency drops punctuate the gradual increases in the oscillation frequencies. The drops are attributed to a sudden loss of <span class="hlt">charge</span>. In most cases a single positive <span class="hlt">charge</span> is lost along with some mass (on average around 1000 Da). <span class="hlt">Charge</span> loss occurs for over 40% of the trapped ions. It usually occurs near the beginning of the trapping event, and it occurs preferentially in regions of the trap with strong electric fields, indicating that external electric fields promote <span class="hlt">charge</span> loss. This process may contribute to the decrease in m/ z resolution that often occurs with megadalton ions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title30-vol1/pdf/CFR-2010-title30-vol1-sec57-4502.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title30-vol1/pdf/CFR-2010-title30-vol1-sec57-4502.pdf"><span>30 CFR 57.4502 - Battery-<span class="hlt">charging</span> stations.</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>2010-07-01</p> <p>... 30 Mineral Resources 1 2010-07-01 2010-07-01 false Battery-<span class="hlt">charging</span> stations. 57.4502 Section 57... and Control Installation/construction/maintenance § 57.4502 Battery-<span class="hlt">charging</span> stations. (a) Battery... shall be prohibited at the battery <span class="hlt">charging</span> station during battery <span class="hlt">charging</span>. (c) Readily visible signs...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title30-vol1/pdf/CFR-2013-title30-vol1-sec57-4502.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title30-vol1/pdf/CFR-2013-title30-vol1-sec57-4502.pdf"><span>30 CFR 57.4502 - Battery-<span class="hlt">charging</span> stations.</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>2013-07-01</p> <p>... 30 Mineral Resources 1 2013-07-01 2013-07-01 false Battery-<span class="hlt">charging</span> stations. 57.4502 Section 57... and Control Installation/construction/maintenance § 57.4502 Battery-<span class="hlt">charging</span> stations. (a) Battery... shall be prohibited at the battery <span class="hlt">charging</span> station during battery <span class="hlt">charging</span>. (c) Readily visible signs...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title30-vol1/pdf/CFR-2012-title30-vol1-sec57-4502.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title30-vol1/pdf/CFR-2012-title30-vol1-sec57-4502.pdf"><span>30 CFR 57.4502 - Battery-<span class="hlt">charging</span> stations.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-07-01</p> <p>... 30 Mineral Resources 1 2012-07-01 2012-07-01 false Battery-<span class="hlt">charging</span> stations. 57.4502 Section 57... and Control Installation/construction/maintenance § 57.4502 Battery-<span class="hlt">charging</span> stations. (a) Battery... shall be prohibited at the battery <span class="hlt">charging</span> station during battery <span class="hlt">charging</span>. (c) Readily visible signs...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title30-vol1/pdf/CFR-2014-title30-vol1-sec57-4502.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title30-vol1/pdf/CFR-2014-title30-vol1-sec57-4502.pdf"><span>30 CFR 57.4502 - Battery-<span class="hlt">charging</span> stations.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-07-01</p> <p>... 30 Mineral Resources 1 2014-07-01 2014-07-01 false Battery-<span class="hlt">charging</span> stations. 57.4502 Section 57... and Control Installation/construction/maintenance § 57.4502 Battery-<span class="hlt">charging</span> stations. (a) Battery... shall be prohibited at the battery <span class="hlt">charging</span> station during battery <span class="hlt">charging</span>. (c) Readily visible signs...</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.gpo.gov/fdsys/pkg/CFR-2011-title30-vol1/pdf/CFR-2011-title30-vol1-sec57-4502.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title30-vol1/pdf/CFR-2011-title30-vol1-sec57-4502.pdf"><span>30 CFR 57.4502 - Battery-<span class="hlt">charging</span> stations.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-07-01</p> <p>... 30 Mineral Resources 1 2011-07-01 2011-07-01 false Battery-<span class="hlt">charging</span> stations. 57.4502 Section 57... and Control Installation/construction/maintenance § 57.4502 Battery-<span class="hlt">charging</span> stations. (a) Battery... shall be prohibited at the battery <span class="hlt">charging</span> station during battery <span class="hlt">charging</span>. (c) Readily visible signs...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23979034','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23979034"><span>Longitudinal <span class="hlt">charge</span> nurse leadership development and evaluation.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Krugman, Mary; Heggem, Laura; Kinney, Lisa Judd; Frueh, Margaret</p> <p>2013-09-01</p> <p>The study's aim was to examine longitudinal outcomes of a leadership program for permanent and relief <span class="hlt">charge</span> nurse from 1996 to 2012 using action research and Kouzes and Posner's The Leadership Challenge conceptual frameworks. <span class="hlt">Charge</span> nurses hold significant oversight of patient safety, quality, and team functioning. This study contributes knowledge regarding <span class="hlt">charge</span> nurse leadership and organization outcomes associated with these essential roles over time. Data were collected over 6 time periods using Kouzes and Posner's The Leadership Practices Inventory (LPI) and internally developed action research tools. Surveys were aligned with leadership and work environment changes to examine outcomes. <span class="hlt">Charge</span> nurse leadership LPI mean ratings improved. Relief <span class="hlt">charge</span> nurses reached similar LPI outcomes by 2012, with no statistical differences in mean or domain scores. Action research methods facilitated executive decision making during change processes. Demographics shifted with younger <span class="hlt">charge</span> nurses with less practice experience serving as <span class="hlt">charge</span> nurses in the most recent years. <span class="hlt">Charge</span> nurse leadership reported significant gains despite institutional changes and uneven delivery of educational interventions.</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 negatively <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('http://adsabs.harvard.edu/abs/2007PhDT........30T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007PhDT........30T"><span>Development and study of <span class="hlt">charge</span> sensors for fast <span class="hlt">charge</span> detection in 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>Thalakulam, Madhu</p> <p></p> <p><span class="hlt">Charge</span> detection at microsecond time-scales has far reaching consequences in both technology and in our understanding of electron dynamics in nanoscale devices such as quantum dots. Radio-frequency superconducting single electron transistors (RF-SET) and quantum point contacts (QPC) are ultra sensitive <span class="hlt">charge</span> sensors operating near the quantum limit. The operation of RF-SETs outside the superconducting gap has been a topic of study; the sub-gap operation, especially in the presence of large quantum fluctuations of quasiparticles remains largely unexplored, both theoretically and experimentally. We have investigated the effects of quantum fluctuations of quasiparticles on the operation of RF-SETs for large values of the quasiparticle cotunneling parameter alpha = 8EJ/Ec, where EJ and Ec are the Josephson and <span class="hlt">charging</span> energies. We find that, for alpha > 1, sub-gap RF-SET operation is still feasible despite quantum fluctuations that wash out quasiparticle tunneling thresholds. Such RF-SETs show linearity and signal-to-noise ratio superior to those obtained when quantum fluctuations are weak, while still demonstrating excellent <span class="hlt">charge</span> sensitivity. We have operated a QPC <span class="hlt">charge</span> detector in a radio frequency mode that allows fast <span class="hlt">charge</span> detection in a bandwidth of several megahertz. The noise limiting the sensitivity of the <span class="hlt">charge</span> detector is not the noise of a secondary amplifier, but the non-equilibrium device noise of the QPC itself. The noise power averaged over a measurement bandwidth of about 10MHz around the carrier frequency is in agreement with the theory of photon-assisted shot noise. Frequency-resolved measurements, however show several significant discrepancies with the theoretical predictions. The measurement techniques developed can also be used to investigate the noise of other semiconductor nanostructures such as quantum dots in the Kondo regime. A study of the noise characteristics alone can not determine whether the device is operating at the quantum</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 addition 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. Additionally, 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.osti.gov/biblio/15020603-summary-update-astm-guide-charge-control-charge-referencing-techniques-ray-photoelectron-spectroscopy','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/15020603-summary-update-astm-guide-charge-control-charge-referencing-techniques-ray-photoelectron-spectroscopy"><span>Summary: Update to ASTM Guide E 1523 to <span class="hlt">Charge</span> Control and <span class="hlt">Charge</span> Referencing Techniques in X-ray Photoelectron Spectroscopy</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>Baer, Donald R.</p> <p>2005-04-22</p> <p>An updated version of the ASTM guide E1523 to the methods to <span class="hlt">charge</span> control and <span class="hlt">charge</span> referencing techniques in x-ray photoelectron spectroscopy has been released by ASTM. The guide is meant to acquaint x-ray photoelectron spectroscopy (XPS) users with the various <span class="hlt">charge</span> control and <span class="hlt">charge</span> referencing techniques that are and have been used in the acquisition and interpretation of XPS data from surfaces of insulating specimens. The current guide has been expanded to include new references as well as recommendations for reporting information on <span class="hlt">charge</span> control and <span class="hlt">charge</span> referencing. The previous version of the document had been published in 1997.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20136335','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20136335"><span>Overcharging and <span class="hlt">charge</span> reversal in the electrical double layer around the point of zero <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>Guerrero-García, G Iván; González-Tovar, Enrique; Chávez-Páez, Martín; Lozada-Cassou, Marcelo</p> <p>2010-02-07</p> <p>The ionic adsorption around a weakly <span class="hlt">charged</span> spherical colloid, immersed in size-asymmetric 1:1 and 2:2 salts, is studied. We use the primitive model (PM) of an electrolyte to perform Monte Carlo simulations as well as theoretical calculations by means of the hypernetted chain/mean spherical approximation (HNC/MSA) and the unequal-radius modified Gouy-Chapman (URMGC) integral equations. Structural quantities such as the radial distribution functions, the integrated <span class="hlt">charge</span>, and the mean electrostatic potential are reported. Our Monte Carlo "experiments" evidence that near the point of zero <span class="hlt">charge</span>, the smallest ionic species is preferentially adsorbed onto the macroparticle, independently of the sign of the <span class="hlt">charge</span> carried by this tiniest electrolytic component, giving rise to the appearance of the phenomena of <span class="hlt">charge</span> reversal (CR) and overcharging (OC). Accordingly, colloidal CR, due to an excessive attachment of counterions, is observed when the macroion is slightly <span class="hlt">charged</span> and the coions are larger than the counterions. In the opposite situation, i.e., if the counterions are larger than the coions, the central macroion acquires additional like-<span class="hlt">charge</span> (coions) and hence becomes "overcharged," a feature theoretically predicted in the past [F. Jiménez-Angeles and M. Lozada-Cassou, J. Phys. Chem. B 108, 7286 (2004)]. In other words, here we present the first simulation data on OC in the PM electrical double layer, showing that close to the point of zero <span class="hlt">charge</span>, this novel effect surges as a consequence of the ionic size asymmetry. We also find that the HNC/MSA theory captures well the CR and OC phenomena exhibited by the computer experiments, especially as the macroion's <span class="hlt">charge</span> increases. On the contrary, even if URMGC also displays CR and OC, its predictions do not compare favorably with the Monte Carlo data, evidencing that the inclusion of hard-core correlations in Monte Carlo and HNC/MSA enhances and extends those effects. We explain our findings in terms of the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23464175','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23464175"><span>Solvation effects on like-<span class="hlt">charge</span> attraction.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ghanbarian, Shahzad; Rottler, Jörg</p> <p>2013-02-28</p> <p>We present results of molecular dynamics simulations of the electrostatic interaction between two parallel <span class="hlt">charged</span> rods in the presence of divalent counterions. Such polyelectrolytes have been considered as a simple model for understanding electrostatic interactions in highly <span class="hlt">charged</span> biomolecules such as DNA. Since there are correlations between the free <span class="hlt">charge</span> carriers, the phenomenon of like <span class="hlt">charge</span> attraction appears for specific parameters. We explore the role of solvation effects and the resulting deviations from Coulomb's law on the nanoscale on this peculiar phenomenon. The behavior of the force between the <span class="hlt">charged</span> rods in a simulation with atomistic representation of water molecules is completely different from a model in which water is modeled as a continuum dielectric. By calculating counterion-rodion pair correlation functions, we find that the presence of water molecules changes the structure of the counterion cloud and results in both qualitative and quantitative changes of the force between highly <span class="hlt">charged</span> polyelectrolytes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/21419433-central-depression-nuclear-charge-density-distribution','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/21419433-central-depression-nuclear-charge-density-distribution"><span>Central depression of nuclear <span class="hlt">charge</span> density distribution</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>Chu Yanyun; Ren Zhongzhou; Center of Theoretical Nuclear Physics, National Laboratory of Heavy-Ion Accelerator, Lanzhou 730000</p> <p></p> <p>The center-depressed nuclear <span class="hlt">charge</span> distributions are investigated with the parametrized distribution and the relativistic mean-field theory, and their corresponding <span class="hlt">charge</span> form factors are worked out with the phase shift analysis method. The central depression of nuclear <span class="hlt">charge</span> distribution of {sup 46}Ar and {sup 44}S is supported by the relativistic mean-field calculation. According to the calculation, the valence protons in {sup 46}Ar and {sup 44}S prefer to occupy the 1d{sub 3/2} state rather than the 2s{sub 1/2} state, which is different from that in the less neutron-rich argon and sulfur isotopes. As a result, the central proton densities of {sup 46}Armore » and {sup 44}S are highly depressed, and so are their central <span class="hlt">charge</span> densities. The <span class="hlt">charge</span> form factors of some argon and sulfur isotopes are presented, and the minima of the <span class="hlt">charge</span> form factors shift upward and inward when the central nuclear <span class="hlt">charge</span> distributions are more depressed. Besides, the effect of the central depression on the <span class="hlt">charge</span> form factors is studied with a parametrized distribution, when the root-mean-square <span class="hlt">charge</span> radii remain constant.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/12563415','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/12563415"><span>The surface <span class="hlt">charge</span> of trypanosomatids.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Souto-Padrón, Thaïs</p> <p>2002-12-01</p> <p>The surface <span class="hlt">charge</span> 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 <span class="hlt">charged</span> 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 <span class="hlt">charge</span> of the trypanosomatids.</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 addition 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('https://www.gpo.gov/fdsys/pkg/CFR-2010-title20-vol2/pdf/CFR-2010-title20-vol2-sec410-692.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title20-vol2/pdf/CFR-2010-title20-vol2-sec410-692.pdf"><span>20 CFR 410.692 - Hearing on <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>2010-04-01</p> <p>..., Finality of Decisions, and Representation of Parties § 410.692 Hearing on <span class="hlt">charges</span>. (a) Hearing officer... the hearing shall be made and transcribed in all cases. (k) Representation. The individual <span class="hlt">charged</span> may... dismiss the <span class="hlt">charges</span> in the event of the death of the individual <span class="hlt">charged</span>. (n) Cost of transcript. On the...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5013471','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5013471"><span>Space <span class="hlt">Charge</span> Modulated Electrical Breakdown</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Li, Shengtao; Zhu, Yuanwei; Min, Daomin; Chen, George</p> <p>2016-01-01</p> <p>Electrical breakdown is one of the most important physical phenomena in electrical and electronic engineering. Since the early 20th century, many theories and models of electrical breakdown have been proposed, but the origin of one key issue, that the explanation for dc breakdown strength being twice or higher than ac breakdown strength in insulating materials, remains unclear. Here, by employing a bipolar <span class="hlt">charge</span> transport model, we investigate the space <span class="hlt">charge</span> dynamics in both dc and ac breakdown processes. We demonstrate the differences in <span class="hlt">charge</span> accumulations under both dc and ac stresses and estimate the breakdown strength, which is modulated by the electric field distortion induced by space <span class="hlt">charge</span>. It is concluded that dc breakdown initializes in the bulk whereas ac breakdown initializes in the vicinity of the sample-electrode interface. Compared with dc breakdown, the lower breakdown strength under ac stress and the decreasing breakdown strength with an increase in applied frequency, are both attributed to the electric field distortion induced by space <span class="hlt">charges</span> located in the vicinity of the electrodes. PMID:27599577</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=electrostatics&pg=3&id=EJ1083345','ERIC'); return false;" href="https://eric.ed.gov/?q=electrostatics&pg=3&id=EJ1083345"><span>Electrostatics with Computer-Interfaced <span class="hlt">Charge</span> Sensors</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>Morse, Robert A.</p> <p>2006-01-01</p> <p>Computer interfaced electrostatic <span class="hlt">charge</span> sensors allow both qualitative and quantitative measurements of electrostatic <span class="hlt">charge</span> but are quite sensitive to <span class="hlt">charges</span> accumulating on modern synthetic materials. They need to be used with care so that students can correctly interpret their measurements. This paper describes the operation of the sensors,…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4763780','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4763780"><span><span class="hlt">Charge</span> of a quasiparticle in a superconductor</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Ronen, Yuval; Cohen, Yonatan; Kang, Jung-Hyun; Haim, Arbel; Rieder, Maria-Theresa; Heiblum, Moty; Mahalu, Diana; Shtrikman, Hadas</p> <p>2016-01-01</p> <p>Nonlinear <span class="hlt">charge</span> transport in superconductor–insulator–superconductor (SIS) Josephson junctions has a unique signature in the shuttled <span class="hlt">charge</span> quantum between the two superconductors. In the zero-bias limit Cooper pairs, each with twice the electron <span class="hlt">charge</span>, carry the Josephson current. An applied bias VSD leads to multiple Andreev reflections (MAR), which in the limit of weak tunneling probability should lead to integer multiples of the electron <span class="hlt">charge</span> ne traversing the junction, with n integer larger than 2Δ/eVSD and Δ the superconducting order parameter. Exceptionally, just above the gap eVSD ≥ 2Δ, with Andreev reflections suppressed, one would expect the current to be carried by partitioned quasiparticles, each with energy-dependent <span class="hlt">charge</span>, being a superposition of an electron and a hole. Using shot-noise measurements in an SIS junction induced in an InAs nanowire (with noise proportional to the partitioned <span class="hlt">charge</span>), we first observed quantization of the partitioned <span class="hlt">charge</span> q = e*/e=n, with n = 1–4, thus reaffirming the validity of our <span class="hlt">charge</span> interpretation. Concentrating next on the bias region eVSD∼2Δ, we found a reproducible and clear dip in the extracted <span class="hlt">charge</span> to q ∼0.6, which, after excluding other possibilities, we attribute to the partitioned quasiparticle <span class="hlt">charge</span>. Such dip is supported by numerical simulations of our SIS structure. PMID:26831071</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26831071','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26831071"><span><span class="hlt">Charge</span> of a quasiparticle in a superconductor.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ronen, Yuval; Cohen, Yonatan; Kang, Jung-Hyun; Haim, Arbel; Rieder, Maria-Theresa; Heiblum, Moty; Mahalu, Diana; Shtrikman, Hadas</p> <p>2016-02-16</p> <p>Nonlinear <span class="hlt">charge</span> transport in superconductor-insulator-superconductor (SIS) Josephson junctions has a unique signature in the shuttled <span class="hlt">charge</span> quantum between the two superconductors. In the zero-bias limit Cooper pairs, each with twice the electron <span class="hlt">charge</span>, carry the Josephson current. An applied bias VSD leads to multiple Andreev reflections (MAR), which in the limit of weak tunneling probability should lead to integer multiples of the electron <span class="hlt">charge</span> ne traversing the junction, with n integer larger than 2Δ/eVSD and Δ the superconducting order parameter. Exceptionally, just above the gap eVSD ≥ 2Δ, with Andreev reflections suppressed, one would expect the current to be carried by partitioned quasiparticles, each with energy-dependent <span class="hlt">charge</span>, being a superposition of an electron and a hole. Using shot-noise measurements in an SIS junction induced in an InAs nanowire (with noise proportional to the partitioned <span class="hlt">charge</span>), we first observed quantization of the partitioned <span class="hlt">charge</span> q = e*/e = n, with n = 1-4, thus reaffirming the validity of our <span class="hlt">charge</span> interpretation. Concentrating next on the bias region eVSD ~ 2Δ, we found a reproducible and clear dip in the extracted <span class="hlt">charge</span> to q ~ 0.6, which, after excluding other possibilities, we attribute to the partitioned quasiparticle <span class="hlt">charge</span>. Such dip is supported by numerical simulations of our SIS structure.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015A%26A...583A..97A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015A%26A...583A..97A"><span>Simulating <span class="hlt">charge</span> transport to understand the spectral response of Swept <span class="hlt">Charge</span> Devices</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Athiray, P. S.; Sreekumar, P.; Narendranath, S.; Gow, J. P. D.</p> <p>2015-11-01</p> <p>Context. Swept <span class="hlt">Charge</span> Devices (SCD) are novel X-ray detectors optimized for improved spectral performance without any demand for active cooling. The Chandrayaan-1 X-ray Spectrometer (C1XS) experiment onboard the Chandrayaan-1 spacecraft used an array of SCDs to map the global surface elemental abundances on the Moon using the X-ray fluorescence (XRF) technique. The successful demonstration of SCDs in C1XS spurred an enhanced version of the spectrometer on Chandrayaan-2 using the next-generation SCD sensors. Aims: The objective of this paper is to demonstrate validation of a physical model developed to simulate X-ray photon interaction and <span class="hlt">charge</span> transportation in a SCD. The model helps to understand and identify the origin of individual components that collectively contribute to the energy-dependent spectral response of the SCD. Furthermore, the model provides completeness to various calibration tasks, such as generating spectral matrices (RMFs - redistribution matrix files), estimating efficiency, optimizing event selection logic, and maximizing event recovery to improve photon-collection efficiency in SCDs. Methods: <span class="hlt">Charge</span> generation and transportation in the SCD at different layers related to channel stops, field zones, and field-free zones due to photon interaction were computed using standard drift and diffusion equations. <span class="hlt">Charge</span> collected in the buried channel due to photon interaction in different volumes of the detector was computed by assuming a Gaussian radial profile of the <span class="hlt">charge</span> cloud. The collected <span class="hlt">charge</span> was processed further to simulate both diagonal clocking read-out, which is a novel design exclusive for SCDs, and event selection logic to construct the energy spectrum. Results: We compare simulation results of the SCD CCD54 with measurements obtained during the ground calibration of C1XS and clearly demonstrate that our model reproduces all the major spectral features seen in calibration data. We also describe our understanding of interactions at</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25181551','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25181551"><span>Surface <span class="hlt">charge</span> mapping with a nanopipette.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>McKelvey, Kim; Kinnear, Sophie L; Perry, David; Momotenko, Dmitry; Unwin, Patrick R</p> <p>2014-10-01</p> <p>Nanopipettes are emerging as simple but powerful tools for probing chemistry at the nanoscale. In this contribution the use of nanopipettes for simultaneous surface <span class="hlt">charge</span> mapping and topographical imaging is demonstrated, using a scanning ion conductance microscopy (SICM) format. When a nanopipette is positioned close to a surface in electrolyte solution, the direct ion current (DC), driven by an applied bias between a quasi-reference counter electrode (QRCE) in the nanopipette and a second QRCE in the bulk solution, is sensitive to surface <span class="hlt">charge</span>. The <span class="hlt">charge</span> sensitivity arises because the diffuse double layers at the nanopipette and the surface interact, creating a perm-selective region which becomes increasingly significant at low ionic strengths (10 mM 1:1 aqueous electrolyte herein). This leads to a polarity-dependent ion current and surface-induced rectification as the bias is varied. Using distance-modulated SICM, which induces an alternating ion current component (AC) by periodically modulating the distance between the nanopipette and the surface, the effect of surface <span class="hlt">charge</span> on the DC and AC is explored and rationalized. The impact of surface <span class="hlt">charge</span> on the AC phase (with respect to the driving sinusoidal signal) is highlighted in particular; this quantity shows a shift that is highly sensitive to interfacial <span class="hlt">charge</span> and provides the basis for visualizing <span class="hlt">charge</span> simultaneously with topography. The studies herein highlight the use of nanopipettes for functional imaging with applications from cell biology to materials characterization where understanding surface <span class="hlt">charge</span> is of key importance. They also provide a framework for the design of SICM experiments, which may be convoluted by topographical and surface <span class="hlt">charge</span> effects, especially for small nanopipettes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1350992','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1350992"><span>Network based management for multiplexed electric vehicle <span class="hlt">charging</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Gadh, Rajit; Chung, Ching Yen; Qui, Li</p> <p>2017-04-11</p> <p>A system for multiplexing <span class="hlt">charging</span> of electric vehicles, comprising a server coupled to a plurality of <span class="hlt">charging</span> control modules over a network. Each of said <span class="hlt">charging</span> modules being connected to a voltage source such that each <span class="hlt">charging</span> control module is configured to regulate distribution of voltage from the voltage source to an electric vehicle coupled to the <span class="hlt">charging</span> control module. Data collection and control software is provided on the server for identifying a plurality of electric vehicles coupled to the plurality of <span class="hlt">charging</span> control modules and selectively distributing <span class="hlt">charging</span> of the plurality of <span class="hlt">charging</span> control modules to multiplex distribution of voltage to the plurality of electric vehicles.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1360099-holographic-heavy-ion-collisions-baryon-charge','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1360099-holographic-heavy-ion-collisions-baryon-charge"><span>Holographic heavy ion collisions with baryon <span class="hlt">charge</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Casalderrey-Solana, Jorge; Mateos, David; van der Schee, Wilke; ...</p> <p>2016-09-19</p> <p>We numerically simulate collisions of <span class="hlt">charged</span> shockwaves in Einstein-Maxwell theory in anti-de Sitter space as a toy model of heavy ion collisions with non-zero baryon <span class="hlt">charge</span>. The stress tensor and the baryon current become well described by <span class="hlt">charged</span> hydrodynamics at roughly the same time. The effect of the <span class="hlt">charge</span> density on generic observables is typically no larger than 15%. Finally, we find significant stopping of the baryon <span class="hlt">charge</span> and compare our results with those in heavy ion collision experiments.</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.osti.gov/biblio/6854074','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/biblio/6854074"><span>Electrostatic wire stabilizing a <span class="hlt">charged</span> particle beam</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Prono, D.S.; Caporaso, G.J.; Briggs, R.J.</p> <p>1983-03-21</p> <p>In combination with a <span class="hlt">charged</span> particle beam generator and accelerator, apparatus and method are provided for stabilizing a beam of electrically <span class="hlt">charged</span> particles. A guiding means, disposed within the particle beam, has an electric <span class="hlt">charge</span> induced upon it by the <span class="hlt">charged</span> particle beam. Because the sign of the electric <span class="hlt">charge</span> on the guiding means and the sign of the particle beam are opposite, the particles are attracted toward and cluster around the guiding means to thereby stabilize the particle beam as it travels.</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 addition 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 addition 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('http://www.dtic.mil/docs/citations/ADA262778','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA262778"><span>Spacecraft Surface <span class="hlt">Charging</span> Handbook</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>1992-11-01</p> <p><span class="hlt">Charging</span> of Large Spwc Structure• . in Polut Otbil.’" Prweedings of thre Air For’e Grespykirs fitrano, W4r4 nop em Natural <span class="hlt">Charging</span> of large Space Stru, ures...3, p. 1433- 1440, 1991. Bowman, C., Bogorad, A., Brucker, G., Seehra, S., and Lloyd, T., "ITO-Coated RF Transparent Materials for Antenna Sunscreen</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016PhDT.......130D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016PhDT.......130D"><span><span class="hlt">Charged</span>-particle emission tomography</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ding, Yijun</p> <p></p> <p>Conventional <span class="hlt">charged</span>-particle imaging techniques--such as autoradiography-- provide only two-dimensional (2D) images of thin tissue slices. To get volumetric information, images of multiple thin slices are stacked. This process is time consuming and prone to distortions, as registration of 2D images is required. We propose a direct three-dimensional (3D) autoradiography technique, which we call <span class="hlt">charged</span>-particle emission tomography (CPET). This 3D imaging technique enables imaging of thick sections, thus increasing laboratory throughput and eliminating distortions due to registration. In CPET, molecules or cells of interest are labeled so that they emit <span class="hlt">charged</span> particles without significant alteration of their biological function. Therefore, by imaging the source of the <span class="hlt">charged</span> particles, one can gain information about the distribution of the molecules or cells of interest. Two special case of CPET include beta emission tomography (BET) and alpha emission tomography (alphaET), where the <span class="hlt">charged</span> particles employed are fast electrons and alpha particles, respectively. A crucial component of CPET is the <span class="hlt">charged</span>-particle detector. Conventional <span class="hlt">charged</span>-particle detectors are sensitive only to the 2-D positions of the detected particles. We propose a new detector concept, which we call particle-processing detector (PPD). A PPD measures attributes of each detected particle, including location, direction of propagation, and/or the energy deposited in the detector. Reconstruction algorithms for CPET are developed, and reconstruction results from simulated data are presented for both BET and alphaET. The results show that, in addition to position, direction and energy provide valuable information for 3D reconstruction of CPET. Several designs of particle-processing detectors are described. Experimental results for one detector are discussed. With appropriate detector design and careful data analysis, it is possible to measure direction and energy, as well as position of each</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20080005071','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20080005071"><span>Event-driven <span class="hlt">charge</span>-coupled device design and applications therefor</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Doty, John P. (Inventor); Ricker, Jr., George R. (Inventor); Burke, Barry E. (Inventor); Prigozhin, Gregory Y. (Inventor)</p> <p>2005-01-01</p> <p>An event-driven X-ray CCD imager device uses a floating-gate amplifier or other non-destructive readout device to non-destructively sense a <span class="hlt">charge</span> level in a <span class="hlt">charge</span> packet associated with a pixel. The output of the floating-gate amplifier is used to identify each pixel that has a <span class="hlt">charge</span> level above a predetermined threshold. If the <span class="hlt">charge</span> level is above a predetermined threshold the <span class="hlt">charge</span> in the triggering <span class="hlt">charge</span> packet and in the <span class="hlt">charge</span> packets from neighboring pixels need to be measured accurately. A <span class="hlt">charge</span> delay register is included in the event-driven X-ray CCD imager device to enable recovery of the <span class="hlt">charge</span> packets from neighboring pixels for accurate measurement. When a <span class="hlt">charge</span> packet reaches the end of the <span class="hlt">charge</span> delay register, control logic either dumps the <span class="hlt">charge</span> packet, or steers the <span class="hlt">charge</span> packet to a <span class="hlt">charge</span> FIFO to preserve it if the <span class="hlt">charge</span> packet is determined to be a packet that needs accurate measurement. A floating-diffusion amplifier or other low-noise output stage device, which converts <span class="hlt">charge</span> level to a voltage level with high precision, provides final measurement of the <span class="hlt">charge</span> packets. The voltage level is eventually digitized by a high linearity ADC.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140011621','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140011621"><span>An Investigation of Low Earth Orbit Internal <span class="hlt">Charging</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>NeergaardParker, Linda; Minow, Joseph I.; Willis, Emily M.</p> <p>2014-01-01</p> <p>Low Earth orbit is usually considered a relatively benign environment for internal <span class="hlt">charging</span> threats due to the low flux of penetrating electrons with energies of a few MeV that are encountered over an orbit. There are configurations, however, where insulators and ungrounded conductors used on the outside of a spacecraft hull may <span class="hlt">charge</span> when exposed to much lower energy electrons of some 100's keV in a process that is better characterized as internal <span class="hlt">charging</span> than surface <span class="hlt">charging</span>. For example, the minimal radiation shielding afforded by thin thermal control materials such as metalized polymer sheets (e.g., aluminized Kapton or Mylar) and multilayer insulation may allow electrons of 100's of keV to <span class="hlt">charge</span> underlying materials. Yet these same thermal control materials protect the underlying insulators and ungrounded conductors from surface <span class="hlt">charging</span> currents due to electrons and ions at energies less than a few keV as well as suppress the photoemission, secondary electron, and backscattered electron processes associated with surface <span class="hlt">charging</span>. We investigate the conditions required for this low Earth orbit "internal <span class="hlt">charging</span>" to occur and evaluate the environments for which the process may be a threat to spacecraft. First, we describe a simple one-dimensional internal <span class="hlt">charging</span> model that is used to compute the <span class="hlt">charge</span> accumulation on materials under thin shielding. Only the electron flux that penetrates exposed surface shielding material is considered and we treat the <span class="hlt">charge</span> balance in underlying insulation as a parallel plate capacitor accumulating <span class="hlt">charge</span> from the penetrating electron flux and losing <span class="hlt">charge</span> due to conduction to a ground plane. <span class="hlt">Charge</span> dissipation due to conduction can be neglected to consider the effects of <span class="hlt">charging</span> an ungrounded conductor. In both cases, the potential and electric field is computed as a function of time. An additional <span class="hlt">charge</span> loss process is introduced due to an electrostatic discharge current when the electric field reaches a</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title14-vol5/pdf/CFR-2013-title14-vol5-sec1215-113.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title14-vol5/pdf/CFR-2013-title14-vol5-sec1215-113.pdf"><span>14 CFR 1215.113 - User <span class="hlt">charges</span>.</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>... 14 Aeronautics and Space 5 2013-01-01 2013-01-01 false User <span class="hlt">charges</span>. 1215.113 Section 1215.113 Aeronautics and Space NATIONAL AERONAUTICS AND SPACE ADMINISTRATION TRACKING AND DATA RELAY SATELLITE SYSTEM... shall reimburse NASA the sum of the <span class="hlt">charges</span> for standard and mission-unique services. <span class="hlt">Charges</span> will be...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title12-vol3/pdf/CFR-2011-title12-vol3-sec226-4.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title12-vol3/pdf/CFR-2011-title12-vol3-sec226-4.pdf"><span>12 CFR 226.4 - Finance <span class="hlt">charge</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-01-01</p> <p>...) of this section: (1) Interest, time price differential, and any amount payable under an add-on or... any <span class="hlt">charge</span> imposed on a checking or other transaction account to the extent that the <span class="hlt">charge</span> exceeds... other credit loss. (6) <span class="hlt">Charges</span> imposed on a creditor by another person for purchasing or accepting a...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19670000446','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19670000446"><span>Battery <span class="hlt">charge</span> regulator is coulometer controlled</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Paulkovich, J.</p> <p>1967-01-01</p> <p>Coulometer controlled battery <span class="hlt">charge</span> regulator controls nickel/cadmium type primary cells used in space applications. The use of the coulometer as an ampere hour measuring device permits all available current to go to the battery until full <span class="hlt">charge</span> state is reached, at which time the <span class="hlt">charge</span> rate is automatically reduced.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title7-vol8/pdf/CFR-2014-title7-vol8-sec956-142.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title7-vol8/pdf/CFR-2014-title7-vol8-sec956-142.pdf"><span>7 CFR 956.142 - Interest <span class="hlt">charges</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-01-01</p> <p>... 7 Agriculture 8 2014-01-01 2014-01-01 false Interest <span class="hlt">charges</span>. 956.142 Section 956.142 Agriculture... VALLEY OF SOUTHEAST WASHINGTON AND NORTHEAST OREGON Rules and Regulations § 956.142 Interest <span class="hlt">charges</span>. For Walla Walla Sweet Onions handled prior to September 1, the Committee shall impose an interest <span class="hlt">charge</span> on...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title7-vol8/pdf/CFR-2013-title7-vol8-sec956-142.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title7-vol8/pdf/CFR-2013-title7-vol8-sec956-142.pdf"><span>7 CFR 956.142 - Interest <span class="hlt">charges</span>.</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 8 2013-01-01 2013-01-01 false Interest <span class="hlt">charges</span>. 956.142 Section 956.142 Agriculture... VALLEY OF SOUTHEAST WASHINGTON AND NORTHEAST OREGON Rules and Regulations § 956.142 Interest <span class="hlt">charges</span>. For Walla Walla Sweet Onions handled prior to September 1, the Committee shall impose an interest <span class="hlt">charge</span> on...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27488797','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27488797"><span>Controlling <span class="hlt">charge</span> quantization with quantum fluctuations.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Jezouin, S; Iftikhar, Z; Anthore, A; Parmentier, F D; Gennser, U; Cavanna, A; Ouerghi, A; Levkivskyi, I P; Idrisov, E; Sukhorukov, E V; Glazman, L I; Pierre, F</p> <p>2016-08-04</p> <p>In 1909, Millikan showed that the <span class="hlt">charge</span> of electrically isolated systems is quantized in units of the elementary electron <span class="hlt">charge</span> e. Today, the persistence of <span class="hlt">charge</span> quantization in small, weakly connected conductors allows for circuits in which single electrons are manipulated, with applications in, for example, metrology, detectors and thermometry. However, as the connection strength is increased, the discreteness of <span class="hlt">charge</span> is progressively reduced by quantum fluctuations. Here we report the full quantum control and characterization of <span class="hlt">charge</span> quantization. By using semiconductor-based tunable elemental conduction channels to connect a micrometre-scale metallic island to a circuit, we explore the complete evolution of <span class="hlt">charge</span> quantization while scanning the entire range of connection strengths, from a very weak (tunnel) to a perfect (ballistic) contact. We observe, when approaching the ballistic limit, that <span class="hlt">charge</span> quantization is destroyed by quantum fluctuations, and scales as the square root of the residual probability for an electron to be reflected across the quantum channel; this scaling also applies beyond the different regimes of connection strength currently accessible to theory. At increased temperatures, the thermal fluctuations result in an exponential suppression of <span class="hlt">charge</span> quantization and in a universal square-root scaling, valid for all connection strengths, in agreement with expectations. Besides being pertinent for the improvement of single-electron circuits and their applications, and for the metal-semiconductor hybrids relevant to topological quantum computing, knowledge of the quantum laws of electricity will be essential for the quantum engineering of future nanoelectronic devices.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title42-vol5/pdf/CFR-2010-title42-vol5-sec489-31.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title42-vol5/pdf/CFR-2010-title42-vol5-sec489-31.pdf"><span>42 CFR 489.31 - Allowable <span class="hlt">charges</span>: Blood.</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 5 2010-10-01 2010-10-01 false Allowable <span class="hlt">charges</span>: Blood. 489.31 Section 489.31... Allowable <span class="hlt">charges</span>: Blood. (a) Limitations on <span class="hlt">charges</span>. (1) A provider may <span class="hlt">charge</span> the beneficiary (or other person on his or her behalf) only for the first three pints of blood or units of packed red cells...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title42-vol5/pdf/CFR-2011-title42-vol5-sec489-31.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title42-vol5/pdf/CFR-2011-title42-vol5-sec489-31.pdf"><span>42 CFR 489.31 - Allowable <span class="hlt">charges</span>: Blood.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-10-01</p> <p>... 42 Public Health 5 2011-10-01 2011-10-01 false Allowable <span class="hlt">charges</span>: Blood. 489.31 Section 489.31... Allowable <span class="hlt">charges</span>: Blood. (a) Limitations on <span class="hlt">charges</span>. (1) A provider may <span class="hlt">charge</span> the beneficiary (or other person on his or her behalf) only for the first three pints of blood or units of packed red cells...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title42-vol5/pdf/CFR-2012-title42-vol5-sec489-31.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title42-vol5/pdf/CFR-2012-title42-vol5-sec489-31.pdf"><span>42 CFR 489.31 - Allowable <span class="hlt">charges</span>: Blood.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-10-01</p> <p>... 42 Public Health 5 2012-10-01 2012-10-01 false Allowable <span class="hlt">charges</span>: Blood. 489.31 Section 489.31... Allowable <span class="hlt">charges</span>: Blood. (a) Limitations on <span class="hlt">charges</span>. (1) A provider may <span class="hlt">charge</span> the beneficiary (or other person on his or her behalf) only for the first three pints of blood or units of packed red cells...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title42-vol5/pdf/CFR-2014-title42-vol5-sec489-31.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title42-vol5/pdf/CFR-2014-title42-vol5-sec489-31.pdf"><span>42 CFR 489.31 - Allowable <span class="hlt">charges</span>: Blood.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-10-01</p> <p>... 42 Public Health 5 2014-10-01 2014-10-01 false Allowable <span class="hlt">charges</span>: Blood. 489.31 Section 489.31... Allowable <span class="hlt">charges</span>: Blood. (a) Limitations on <span class="hlt">charges</span>. (1) A provider may <span class="hlt">charge</span> the beneficiary (or other person on his or her behalf) only for the first three pints of blood or units of packed red cells...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title42-vol5/pdf/CFR-2013-title42-vol5-sec489-31.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title42-vol5/pdf/CFR-2013-title42-vol5-sec489-31.pdf"><span>42 CFR 489.31 - Allowable <span class="hlt">charges</span>: Blood.</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>2013-10-01</p> <p>... 42 Public Health 5 2013-10-01 2013-10-01 false Allowable <span class="hlt">charges</span>: Blood. 489.31 Section 489.31... Allowable <span class="hlt">charges</span>: Blood. (a) Limitations on <span class="hlt">charges</span>. (1) A provider may <span class="hlt">charge</span> the beneficiary (or other person on his or her behalf) only for the first three pints of blood or units of packed red cells...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1240421','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1240421"><span>Distributed <span class="hlt">charging</span> of electrical assets</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Ghosh, Soumyadip; Phan, Dung; Sharma, Mayank; Wu, Chai Wah; Xiong, Jinjun</p> <p>2016-02-16</p> <p>The present disclosure relates generally to the field of distributed <span class="hlt">charging</span> of electrical assets. In various examples, distributed <span class="hlt">charging</span> of electrical assets may be implemented in the form of systems, methods and/or algorithms.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ghr.nlm.nih.gov/condition/charge-syndrome','NIH-MEDLINEPLUS'); return false;" href="https://ghr.nlm.nih.gov/condition/charge-syndrome"><span>Genetics Home Reference: <span class="hlt">CHARGE</span> syndrome</span></a></p> <p><a target="_blank" href="http://medlineplus.gov/">MedlinePlus</a></p> <p></p> <p></p> <p>... hormones that direct sexual development. As a result, males with <span class="hlt">CHARGE</span> syndrome are often born with an ... Puberty can be incomplete or delayed in affected males and females. Another minor feature of <span class="hlt">CHARGE</span> syndrome ...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27538341','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27538341"><span>What Controls the Rate of Ultrafast <span class="hlt">Charge</span> Transfer and <span class="hlt">Charge</span> Separation Efficiency in Organic Photovoltaic Blends.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Jakowetz, Andreas C; Böhm, Marcus L; Zhang, Jiangbin; Sadhanala, Aditya; Huettner, Sven; Bakulin, Artem A; Rao, Akshay; Friend, Richard H</p> <p>2016-09-14</p> <p>In solar energy harvesting devices based on molecular semiconductors, such as organic photovoltaics (OPVs) and artificial photosynthetic systems, Frenkel excitons must be dissociated via <span class="hlt">charge</span> transfer at heterojunctions to yield free <span class="hlt">charges</span>. What controls the rate and efficiency of <span class="hlt">charge</span> transfer and <span class="hlt">charge</span> separation is an important question, as it determines the overall power conversion efficiency (PCE) of these systems. In bulk heterojunctions between polymer donor and fullerene acceptors, which provide a model system to understand the fundamental dynamics of electron transfer in molecular systems, it has been established that the first step of photoinduced electron transfer can be fast, of order 100 fs. But here we report the first study which correlates differences in the electron transfer rate with electronic structure and morphology, achieved with sub-20 fs time resolution pump-probe spectroscopy. We vary both the fullerene substitution and donor/fullerene ratio which allow us to control both aggregate size and the energetic driving force for <span class="hlt">charge</span> transfer. We observe a range of electron transfer times from polymer to fullerene, from 240 fs to as short as 37 fs. Using ultrafast electro-optical pump-push-photocurrent spectroscopy, we find the yield of free versus bound <span class="hlt">charges</span> to be weakly dependent on the energetic driving force, but to be very strongly dependent on fullerene aggregate size and packing. Our results point toward the importance of state accessibility and <span class="hlt">charge</span> delocalization and suggest that energetic offsets between donor and acceptor levels are not an important criterion for efficient <span class="hlt">charge</span> generation. This provides design rules for next-generation materials to minimize losses related to driving energy and boost PCE.</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('http://adsabs.harvard.edu/abs/2017CP....482...52S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017CP....482...52S"><span>Using quantum dynamics simulations to follow the competition between <span class="hlt">charge</span> migration and <span class="hlt">charge</span> transfer in polyatomic molecules</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Spinlove, K. E.; Vacher, M.; Bearpark, M.; Robb, M. A.; Worth, G. A.</p> <p>2017-01-01</p> <p>Recent work, particularly by Cederbaum and co-workers, has identified the phenomenon of <span class="hlt">charge</span> migration, whereby <span class="hlt">charge</span> flow occurs over a static molecular framework after the creation of an electronic wavepacket. In a real molecule, this <span class="hlt">charge</span> migration competes with <span class="hlt">charge</span> transfer, whereby the nuclear motion also results in the re-distribution of <span class="hlt">charge</span>. To study this competition, quantum dynamics simulations need to be performed. To break the exponential scaling of standard grid-based algorithms, approximate methods need to be developed that are efficient yet able to follow the coupled electronic-nuclear motion of these systems. Using a simple model Hamiltonian based on the ionisation of the allene molecule, the performance of different methods based on Gaussian Wavepackets is demonstrated.</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 addition 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('https://www.gpo.gov/fdsys/pkg/CFR-2010-title47-vol5/pdf/CFR-2010-title47-vol5-sec80-95.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title47-vol5/pdf/CFR-2010-title47-vol5-sec80-95.pdf"><span>47 CFR 80.95 - Message <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>... <span class="hlt">charges</span>. (a) Except as specified in § 20.15(c) of this chapter with respect to commercial mobile radio service providers, <span class="hlt">charges</span> must not be made for service of: (1) Any public coast station unless tariffs... 47 Telecommunication 5 2010-10-01 2010-10-01 false Message <span class="hlt">charges</span>. 80.95 Section 80.95...</p> </li> <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 negatively <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('https://www.ncbi.nlm.nih.gov/pubmed/20869721','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20869721"><span>The pH-dependent surface <span class="hlt">charging</span> and points of zero <span class="hlt">charge</span>: V. Update.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kosmulski, Marek</p> <p>2011-01-01</p> <p>The points of zero <span class="hlt">charge</span> (PZC) and isoelectric points (IEP) from the recent literature are discussed. This study is an update of the previous compilation [M. Kosmulski, Surface <span class="hlt">Charging</span> and Points of Zero <span class="hlt">Charge</span>, CRC, Boca Raton, FL, 2009] and of its previous update [J. Colloid Interface Sci. 337 (2009) 439]. In several recent publications, the terms PZC/IEP have been used outside their usual meaning. Only the PZC/IEP obtained according to the methods recommended by the present author are reported in this paper, and the other results are ignored. PZC/IEP of albite, sepiolite, and sericite, which have not been studied before, became available over the past 2 years. Copyright © 2010 Elsevier Inc. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=10587&hterms=exchange&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dexchange','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=10587&hterms=exchange&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dexchange"><span><span class="hlt">Charge</span> and Exchange</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p></p> <p>2008-01-01</p> <p>Even though comets are basically giant dirty snowballs, a few years ago they surprised astronomers by emitting X-radiation. These X-rays are not produced by multi-million degree gas (as is often the case) but rather by a process called '<span class="hlt">charge</span> exchange'. In this process, ionized atoms (which have lost one or more electrons) which are carried within the solar wind collide with neutral atoms in the comet's coma. The solar wind ion can collide with and capture an electron from the neutral comet atom, and in doing so some of the energy of the collision is observed in the form of X-rays. This produces a glow of X-rays on the sunward side of the comet's atmosphere. <span class="hlt">Charge</span> exchange can occur in a variety of astrophysical settings, and cometary <span class="hlt">charge</span> exchange provides astronomers a means to study this process up close. The image above is a pretty picture of comet 73P/Schwassmann-Wachmann 3 passing by the Ring Nebula. This image was obtained by the ultraviolet and optical telescope (UVOT) on the Swift gamma-ray burst hunter. The UVOT observations help astronomers to study the structure and chemistry of the comet, while Swift's X-ray Telescope (XRT) simultaneously monitors the <span class="hlt">charge</span> exchange process. Comet 73P/Schwassmann-Wachmann 3 is currently in the process of breaking up, and the UVOT observations show important details of how this breakup is occurring.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/868095','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/868095"><span>Detection method for dissociation of multiple-<span class="hlt">charged</span> ions</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Smith, Richard D.; Udseth, Harold R.; Rockwood, Alan L.</p> <p>1991-01-01</p> <p>Dissociations of multiple-<span class="hlt">charged</span> ions are detected and analyzed by <span class="hlt">charge</span>-separation tandem mass spectrometry. Analyte molecules are ionized to form multiple-<span class="hlt">charged</span> parent ions. A particular <span class="hlt">charge</span> parent ion state is selected in a first-stage mass spectrometer and its mass-to-<span class="hlt">charge</span> ratio (M/Z) is detected to determine its mass and <span class="hlt">charge</span>. The selected parent ions are then dissociated, each into a plurality of fragments including a set of daughter ions each having a mass of at least one molecular weight and a <span class="hlt">charge</span> of at least one. Sets of daughter ions resulting from the dissociation of one parent ion (sibling ions) vary in number but typically include two to four ions, one or more multiply-<span class="hlt">charged</span>. A second stage mass spectrometer detects mass-to-<span class="hlt">charge</span> ratio (m/z) of the daughter ions and a temporal or temporo-spatial relationship among them. This relationship is used to correlate the daughter ions to determine which (m/z) ratios belong to a set of sibling ions. Values of mass and <span class="hlt">charge</span> of each of the sibling ions are determined simultaneously from their respective (m/z) ratios such that the sibling ion <span class="hlt">charges</span> are integers and sum to the parent ion <span class="hlt">charge</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title36-vol1/pdf/CFR-2013-title36-vol1-sec10-2.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title36-vol1/pdf/CFR-2013-title36-vol1-sec10-2.pdf"><span>36 CFR 10.2 - <span class="hlt">Charges</span>.</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>2013-07-01</p> <p>... services of a veterinarian for testing, vaccinating, and treating the animals at the park for communicable... CERTAIN WILD ANIMALS § 10.2 <span class="hlt">Charges</span>. No <span class="hlt">charge</span> will be made for the animals, but the receiver will be...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title36-vol1/pdf/CFR-2012-title36-vol1-sec10-2.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title36-vol1/pdf/CFR-2012-title36-vol1-sec10-2.pdf"><span>36 CFR 10.2 - <span class="hlt">Charges</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-07-01</p> <p>... services of a veterinarian for testing, vaccinating, and treating the animals at the park for communicable... CERTAIN WILD ANIMALS § 10.2 <span class="hlt">Charges</span>. No <span class="hlt">charge</span> will be made for the animals, but the receiver will be...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title36-vol1/pdf/CFR-2011-title36-vol1-sec10-2.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title36-vol1/pdf/CFR-2011-title36-vol1-sec10-2.pdf"><span>36 CFR 10.2 - <span class="hlt">Charges</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-07-01</p> <p>... services of a veterinarian for testing, vaccinating, and treating the animals at the park for communicable... CERTAIN WILD ANIMALS § 10.2 <span class="hlt">Charges</span>. No <span class="hlt">charge</span> will be made for the animals, but the receiver will be...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title36-vol1/pdf/CFR-2014-title36-vol1-sec10-2.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title36-vol1/pdf/CFR-2014-title36-vol1-sec10-2.pdf"><span>36 CFR 10.2 - <span class="hlt">Charges</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-07-01</p> <p>... services of a veterinarian for testing, vaccinating, and treating the animals at the park for communicable... CERTAIN WILD ANIMALS § 10.2 <span class="hlt">Charges</span>. No <span class="hlt">charge</span> will be made for the animals, but the receiver will be...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title36-vol1/pdf/CFR-2010-title36-vol1-sec10-2.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title36-vol1/pdf/CFR-2010-title36-vol1-sec10-2.pdf"><span>36 CFR 10.2 - <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>2010-07-01</p> <p>... services of a veterinarian for testing, vaccinating, and treating the animals at the park for communicable... CERTAIN WILD ANIMALS § 10.2 <span class="hlt">Charges</span>. No <span class="hlt">charge</span> will be made for the animals, but the receiver will be...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title12-vol5/pdf/CFR-2010-title12-vol5-sec535-4.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title12-vol5/pdf/CFR-2010-title12-vol5-sec535-4.pdf"><span>12 CFR 535.4 - Late <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>2010-01-01</p> <p>... delinquency <span class="hlt">charge</span> on a payment, which payment is otherwise a full payment for the applicable period and is paid on its due date or within an applicable grace period, when the only delinquency is attributable to late fee(s) or delinquency <span class="hlt">charge(s</span>) assessed on earlier installment(s). (b) For the purposes of this...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title22-vol2/pdf/CFR-2010-title22-vol2-sec901-17.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title22-vol2/pdf/CFR-2010-title22-vol2-sec901-17.pdf"><span>22 CFR 901.17 - <span class="hlt">Charged</span> employee.</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>2010-04-01</p> <p>... 22 Foreign Relations 2 2010-04-01 2010-04-01 true <span class="hlt">Charged</span> employee. 901.17 Section 901.17 Foreign Relations FOREIGN SERVICE GRIEVANCE BOARD GENERAL Meanings of Terms As Used in This Chapter § 901.17 <span class="hlt">Charged</span> employee. <span class="hlt">Charged</span> employee means a member of the Senior Foreign Service or a member of the Service assigned...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title12-vol8/pdf/CFR-2013-title12-vol8-sec1026-4.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title12-vol8/pdf/CFR-2013-title12-vol8-sec1026-4.pdf"><span>12 CFR 1026.4 - Finance <span class="hlt">charge</span>.</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>... 12 Banks and Banking 8 2013-01-01 2013-01-01 false Finance <span class="hlt">charge</span>. 1026.4 Section 1026.4 Banks and Banking BUREAU OF CONSUMER FINANCIAL PROTECTION TRUTH IN LENDING (REGULATION Z) General § 1026.4 Finance <span class="hlt">charge</span>. (a) Definition. The finance <span class="hlt">charge</span> is the cost of consumer credit as a dollar amount. It includes...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title12-vol8/pdf/CFR-2012-title12-vol8-sec1026-4.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title12-vol8/pdf/CFR-2012-title12-vol8-sec1026-4.pdf"><span>12 CFR 1026.4 - Finance <span class="hlt">charge</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-01-01</p> <p>... 12 Banks and Banking 8 2012-01-01 2012-01-01 false Finance <span class="hlt">charge</span>. 1026.4 Section 1026.4 Banks and Banking BUREAU OF CONSUMER FINANCIAL PROTECTION TRUTH IN LENDING (REGULATION Z) General § 1026.4 Finance <span class="hlt">charge</span>. (a) Definition. The finance <span class="hlt">charge</span> is the cost of consumer credit as a dollar amount. It includes...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title12-vol9/pdf/CFR-2014-title12-vol9-sec1026-4.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title12-vol9/pdf/CFR-2014-title12-vol9-sec1026-4.pdf"><span>12 CFR 1026.4 - Finance <span class="hlt">charge</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-01-01</p> <p>... 12 Banks and Banking 9 2014-01-01 2014-01-01 false Finance <span class="hlt">charge</span>. 1026.4 Section 1026.4 Banks and Banking BUREAU OF CONSUMER FINANCIAL PROTECTION TRUTH IN LENDING (REGULATION Z) § 1026.4 Finance <span class="hlt">charge</span>. (a) Definition. The finance <span class="hlt">charge</span> is the cost of consumer credit as a dollar amount. It includes any...</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. Negatively <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.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4726152','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4726152"><span><span class="hlt">Charge</span> carrier thermalization in organic diodes</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>van der Kaap, N. J.; Koster, L. J. A.</p> <p>2016-01-01</p> <p><span class="hlt">Charge</span> carrier mobilities of organic semiconductors are often characterized using steady-state measurements of space <span class="hlt">charge</span> limited diodes. These measurements assume that <span class="hlt">charge</span> carriers are in a steady-state equilibrium. In reality, however, energetically hot carriers are introduces by photo-excitation and injection into highly energetic sites from the electrodes. These carriers perturb the equilibrium density of occupied states, and therefore change the overall <span class="hlt">charge</span> transport properties. In this paper, we look into the effect of energetically hot carriers on the <span class="hlt">charge</span> transport in organic semiconductors using steady state kinetic Monte Carlo simulations. For injected hot carriers in a typical organic semiconductor, rapid energetic relaxation occurs in the order of tens of nanoseconds, which is much faster than the typical transit time of a <span class="hlt">charge</span> carrier throught the device. Furthermore, we investigate the impact of photo-generated carriers on the steady-state mobility. For a typical organic voltaic material, an increase in mobility of a factor of 1.1 is found. Therefore, we conclude that the impact of energetically hot carriers on normal device operation is limited. PMID:26791095</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29566508','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29566508"><span>Weak polyelectrolyte complexation driven by associative <span class="hlt">charging</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Rathee, Vikramjit S; Zervoudakis, Aristotle J; Sidky, Hythem; Sikora, Benjamin J; Whitmer, Jonathan K</p> <p>2018-03-21</p> <p>Weak polyelectrolytes are relevant for a wide range of fields; in particular, they have been investigated as "smart" materials for chemical separations and drug delivery. The <span class="hlt">charges</span> on weak polyelectrolytes are dynamic, causing polymer chains to adopt different equilibrium conformations even with relatively small changes to the surrounding environment. Currently, there exists no comprehensive picture of this behavior, particularly where polymer-polymer interactions have the potential to affect <span class="hlt">charging</span> properties significantly. In this study, we elucidate the novel interplay between weak polyelectrolyte <span class="hlt">charging</span> and complexation behavior through coupled molecular dynamics and Monte Carlo simulations. Specifically, we investigate a model of two equal-length and oppositely <span class="hlt">charging</span> polymer chains in an implicit salt solution represented through Debye-Hückel interactions. The <span class="hlt">charging</span> tendency of each chain, along with the salt concentration, is varied to determine the existence and extent of cooperativity in <span class="hlt">charging</span> and complexation. Strong cooperation in the <span class="hlt">charging</span> of these chains is observed at large Debye lengths, corresponding to low salt concentrations, while at lower Debye lengths (higher salt concentrations), the chains behave in apparent isolation. When the electrostatic coupling is long-ranged, we find that a highly <span class="hlt">charged</span> chain strongly promotes the <span class="hlt">charging</span> of its partner chain, even if the environment is unfavorable for an isolated version of that partner chain. Evidence of this phenomenon is supported by a drop in the potential energy of the system, which does not occur at the lower Debye lengths where both potential energies and <span class="hlt">charge</span> fractions converge for all partner chain <span class="hlt">charging</span> tendencies. The discovery of this cooperation will be helpful in developing "smart" drug delivery mechanisms by allowing for better predictions for the dissociation point of delivery complexes.</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/2018JChPh.148k4901R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JChPh.148k4901R"><span>Weak polyelectrolyte complexation driven by associative <span class="hlt">charging</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rathee, Vikramjit S.; Zervoudakis, Aristotle J.; Sidky, Hythem; Sikora, Benjamin J.; Whitmer, Jonathan K.</p> <p>2018-03-01</p> <p>Weak polyelectrolytes are relevant for a wide range of fields; in particular, they have been investigated as "smart" materials for chemical separations and drug delivery. The <span class="hlt">charges</span> on weak polyelectrolytes are dynamic, causing polymer chains to adopt different equilibrium conformations even with relatively small changes to the surrounding environment. Currently, there exists no comprehensive picture of this behavior, particularly where polymer-polymer interactions have the potential to affect <span class="hlt">charging</span> properties significantly. In this study, we elucidate the novel interplay between weak polyelectrolyte <span class="hlt">charging</span> and complexation behavior through coupled molecular dynamics and Monte Carlo simulations. Specifically, we investigate a model of two equal-length and oppositely <span class="hlt">charging</span> polymer chains in an implicit salt solution represented through Debye-Hückel interactions. The <span class="hlt">charging</span> tendency of each chain, along with the salt concentration, is varied to determine the existence and extent of cooperativity in <span class="hlt">charging</span> and complexation. Strong cooperation in the <span class="hlt">charging</span> of these chains is observed at large Debye lengths, corresponding to low salt concentrations, while at lower Debye lengths (higher salt concentrations), the chains behave in apparent isolation. When the electrostatic coupling is long-ranged, we find that a highly <span class="hlt">charged</span> chain strongly promotes the <span class="hlt">charging</span> of its partner chain, even if the environment is unfavorable for an isolated version of that partner chain. Evidence of this phenomenon is supported by a drop in the potential energy of the system, which does not occur at the lower Debye lengths where both potential energies and <span class="hlt">charge</span> fractions converge for all partner chain <span class="hlt">charging</span> tendencies. The discovery of this cooperation will be helpful in developing "smart" drug delivery mechanisms by allowing for better predictions for the dissociation point of delivery complexes.</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 negative <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('http://adsabs.harvard.edu/abs/2014PhRvS..17l3501K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014PhRvS..17l3501K"><span><span class="hlt">Charge</span> state distribution of 86Kr in hydrogen and helium gas <span class="hlt">charge</span> strippers at 2.7 MeV /nucleon</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kuboki, H.; Okuno, H.; Hasebe, H.; Fukunishi, N.; Ikezawa, E.; Imao, H.; Kamigaito, O.; Kase, M.</p> <p>2014-12-01</p> <p>The <span class="hlt">charge</span> state distributions of krypton (86Kr) with an energy of 2.7 MeV /nucleon were measured using hydrogen (H2 ) and helium (He) gas <span class="hlt">charge</span> strippers. A differential pumping system was constructed to confine H2 and He gases to a thickness sufficient for the <span class="hlt">charge</span> state distributions to attain equilibrium. The mean <span class="hlt">charge</span> states of 86Kr in H2 and He gases attained equilibrium at 25.1 and 23.2, respectively, whereas the mean <span class="hlt">charge</span> state in N2 gas at equilibrium was estimated to be less than 20. The <span class="hlt">charge</span> distributions are successfully reproduced by the cross sections of ionization and electron capture processes optimized by a fitting procedure.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1247645','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1247645"><span>Emissions Associated with Electric Vehicle <span class="hlt">Charging</span>: Impact of Electricity Generation Mix, <span class="hlt">Charging</span> Infrastructure Availability, and Vehicle Type</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>McLaren, Joyce; Miller, John; O'Shaughnessy, Eric</p> <p></p> <p>With the aim of reducing greenhouse gas emissions associated with the transportation sector, policy-makers are supporting a multitude of measures to increase electric vehicle adoption. The actual level of emission reduction associated with the electrification of the transport sector is dependent on the contexts that determine when and where drivers <span class="hlt">charge</span> electric vehicles. This analysis contributes to our understanding of the degree to which a particular electricity grid profile, vehicle type, and <span class="hlt">charging</span> patterns impact CO2 emissions from light-duty, plug-in electric vehicles. We present an analysis of emissions resulting from both battery electric and plug-in hybrid electric vehicles for fourmore » <span class="hlt">charging</span> scenarios and five electricity grid profiles. A scenario that allows drivers to <span class="hlt">charge</span> electric vehicles at the workplace yields the lowest level of emissions for the majority of electricity grid profiles. However, vehicle emissions are shown to be highly dependent on the percentage of fossil fuels in the grid mix, with different vehicle types and <span class="hlt">charging</span> scenarios resulting in fewer emissions when the carbon intensity of the grid is above a defined level. Restricting <span class="hlt">charging</span> to off-peak hours results in higher total emissions for all vehicle types, as compared to other <span class="hlt">charging</span> scenarios.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1390898-combining-electronic-geometric-effects-zno-promoted-pt-nanocatalysts-aqueous-phase-reforming-propanol','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1390898-combining-electronic-geometric-effects-zno-promoted-pt-nanocatalysts-aqueous-phase-reforming-propanol"><span>Combining Electronic and Geometric Effects of ZnO-Promoted Pt Nanocatalysts for Aqueous Phase Reforming of 1-Propanol</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Lei, Yu; Lee, Sungsik; Low, Ke -Bin; ...</p> <p>2016-04-26</p> <p>Compared with Pt/Al 2O 3, sintering-resistant Pt nanoparticle catalysts promoted by ZnO significantly improved the reactivity and selectivity toward hydrogen formation in the aqueous phase reforming (<span class="hlt">APR</span>) of 1-propanol. The improved performance was found to benefit from both the electronic and geometric effects of ZnO thin films. In situ small-angle X-ray scattering and scanning transmission electron microscopy showed that ZnO-promoted Pt possessed promising thermal stability under <span class="hlt">APR</span> reaction conditions. In situ X-ray absorption spectroscopy showed clear <span class="hlt">charge</span> transfer between ZnO and Pt nanoparticles. The improved reactivity and selectivity seemed to benefit from having both Pt-ZnO and Pt-Al 2O 3 interfaces.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2001JPS...101..158Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2001JPS...101..158Y"><span>Fast <span class="hlt">charging</span> nickel-metal hydride traction batteries</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yang, Xiao Guang; Liaw, Bor Yann</p> <p></p> <p>This paper describes the fast <span class="hlt">charge</span> ability, or "fast rechargeability", of nominal 85 Ah Ni-MH modules under various fast <span class="hlt">charge</span> conditions, including constant current (CC); typically 1-3C, and constant power (CP) regimes. Our tests revealed that there is no apparent difference between CC and CP fast <span class="hlt">charge</span> regimes with respect to <span class="hlt">charge</span> efficiency and time. Following the USABC Electric Vehicle Battery Test Procedures Manual (Revision 2, 1996), we demonstrated that we were able to return 40% state of <span class="hlt">charge</span> (SOC) from 60% depth of discharge (DOD) to 20% DOD within 15 min. Most importantly, we found that the internal pressure of the cell is the most critical parameter in the control of the fast <span class="hlt">charge</span> process and the safe operation of the modules.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19840020506','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19840020506"><span>Apparatus for measuring <span class="hlt">charged</span> particle beam</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gregory, D. A.; Stocks, C. D. (Inventor)</p> <p>1984-01-01</p> <p>An apparatus to measure the incident <span class="hlt">charged</span> particle beam flux while effectively eliminating losses to reflection and/or secondary emission of the <span class="hlt">charged</span> particle beam being measured is described. It comprises a sense cup through which the <span class="hlt">charged</span> particle beam enters. A sense cone forms the rear wall of the interior chamber with the cone apex adjacent the entry opening. An outer case surrounds the sense cup and is electrically insulated therefrom. <span class="hlt">Charged</span> particles entering the interior chamber are trapped and are absorbed by the sense cup and cone and travel through a current measuring device to ground.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19100868','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19100868"><span>Role of protein surface <span class="hlt">charge</span> in monellin sweetness.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Xue, Wei-Feng; Szczepankiewicz, Olga; Thulin, Eva; Linse, Sara; Carey, Jannette</p> <p>2009-03-01</p> <p>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 <span class="hlt">charged</span> residues in sweetness. In the present work, the effect of overall net <span class="hlt">charge</span> was investigated using the complementary approach of negative <span class="hlt">charge</span> alterations. Multiple substitutions of Asp/Asn and Glu/Gln residues radically altered the surface <span class="hlt">charge</span> of single-chain monellin by removing six negative <span class="hlt">charges</span> or adding four negative <span class="hlt">charges</span>. 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 <span class="hlt">charges</span> preserves monellin sweetness, whereas added negative <span class="hlt">charge</span> has a large negative impact on sweetness. Meta-analysis of published <span class="hlt">charge</span> variants of monellin and other sweet proteins reveals a general trend toward increasing sweetness with increasing positive net <span class="hlt">charge</span>. Structural mapping of monellin variants identifies a hydrophobic surface predicted to face the receptor where introduced positive or negative <span class="hlt">charge</span> reduces sweetness, and a polar surface where <span class="hlt">charges</span> modulate long-range electrostatic complementarity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016APS..GECET1005H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016APS..GECET1005H"><span><span class="hlt">Charging</span> of particles on a surface</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Heijmans, Lucas; Nijdam, Sander</p> <p>2016-09-01</p> <p>This contribution focusses on the seemingly easy problem of the <span class="hlt">charging</span> of micrometer sized particles on a substrate in a plasma. This seems trivial, because much is known about both the <span class="hlt">charging</span> of surfaces near a plasma and of particles in the plasma bulk. The problem, however, becomes much more complicated when the particle is on the substrate surface. The <span class="hlt">charging</span> currents to the particle are then highly altered by the substrate plasma sheath. Currently there is no consensus in literature about the resulting particle <span class="hlt">charge</span>. We shall present both experimental measurements and numerical simulations of the <span class="hlt">charge</span> on these particles. The experimental results are acquired by measuring the particle acceleration in an external electric field. For the simulations we have used our specially developed model. We shall compare these results to other estimates found in literature.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19800011422','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19800011422"><span>Fog dispersion. [<span class="hlt">charged</span> particle technique</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Christensen, L. S.; Frost, W.</p> <p>1980-01-01</p> <p>The concept of using the <span class="hlt">charged</span> particle technique to disperse warm fog at airports is investigated and compared with other techniques. The <span class="hlt">charged</span> particle technique shows potential for warm fog dispersal, but experimental verification of several significant parameters, such as particle mobility and <span class="hlt">charge</span> density, is needed. Seeding and helicopter downwash techniques are also effective for warm fog disperals, but presently are not believed to be viable techniques for routine airport operations. Thermal systems are currently used at a few overseas airports; however, they are expensive and pose potential environmental problems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017MS%26E..199a2041Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017MS%26E..199a2041Y"><span>Economic Analysis of Different Electric Vehicle <span class="hlt">Charging</span> Scenarios</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ying, Li; Haiming, Zhou; Xiufan, Ma; Hao, Wang</p> <p>2017-05-01</p> <p>Influence of electric vehicles (EV) to grid cannot be ignored. Research on the economy analysis of different <span class="hlt">charging</span> scenarios is helpful to guide the user to <span class="hlt">charge</span> or discharge orderly. EV <span class="hlt">charging</span> models are built such as disordered <span class="hlt">charging</span>, valley <span class="hlt">charging</span>, intelligent <span class="hlt">charging</span>, and V2G (Vehicle to Grid), by which changes of <span class="hlt">charging</span> load in different scenarios can be seen to analyze the influence to initial load curve, and comparison can be done about user’s average cost. Monte Carlo method is used to simulate the electric vehicle <span class="hlt">charging</span> behavior, cost in different <span class="hlt">charging</span> scenarios are compared, social cost is introduced in V2G scene, and the relationship between user’s average cost and social cost is analyzed. By test, it is proved that user’s cost is the lowest in V2G scenario, and the larger the scale of vehicles is, the more the social cost can save.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19780002201','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19780002201"><span>Modeling of spacecraft <span class="hlt">charging</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Whipple, E. C., Jr.</p> <p>1977-01-01</p> <p>Three types of modeling of spacecraft <span class="hlt">charging</span> are discussed: statistical models, parametric models, and physical models. Local time dependence of circuit upset for DoD and communication satellites, and electron current to a sphere with an assumed Debye potential distribution are presented. Four regions were involved in spacecraft <span class="hlt">charging</span>: (1) undisturbed plasma, (2) plasma sheath region, (3) spacecraft surface, and (4) spacecraft equivalent circuit.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title12-vol3/pdf/CFR-2010-title12-vol3-sec226-4.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title12-vol3/pdf/CFR-2010-title12-vol3-sec226-4.pdf"><span>12 CFR 226.4 - Finance <span class="hlt">charge</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>2010-01-01</p> <p>... 12 Banks and Banking 3 2010-01-01 2010-01-01 false Finance <span class="hlt">charge</span>. 226.4 Section 226.4 Banks and Banking FEDERAL RESERVE SYSTEM (CONTINUED) BOARD OF GOVERNORS OF THE FEDERAL RESERVE SYSTEM TRUTH IN LENDING (REGULATION Z) General § 226.4 Finance <span class="hlt">charge</span>. (a) Definition. The finance <span class="hlt">charge</span> is the cost of consumer credit as a dollar amount. It...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/870170','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/870170"><span>Circular, confined distribution for <span class="hlt">charged</span> particle beams</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Garnett, Robert W.; Dobelbower, M. Christian</p> <p>1995-01-01</p> <p>A <span class="hlt">charged</span> particle beam line is formed with magnetic optics that manipulate the <span class="hlt">charged</span> particle beam to form the beam having a generally rectangular configuration to a circular beam cross-section having a uniform particle distribution at a predetermined location. First magnetic optics form a <span class="hlt">charged</span> particle beam to a generally uniform particle distribution over a square planar area at a known first location. Second magnetic optics receive the <span class="hlt">charged</span> particle beam with the generally square configuration and affect the <span class="hlt">charged</span> particle beam to output the <span class="hlt">charged</span> particle beam with a phase-space distribution effective to fold corner portions of the beam toward the core region of the beam. The beam forms a circular configuration having a generally uniform spatial particle distribution over a target area at a predetermined second location.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/131939','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/biblio/131939"><span>Circular, confined distribution for <span class="hlt">charged</span> particle beams</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Garnett, R.W.; Dobelbower, M.C.</p> <p>1995-11-21</p> <p>A <span class="hlt">charged</span> particle beam line is formed with magnetic optics that manipulate the <span class="hlt">charged</span> particle beam to form the beam having a generally rectangular configuration to a circular beam cross-section having a uniform particle distribution at a predetermined location. First magnetic optics form a <span class="hlt">charged</span> particle beam to a generally uniform particle distribution over a square planar area at a known first location. Second magnetic optics receive the <span class="hlt">charged</span> particle beam with the generally square configuration and affect the <span class="hlt">charged</span> particle beam to output the <span class="hlt">charged</span> particle beam with a phase-space distribution effective to fold corner portions of the beam toward the core region of the beam. The beam forms a circular configuration having a generally uniform spatial particle distribution over a target area at a predetermined second location. 26 figs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1998AIPC..454..117W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1998AIPC..454..117W"><span><span class="hlt">Charge</span> transfer and <span class="hlt">charge</span> localization in extended radical cations: Investigation of model molecules for peptides</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Weinkauf, Rainer; Lehrer, Florian</p> <p>1998-12-01</p> <p>Molecules consisting of a flexible tail and an aromatic chromophore are used as model systems to understand the situation of a single chromophore in a small peptide. Their S0-S1 resonant multiphoton ionization (REMPI) spectra show, that in neutral molecules the tail-chromophore interaction is weak and electronic excitation is localized at the chromophore. For molecules, where the ionization energy of the tail is considerable higher than that of the chromophore, by high resolution REMPI photoelectron spectroscopy we find the <span class="hlt">charge</span> to be localized on the aromatic chromophore. This scheme also in suitable peptides allows local ionization at the aromatic chromophore. An estimate for various <span class="hlt">charge</span> positions in peptide chains, however, shows, that for most of the amino acids electron hole positions in the nitrogen and oxygen "lone pair" orbitals of the peptide bond are nearly degenerate. REMPI photoelectron spectra of phenylethylamine, which as a model system contains such two degenerate <span class="hlt">charge</span> positions, show small energetic shift of the ionization energy but strong geometry changes upon electron removal. This result is interpreted as direct ionization into a mixed <span class="hlt">charge</span> delocalized state. Consequences for the <span class="hlt">charge</span> transfer mechanism in peptides are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016PhLB..755..177H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016PhLB..755..177H"><span>The <span class="hlt">charged</span> black-hole bomb: A lower bound on the <span class="hlt">charge</span>-to-mass ratio of the explosive scalar field</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hod, Shahar</p> <p>2016-04-01</p> <p>The well-known superradiant amplification mechanism allows a <span class="hlt">charged</span> scalar field of proper mass μ and electric <span class="hlt">charge</span> q to extract the Coulomb energy of a <span class="hlt">charged</span> Reissner-Nordström black hole. The rate of energy extraction can grow exponentially in time if the system is placed inside a reflecting cavity which prevents the <span class="hlt">charged</span> scalar field from escaping to infinity. This composed black-hole-<span class="hlt">charged</span>-scalar-field-mirror system is known as the <span class="hlt">charged</span> black-hole bomb. Previous numerical studies of this composed physical system have shown that, in the linearized regime, the inequality q / μ > 1 provides a necessary condition for the development of the superradiant instability. In the present paper we use analytical techniques to study the instability properties of the <span class="hlt">charged</span> black-hole bomb in the regime of linearized scalar fields. In particular, we prove that the lower bound q/μ>√{rm /r- - 1/ rm /r+ - 1 } provides a necessary condition for the development of the superradiant instability in this composed physical system (here r± are the horizon radii of the <span class="hlt">charged</span> Reissner-Nordström black hole and rm is the radius of the confining mirror). This analytically derived lower bound on the superradiant instability regime of the composed black-hole-<span class="hlt">charged</span>-scalar-field-mirror system is shown to agree with direct numerical computations of the instability spectrum.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018EPJC...78...62A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018EPJC...78...62A"><span>Study of <span class="hlt">charged</span> hadron multiplicities in <span class="hlt">charged</span>-current neutrino-lead interactions in the OPERA detector</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Agafonova, N.; Aleksandrov, A.; Anokhina, A.; Aoki, S.; Ariga, A.; Ariga, T.; Bertolin, A.; Bodnarchuk, I.; Bozza, C.; Brugnera, R.; Buonaura, A.; Buontempo, S.; Chernyavskiy, M.; Chukanov, A.; Consiglio, L.; D'Ambrosio, N.; De Lellis, G.; De Serio, M.; del Amo Sanchez, P.; Di Crescenzo, A.; Di Ferdinando, D.; Di Marco, N.; Dmitrievski, S.; Dracos, M.; Duchesneau, D.; Dusini, S.; Dzhatdoev, T.; Ebert, J.; Ereditato, A.; Fini, R. A.; Fornari, F.; Fukuda, T.; Galati, G.; Garfagnini, A.; Gentile, V.; Goldberg, J.; Gornushkin, Y.; Gorbunov, S.; Grella, G.; Guler, A. M.; Gustavino, C.; Hagner, C.; Hara, T.; Hayakawa, T.; Hollnagel, A.; Hosseini, B.; Ishiguro, K.; Jakovcic, K.; Jollet, C.; Kamiscioglu, C.; Kamiscioglu, M.; Kim, S. H.; Kitagawa, N.; Klicek, B.; Kodama, K.; Komatsu, M.; Kose, U.; Kreslo, I.; Laudisio, F.; Lauria, A.; Ljubicic, A.; Longhin, A.; Loverre, P.; Malgin, A.; Malenica, M.; Mandrioli, G.; Matsuo, T.; Matveev, V.; Mauri, N.; Medinaceli, E.; Meregaglia, A.; Mikado, S.; Miyanishi, M.; Mizutani, F.; Monacelli, P.; Montesi, M. C.; Morishima, K.; Muciaccia, M. T.; Naganawa, N.; Naka, T.; Nakamura, M.; Nakano, T.; Niwa, K.; Okateva, N.; Ogawa, S.; Ozaki, K.; Paoloni, A.; Paparella, L.; Park, B. D.; Pasqualini, L.; Pastore, A.; Patrizii, L.; Pessard, H.; Podgrudkov, D.; Polukhina, N.; Pozzato, M.; Pupilli, F.; Roda, M.; Roganova, T.; Rokujo, H.; Rosa, G.; Ryazhskaya, O.; Sato, O.; Schembri, A.; Shakirianova, I.; Shchedrina, T.; Shibuya, H.; Shibayama, E.; Shiraishi, T.; Simone, S.; Sirignano, C.; Sirri, G.; Sotnikov, A.; Spinetti, M.; Stanco, L.; Starkov, N.; Stellacci, S. M.; Stipcevic, M.; Strolin, P.; Takahashi, S.; Tenti, M.; Terranova, F.; Tioukov, V.; Vasina, S.; Vilain, P.; Voevodina, E.; Votano, L.; Vuilleumier, J. L.; Wilquet, G.; Wonsak, B.; Yoon, C. S.</p> <p>2018-01-01</p> <p>The OPERA experiment was designed to search for ν _{μ } → ν _{τ } oscillations in appearance mode through the direct observation of tau neutrinos in the CNGS neutrino beam. In this paper, we report a study of the multiplicity of <span class="hlt">charged</span> particles produced in <span class="hlt">charged</span>-current neutrino interactions in lead. We present <span class="hlt">charged</span> hadron average multiplicities, their dispersion and investigate the KNO scaling in different kinematical regions. The results are presented in detail in the form of tables that can be used in the validation of Monte Carlo generators of neutrino-lead interactions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007JPhCS..58..188A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007JPhCS..58..188A"><span><span class="hlt">Charge</span> exchange of highly <span class="hlt">charged</span> argon ions as a function of projectile energy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Allen, F. I.; Biedermann, C.; Radtke, R.; Fussmann, G.</p> <p>2007-03-01</p> <p>X-ray emission of highly <span class="hlt">charged</span> argon ions following <span class="hlt">charge</span> exchange collisions with argon atoms has been measured as a function of projectile energy. The ions are extracted from the Electron Beam Ion Trap (EBIT) in Berlin and selected according to their massto-<span class="hlt">charge</span> ratios. Experiments focussed on hydrogen-like and bare argon ions which were decelerated from 125q eV/amu to below 0.25q eV/amu prior to interaction with an argon gas target. The x-ray spectra recorded probe the cascading transitions resulting from electron capture into Rydberg states and are found to vary significantly with collision velocity. This indicates a shift in the orbital angular momentum of the capture state. Hardness ratios are observed to increase with decreasing projectile energy though at a rate which differs from the results of simulations. For comparison, measurements of the x-ray emission following <span class="hlt">charge</span> exchange within the trap were carried out and are in agreement with the findings of the EBIT group at LLNL. Both of these in situ measurements, however, are in discrepancy with the results of the experiments using extracted ions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/6575057','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/biblio/6575057"><span>Electrochemically controlled <span class="hlt">charging</span> circuit for storage batteries</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Onstott, E.I.</p> <p>1980-06-24</p> <p>An electrochemically controlled <span class="hlt">charging</span> circuit for <span class="hlt">charging</span> storage batteries is disclosed. The embodiments disclosed utilize dc amplification of battery control current to minimize total energy expended for <span class="hlt">charging</span> storage batteries to a preset voltage level. The circuits allow for selection of Zener diodes having a wide range of reference voltage levels. Also, the preset voltage level to which the storage batteries are <span class="hlt">charged</span> can be varied over a wide range.</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('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=128532&Lab=NRMRL&keyword=electronics&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=128532&Lab=NRMRL&keyword=electronics&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>MODELING PARTICULATE <span class="hlt">CHARGING</span> IN ESPS</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>In electrostatic precipitators there is a strong interaction between the particulate space <span class="hlt">charge</span> and the operating voltage and current of an electrical section. Calculating either the space <span class="hlt">charge</span> or the operating point when the other is fixed is not difficult, but calculating b...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvD..97j4058Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvD..97j4058Z"><span>Inspirals into a <span class="hlt">charged</span> black hole</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhu, Ruomin; Osburn, Thomas</p> <p>2018-05-01</p> <p>We model the quasicircular inspiral of a compact object into a more massive <span class="hlt">charged</span> black hole. Extreme and intermediate mass-ratio inspirals are considered through a small mass-ratio approximation. Reissner-Nordström spacetime is used to describe the <span class="hlt">charged</span> black hole. The effect of radiation reaction on the smaller body is quantified through calculation of electromagnetic and gravitational energy fluxes via solution of Einstein's and Maxwell's equations. Inspiral trajectories are determined by matching the orbital energy decay rate to the rate of radiative energy dissipation. We observe that inspirals into a <span class="hlt">charged</span> black hole evolve more rapidly than comparable inspirals into a neutral black hole. Through analysis of a variety of inspiral configurations, we conclude that electric <span class="hlt">charge</span> is an important effect concerning gravitational wave observations when the <span class="hlt">charge</span> exceeds the threshold |Q |/M ≳0.071 √{ɛ }, where ɛ is the mass ratio.</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 negatively <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/1618818','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/1618818"><span>The influence of <span class="hlt">charge</span> and the distribution of <span class="hlt">charge</span> in the polar region of phospholipids on the activity of UDP-glucuronosyltransferase.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zakim, D; Eibl, H</p> <p>1992-07-05</p> <p>Studies of the mechanism of lipid-induced regulation of the microsomal enzyme UDP-glucuronosyltransferase have been extended by examining the influence of <span class="hlt">charge</span> within the polar region on the ability of lipids to activate delipidated pure enzyme. The effects of net negative <span class="hlt">charge</span>, of <span class="hlt">charge</span> separation in phosphocholine, and of the distribution of <span class="hlt">charge</span> 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 <span class="hlt">charge</span> 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 <span class="hlt">charge</span> increases from -1 to -2. The inhibitory effect of negatively <span class="hlt">charged</span> lipids is on the functional state of the enzyme and is not due to electrostatic repulsion of negatively <span class="hlt">charged</span> substrates of the enzyme. Although the inhibitory effect of net negative <span class="hlt">charge</span> is removed when negative <span class="hlt">charge</span> is balanced by a positive <span class="hlt">charge</span> 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 <span class="hlt">charge</span> between Pi and the quaternary nitrogen, the distance between the negative and positive <span class="hlt">charges</span> and the orientation of the dipole created by them are critical for activation of GT2p. The negative and positive <span class="hlt">charges</span> 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 <span class="hlt">charge</span> is on the polymethylene side of the lipid-water interface and the positive <span class="hlt">charge</span> 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 <span class="hlt">charge</span>, do</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3970531','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3970531"><span><span class="hlt">Charge</span> separation and <span class="hlt">charge</span> delocalization identified in long-living states of photoexcited DNA</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Bucher, Dominik B.; Pilles, Bert M.; Carell, Thomas; Zinth, Wolfgang</p> <p>2014-01-01</p> <p>Base stacking in DNA is related to long-living excited states whose molecular nature is still under debate. To elucidate the molecular background we study well-defined oligonucleotides with natural bases, which allow selective UV excitation of one single base in the strand. IR probing in the picosecond regime enables us to dissect the contribution of different single bases to the excited state. All investigated oligonucleotides show long-living states on the 100-ps time scale, which are not observable in a mixture of single bases. The fraction of these states is well correlated with the stacking probabilities and reaches values up to 0.4. The long-living states show characteristic absorbance bands that can be assigned to <span class="hlt">charge</span>-transfer states by comparing them to marker bands of radical cation and anion spectra. The <span class="hlt">charge</span> separation is directed by the redox potential of the involved bases and thus controlled by the sequence. The spatial dimension of this <span class="hlt">charge</span> separation was investigated in longer oligonucleotides, where bridging sequences separate the excited base from a sensor base with a characteristic marker band. After excitation we observe a bleach of all involved bases. The contribution of the sensor base is observable even if the bridge is composed of several bases. This result can be explained by a <span class="hlt">charge</span> delocalization along a well-stacked domain in the strand. The presence of <span class="hlt">charged</span> radicals in DNA strands after light absorption may cause reactions—oxidative or reductive damage—currently not considered in DNA photochemistry. PMID:24616517</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016APS..MAR.A4005K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016APS..MAR.A4005K"><span>Nanotribology of <span class="hlt">charged</span> polymer brushes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Klein, Jacob</p> <p></p> <p>Polymers at surfaces, whose modern understanding may be traced back to early work by Sam Edwards1, have become a paradigm for modification of surface properties, both as steric stabilizers and as remarkable boundary lubricants2. <span class="hlt">Charged</span> polymer brushes are of particular interest, with both technological implications and especially biological relevance where most macromolecules are <span class="hlt">charged</span>. In the context of biolubrication, relevant in areas from dry eye syndrome to osteoarthritis, <span class="hlt">charged</span> polymer surface phases and their complexes with other macromolecules may play a central role. The hydration lubrication paradigm, where tenaciously-held yet fluid hydration shells surrounding ions or zwitterions serve as highly-efficient friction-reducing elements, has been invoked to understand the excellent lubrication provided both by ionized3 and by zwitterionic4 brushes. In this talk we describe recent advances in our understanding of the nanotribology of such <span class="hlt">charged</span> brush systems. We consider interactions between <span class="hlt">charged</span> end-grafted polymers, and how one may disentangle the steric from the electrostatic surface forces5. We examine the limits of lubrication by ionized brushes, both synthetic and of biological origins, and how highly-hydrated zwitterionic chains may provide extremely effective boundary lubrication6. Finally we describe how the lubrication of articular cartilage in the major joints, a tribosystem presenting some of the greatest challenges and opportunities, may be understood in terms of a supramolecular synergy between <span class="hlt">charged</span> surface-attached polymers and zwitterionic groups7. Work supported by European Research Council (HydrationLube), Israel Science Foundation (ISF), Petroleum Research Fund of the American Chemical Society, ISF-NSF China Joint Program.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20060009004','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20060009004"><span><span class="hlt">CHARGING</span> OF DEVICES BY MICROWAVE POWER BEAMING</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Landis, Geoffrey A. (Inventor)</p> <p>2005-01-01</p> <p>A system for providing wireless, <span class="hlt">charging</span> power and/or primary power to electronic/electrical devices is described whereby microwave energy is employed. Microwave energy is focused by a power transmitter comprising one or more adaptively-phased microwave array emitters onto a device to be <span class="hlt">charged</span>. Rectennas within the device to be <span class="hlt">charged</span> receive and rectify the microwave energy and use it for battery <span class="hlt">charging</span> and/or for primary power. A locator signal generated by the device to be <span class="hlt">charged</span> is analyzed by the system to determine the location of the device to be <span class="hlt">charged</span> relative to the microwave array emitters, permitting thc microwave energy to be directly specifically towards the device to be <span class="hlt">charged</span>. Backscatter detectors respond to backscatter energy reflected off of any obstacle between the device to be <span class="hlt">charged</span> and the microwave array emitters. Power to any obstructed microwave array emitter is reduced until the obstruction is removed. Optionally, data can be modulated onto microwave energy beams produced by the array emitter and demodulated by the device, thereby providing means of data communication from the power transmitter to the device. Similarly, data can be modulated onto the locator signal and demodulated in the power transmitter, thereby providing means of data communication from the device to the power transmitter.</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 addition 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('http://adsabs.harvard.edu/abs/2002GeoRL..29.2108P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002GeoRL..29.2108P"><span>Recovery curves of the surface electric field after lightning discharges occurring between the positive <span class="hlt">charge</span> pocket and negative <span class="hlt">charge</span> centre in a thundercloud</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pawar, S. D.; Kamra, A. K.</p> <p>2002-12-01</p> <p>Surface observations of the electric field recovery curves of the lightning discharges occurring between the positive <span class="hlt">charge</span> pocket and negative main <span class="hlt">charge</span> 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 <span class="hlt">charge</span> and the relative efficiencies of the <span class="hlt">charge</span> generating processes responsible for growth of positive <span class="hlt">charge</span> pocket and main negative <span class="hlt">charge</span> centre in the thundercloud. The <span class="hlt">charging</span> currents responsible for the growth of <span class="hlt">charge</span> in positive <span class="hlt">charge</span> pockets is computed to be 2-4 times larger than that for the growth of the main negative <span class="hlt">charge</span>. However, the <span class="hlt">charge</span> destroyed in such a discharge is found to be comparable to that in a discharge between the main <span class="hlt">charge</span> centres of the thundercloud.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19910014911','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19910014911"><span>A <span class="hlt">charging</span> study of ACTS using NASCAP</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Herr, Joel L.</p> <p>1991-01-01</p> <p>The NASA <span class="hlt">Charging</span> Analyzer Program (NASCAP) computer code is a three dimensional finite element <span class="hlt">charging</span> code designed to analyze spacecraft <span class="hlt">charging</span> in the magnetosphere. Because of the characteristics of this problem, NASCAP can use an quasi-static approach to provide a spacecraft designer with an understanding of how a specific spacecraft will interact with a geomagnetic substorm. The results of the simulation can help designers evaluate the probability and location of arc discharges of <span class="hlt">charged</span> surfaces on the spacecraft. A <span class="hlt">charging</span> study of NASA's Advanced Communication Technology Satellite (ACTS) using NASCAP is reported. The results show that the ACTS metalized multilayer insulating blanket design should provide good electrostatic discharge control.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1390235','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1390235"><span>Phased <span class="hlt">charging</span> and discharging in capacitive desalinatio</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Stadermann, Michael; Qu, Yatian; Santiago, Juan G.; Hemmatifar, Ali</p> <p>2017-09-12</p> <p>A system combines complete, ultra-thin cells into a monolithic and robust framework necessary for desalination applications which yields orders of magnitude faster desalination. The electrode pairs are located so that a flow of feed water flows through or around the electrode pairs with the flow perpendicular to sequentially applied electric potentials. The system is controlled to <span class="hlt">charge</span> the series of electrode pairs sequentially or phased. That means the <span class="hlt">charging</span> of the second electrode pair is delayed with regard to the <span class="hlt">charging</span> of the first electrode pair and the <span class="hlt">charging</span> of a third electrode pair is delayed with respect to the <span class="hlt">charging</span> of the second electrode pair.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016PhRvE..93c3208H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016PhRvE..93c3208H"><span><span class="hlt">Charging</span> of nonspherical macroparticles in a plasma</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Holgate, J. T.; Coppins, M.</p> <p>2016-03-01</p> <p>The current theories of macroparticle <span class="hlt">charging</span> in a plasma are limited to spheres, and are unsuitable for the multitude of nonspherical objects existing in astrophysical, atmospheric, laboratory, and fusion plasmas. This paper extends the most widely used spherical <span class="hlt">charging</span> theory, orbit motion limited theory, to spheroids and, as such, provides a comprehensive study of the <span class="hlt">charging</span> of nonspherical objects in a plasma. The spherical <span class="hlt">charging</span> theory is shown to be a reasonable approximation for a considerable range of spheroids. However, the electric potential of highly elongated spheroids can be almost twice the spherical value. Furthermore, the total <span class="hlt">charge</span> on the spheroids increases by a significantly larger factor than their potential.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008PSST...17d5012S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008PSST...17d5012S"><span>Formation of <span class="hlt">charged</span> nanoparticles in hydrocarbon flames: principal mechanisms</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Starik, A. M.; Savel'ev, A. M.; Titova, N. S.</p> <p>2008-11-01</p> <p>The processes of <span class="hlt">charged</span> gaseous and particulate species formation in sooting hydrocarbon/air flame are studied. The original kinetic model, comprising the chemistry of neutral and <span class="hlt">charged</span> gaseous species, generation of primary clusters, which then undergo <span class="hlt">charging</span> due to attachment of ions and electrons to clusters and via thermoemission, and coagulation of <span class="hlt">charged-charged</span>, <span class="hlt">charged</span>-neutral and neutral-neutral particles, is reported. The analysis shows that the principal mechanisms of <span class="hlt">charged</span> particle origin in hydrocarbon flames are associated with the attachment of ions and electrons produced in the course of chemoionization reactions to primary small clusters and particles and coagulation via <span class="hlt">charged-charged</span> and <span class="hlt">charged</span>-neutral particle interaction. Thermal ionization of particles does not play a significant role in the particle <span class="hlt">charging</span>. This paper was presented at the Third International Symposium on Nonequilibrium Process, combustion, and Atmospheric Phenomena (Dagomys, Sochi, Russia, 25-29 June 2007).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011AIPC.1336..106D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011AIPC.1336..106D"><span>Solar Wind <span class="hlt">Charge</span> Exchange Studies Of Highly <span class="hlt">Charged</span> Ions On Atomic Hydrogen</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Draganić, I. N.; Seely, D. G.; McCammon, D.; Havener, C. C.</p> <p>2011-06-01</p> <p>Accurate studies of low-energy <span class="hlt">charge</span> exchange (CX) are critical to understanding underlying soft X-ray radiation processes in the interaction of highly <span class="hlt">charged</span> ions from the solar wind with the neutral atoms and molecules in the heliosphere, cometary comas, planetary atmospheres, interstellar winds, etc.. Particularly important are the CX cross sections for bare, H-like, and He-like ions of C, N, O and Ne, which are the dominant <span class="hlt">charge</span> states for these heavier elements in the solar wind. Absolute total cross sections for single electron capture by H-like ions of C, N, O and fully-stripped O ions from atomic hydrogen have been measured in an expanded range of relative collision energies (5 eV/u-20 keV/u) and compared to previous H-oven measurements. The present measurements are performed using a merged-beams technique with intense highly <span class="hlt">charged</span> ion beams extracted from a 14.5 GHz ECR ion source installed on a high voltage platform at the Oak Ridge National Laboratory. For the collision energy range of 0.3 keV/u-3.3 keV/u, which corresponds to typical ion velocities in the solar wind, the new measurements are in good agreement with previous H-oven measurements. The experimental results are discussed in detail and compared with theoretical calculations where available.</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 addition, 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 addition, 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://hdl.handle.net/2060/19840025600','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19840025600"><span><span class="hlt">Charge</span> Control Investigation of Rechargeable Lithium Cells</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Otzinger, B.; Somoano, R.</p> <p>1984-01-01</p> <p>An ambient temperature rechargeable Li-TiS2 cell was cycled under conditions which simulate aerospace applications. A novel <span class="hlt">charge</span>/discharge state-of-<span class="hlt">charge</span> control scheme was used, together with tapered current <span class="hlt">charging</span>, to overcome deleterious effects associated with end-of-<span class="hlt">charge</span> and end-of-discharge voltages. The study indicates that Li-TiS2 cells hold promise for eventual synchronous satellite-type applications. Problem areas associated with performance degradation and reconditioning effects are identified.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EPJD...71..318K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EPJD...71..318K"><span>Numerical experiments on <span class="hlt">charging</span> of a spherical body in a plasma with Maxwellian distributions of <span class="hlt">charged</span> particles</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Krasovsky, Victor L.; Kiselyov, Alexander A.</p> <p>2017-12-01</p> <p>New results of numerical simulation of collisionless plasma perturbation caused by a sphere absorbing electrons and ions are presented. Consideration is given to nonstationary phenomena accompanying the process of <span class="hlt">charging</span> as well as to plasma steady state reached at long times. Corresponding asymptotic values of <span class="hlt">charges</span> of the sphere and trapped-ion cloud around it have been found along with self-consistent electric field pattern depending on parameters of the unperturbed plasma. It is established that contribution of the trapped ions to screening of the <span class="hlt">charged</span> sphere can be quite significant, so that the screening becomes essentially nonlinear in nature. A simple interconnection between the sphere radius, electron and ion Debye lengths has been revealed as the condition for maximum trapped-ion effect. Kinetic structure of the space <span class="hlt">charge</span> induced in the plasma is discussed with relation to the specific form of the unperturbed <span class="hlt">charged</span> particle distribution functions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/868019','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/868019"><span>Nonvolatile semiconductor memory having three dimension <span class="hlt">charge</span> confinement</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Dawson, L. Ralph; Osbourn, Gordon C.; Peercy, Paul S.; Weaver, Harry T.; Zipperian, Thomas E.</p> <p>1991-01-01</p> <p>A layered semiconductor device with a nonvolatile three dimensional memory comprises a storage channel which stores <span class="hlt">charge</span> carriers. <span class="hlt">Charge</span> carriers flow laterally through the storage channel from a source to a drain. Isolation material, either a Schottky barrier or a heterojunction, located in a trench of an upper layer controllably retains the <span class="hlt">charge</span> within the a storage portion determined by the confining means. The <span class="hlt">charge</span> is retained for a time determined by the isolation materials' nonvolatile characteristics or until a change of voltage on the isolation material and the source and drain permit a read operation. Flow of <span class="hlt">charge</span> through an underlying sense channel is affected by the presence of <span class="hlt">charge</span> within the storage channel, thus the presences of <span class="hlt">charge</span> in the memory can be easily detected.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008AGUFM.V33F..03S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008AGUFM.V33F..03S"><span>Effects of granular <span class="hlt">charge</span> on flow and mixing</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shinbrot, T.; Herrmann, H. J.</p> <p>2008-12-01</p> <p>Sandstorms in the desert have long been reported to produce sparks and other electrical disturbances - indeed as long ago as 1850, Faraday commented on the peculiarities of granular <span class="hlt">charging</span> during desert sandstorms. Similarly, lightning strikes within volcanic dust plumes have been repeatedly reported for over half a century, but remain unexplained. The problem of granular <span class="hlt">charging</span> has applied, as well as natural, implications, for <span class="hlt">charged</span> particle clouds frequently generate spectacularly devastating dust explosions in granular processing plants, and sand becomes strongly electrified by helicopters traveling in desert environments. The issue even has implications for missions to the Moon and to Mars, where <span class="hlt">charged</span> dust degrades solar cells viability and clings to spacesuits, limiting the lifetime of their joints. Despite the wide-ranging importance of granular <span class="hlt">charging</span>, even the simplest aspects of its causes remain elusive. To take one example, sand grains in the desert manage to <span class="hlt">charge</span> one another despite having only similar materials to rub against over expanses of many miles - thus existing theories of <span class="hlt">charging</span> due to material differences fail entirely to account for the observed <span class="hlt">charging</span> of desert sands. In this talk, we describe recent progress made in identifying underlying causes of granular <span class="hlt">charging</span>, both in desert-like environments and in industrial applications, and we examine effects of granular <span class="hlt">charging</span> on flow, mixing and separation of common granular materials. We find that <span class="hlt">charging</span> of identical grains can occur under simple laboratory conditions, and we make new predictions for the effects of this <span class="hlt">charging</span> on granular behaviours.</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('http://adsabs.harvard.edu/abs/2016PhyU...59..531Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016PhyU...59..531Y"><span>Physical stage of photosynthesis <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>Yakovlev, A. G.; Shuvalov, V. A.</p> <p>2016-06-01</p> <p>An analytical review is given concerning the biophysical aspects of light-driven primary <span class="hlt">charge</span> separation in photosynthesis reaction centers (RCs) which are special pigment-protein complexes residing in a cell membrane. The primary (physical) stage of <span class="hlt">charge</span> separation occurs in the pico- and femtosecond ranges and consists of transferring an electron along the active A-branch of pigments. The review presents vast factual material on both the general issues of primary photosynthesis and some more specific topics, including (1) the role of the inactive B-branch of pigments, (2) the effect of the protein environment on the <span class="hlt">charge</span> separation, and (3) the participation of monomeric bacteriochlorophyll BA in primary electron acceptance. It is shown that the electron transfer and stabilization are strongly influenced by crystallographic water and tyrosine M210 molecules from the nearest environment of BA. A linkage between collective nuclear motions and electron transfer upon <span class="hlt">charge</span> separation is demonstrated. The nature of the high quantum efficiency of primary <span class="hlt">charge</span> separation reactions is discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23962575','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23962575"><span>Universal health coverage and user <span class="hlt">charges</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Smith, Peter C</p> <p>2013-10-01</p> <p>There has been an explosion of interest in the concept of ‘universal health coverage’, fuelled by publication of the World Health Report 2010. This paper argues that the system of user <span class="hlt">charges</span> for health services is a fundamental determinant of levels of coverage. A <span class="hlt">charge</span> can lead to a loss of utility in two ways. Citizens who are deterred from using services by the <span class="hlt">charge</span> will suffer an adverse health impact. And citizens who use the service will suffer a loss of wealth. The role of social health insurance is threefold: to reduce households’ financial risk associated with sickness; to promote enhanced access to needed health services; and to contribute to societal equity objectives, through an implicit financial transfer from rich to poor and healthy to sick. In principle, an optimal user <span class="hlt">charge</span> policy can ensure that the social health insurance funds are used to best effect in pursuit of these objectives. This paper calls for a fundamental rethink of attitudes and policy towards user <span class="hlt">charges</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1096783','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1096783"><span>Proximity <span class="hlt">charge</span> sensing for semiconductor detectors</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Luke, Paul N; Tindall, Craig S; Amman, Mark</p> <p>2013-10-08</p> <p>A non-contact <span class="hlt">charge</span> sensor includes a semiconductor detector having a first surface and an opposing second surface. The detector includes a high resistivity electrode layer on the first surface and a low resistivity electrode on the high resistivity electrode layer. A portion of the low resistivity first surface electrode is deleted to expose the high resistivity electrode layer in a portion of the area. A low resistivity electrode layer is disposed on the second surface of the semiconductor detector. A voltage applied between the first surface low resistivity electrode and the second surface low resistivity electrode causes a free <span class="hlt">charge</span> to drift toward the first or second surface according to a polarity of the free <span class="hlt">charge</span> and the voltage. A <span class="hlt">charge</span> sensitive preamplifier coupled to a non-contact electrode disposed at a distance from the exposed high resistivity electrode layer outputs a signal in response to movement of free <span class="hlt">charge</span> within the detector.</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 negative (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.ncbi.nlm.nih.gov/pubmed/29727176','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29727176"><span>Through-Space Intervalence <span class="hlt">Charge</span> Transfer as a Mechanism for <span class="hlt">Charge</span> Delocalisation in Metal-Organic Frameworks.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Hua, Carol; Doheny, Patrick William; Ding, Bowen; Chan, Bun; Yu, Michelle; Kepert, Cameron J; D'Alessandro, Deanna M</p> <p>2018-05-04</p> <p>Understanding the nature of <span class="hlt">charge</span> transfer mechanisms in 3-dimensional Metal-Organic Frameworks (MOFs) is an important goal owing to the possibility of harnessing this knowledge to design conductive frameworks. These materials have been implicated as the basis for the next generation of technological devices for applications in energy storage and conversion, including electrochromic devices, electrocatalysts, and battery materials. After nearly two decades of intense research into MOFs, the mechanisms of <span class="hlt">charge</span> transfer remain relatively poorly understood, and new strategies to achieve <span class="hlt">charge</span> mobility remain elusive and challenging to experimentally explore, validate and model. We now demonstrate that aromatic stacking interactions in Zn(II) frameworks containing cofacial thiazolo[5,4-d]thiazole units lead to a mixed-valence state upon electrochemical or chemical reduction. This through-space Intervalence <span class="hlt">Charge</span> Transfer (IVCT) phenomenon represents a new mechanism for <span class="hlt">charge</span> delocalisation in MOFs. Computational modelling of the optical data combined with application of Marcus-Hush theory to the IVCT bands for the mixed-valence framework has enabled quantification of the degree of delocalisation using both in situ and ex situ electro- and spectro-electrochemical methods. A distance dependence for the through-space electron transfer has also been identified on the basis of experimental studies and computational calculations. This work provides a new window into electron transfer phenomena in 3-dimensional coordination space, of relevance to electroactive MOFs where new mechanisms for <span class="hlt">charge</span> transfer are highly sought after, and to understanding biological light harvesting systems where through-space mixed-valence interactions are operative.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA133722','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA133722"><span>Maneuvering Characteristics of the YP 676 Class Seamanship Training Craft as Represented by Radio-Controlled Model 9022.</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>1983-04-01</p> <p>CENTER BET.. UNCLASSIFIED G A ROSSIGNOL <span class="hlt">APR</span> 83 DTNSRDC/SPD- 1082 -0I FIG 13/110 NL Ehhmhmommhhu ILJEUIEEE 1.2. 1 1 1 m - 11111_.25 .4i .4 ....’ll’- L... 1082 -Ol 8._ , ’ ’... . * .. . ’ ’"" --’- " ’ : 8 MAJOR DTNSRDC ORGANIZATIONAL COMPONENTS DTNSRDC COMMANDER TECHNICAL DIRECTOR 01 OFFICER-IN-<span class="hlt">CHARGE</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/918049-charge-retraction-time-flight-measurement-organic-charge-transport-materials','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/918049-charge-retraction-time-flight-measurement-organic-charge-transport-materials"><span><span class="hlt">Charge</span>-Retraction Time-of-Flight Measurement for Organic <span class="hlt">Charge</span> Transport Materials</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>Wallace, J.U.; Young, R.H.; Tang, C.W.</p> <p></p> <p>This describes an all-electrical technique, <span class="hlt">charge</span>-retraction time-of-flight (CR-TOF), to measure <span class="hlt">charge</span> carrier mobility through an organic layer. Carriers are injected and accumulated at a blocking interface, then retracted. The retraction current transient is nearly indistinguishable from a traditional time-of-flight photocurrent. The CR-TOF technique is validated by measurement of the hole mobility of two well-known compounds, 4,4',4"-tris[N-(3-methylphenyl)-N-phenylamino]triphenylamine and 4,4'-bis[N-1-napthyl)-N-phenylamino]biphenyl, utilizing 1,3,5-tris(N-phenylbenzimidazol-2-yl)-benzene as a hole-blocking layer.</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 addition 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.osti.gov/biblio/1338192-charge-transport-network-dynamics-molecular-aggregates','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1338192-charge-transport-network-dynamics-molecular-aggregates"><span><span class="hlt">Charge</span> transport network dynamics in molecular aggregates</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>Jackson, Nicholas E.; Chen, Lin X.; Ratner, Mark A.</p> <p>2016-07-20</p> <p>Due to the nonperiodic nature of <span class="hlt">charge</span> transport in disordered systems, generating insight into static <span class="hlt">charge</span> transport networks, as well as analyzing the network dynamics, can be challenging. Here, we apply time-dependent network analysis to scrutinize the <span class="hlt">charge</span> transport networks of two representative molecular semiconductors: a rigid n-type molecule, perylenediimide, and a flexible p-type molecule, bBDT(TDPP)2. Simulations reveal the relevant timescale for local transfer integral decorrelation to be ~100 fs, which is shown to be faster than that of a crystalline morphology of the same molecule. Using a simple graph metric, global network changes are observed over timescales competitive withmore » <span class="hlt">charge</span> carrier lifetimes. These insights demonstrate that static <span class="hlt">charge</span> transport networks are qualitatively inadequate, whereas average networks often overestimate network connectivity. Finally, a simple methodology for tracking dynamic <span class="hlt">charge</span> transport properties is proposed.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1270770','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1270770"><span><span class="hlt">Charge</span> Management Optimization for Future TOU Rates: Preprint</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, Jiucai; Markel, Tony</p> <p>2016-07-01</p> <p>The effectiveness of future time of use (TOU) rates to enable managed <span class="hlt">charging</span> for providing demand response depends on the vehicle's flexibility and the benefits to owners. This paper adopts opportunity, delayed, and smart <span class="hlt">charging</span> methods to quantify these impacts, flexibilities, and benefits. Simulation results show that delayed and smart <span class="hlt">charging</span> methods can shift most <span class="hlt">charging</span> events to lower TOU rate periods without compromising the <span class="hlt">charged</span> energy and individual driver mobility needs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title30-vol1/pdf/CFR-2010-title30-vol1-sec77-1106.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title30-vol1/pdf/CFR-2010-title30-vol1-sec77-1106.pdf"><span>30 CFR 77.1106 - Battery-<span class="hlt">charging</span> stations; ventilation.</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>2010-07-01</p> <p>... 30 Mineral Resources 1 2010-07-01 2010-07-01 false Battery-<span class="hlt">charging</span> stations; ventilation. 77.1106... COAL MINES Fire Protection § 77.1106 Battery-<span class="hlt">charging</span> stations; ventilation. Battery-<span class="hlt">charging</span> stations shall be located in well-ventilated areas. Battery-<span class="hlt">charging</span> stations shall be equipped with reverse...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title30-vol1/pdf/CFR-2012-title30-vol1-sec77-1106.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title30-vol1/pdf/CFR-2012-title30-vol1-sec77-1106.pdf"><span>30 CFR 77.1106 - Battery-<span class="hlt">charging</span> stations; ventilation.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-07-01</p> <p>... 30 Mineral Resources 1 2012-07-01 2012-07-01 false Battery-<span class="hlt">charging</span> stations; ventilation. 77.1106... COAL MINES Fire Protection § 77.1106 Battery-<span class="hlt">charging</span> stations; ventilation. Battery-<span class="hlt">charging</span> stations shall be located in well-ventilated areas. Battery-<span class="hlt">charging</span> stations shall be equipped with reverse...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title30-vol1/pdf/CFR-2011-title30-vol1-sec77-1106.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title30-vol1/pdf/CFR-2011-title30-vol1-sec77-1106.pdf"><span>30 CFR 77.1106 - Battery-<span class="hlt">charging</span> stations; ventilation.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-07-01</p> <p>... 30 Mineral Resources 1 2011-07-01 2011-07-01 false Battery-<span class="hlt">charging</span> stations; ventilation. 77.1106... COAL MINES Fire Protection § 77.1106 Battery-<span class="hlt">charging</span> stations; ventilation. Battery-<span class="hlt">charging</span> stations shall be located in well-ventilated areas. Battery-<span class="hlt">charging</span> stations shall be equipped with reverse...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title30-vol1/pdf/CFR-2014-title30-vol1-sec77-1106.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title30-vol1/pdf/CFR-2014-title30-vol1-sec77-1106.pdf"><span>30 CFR 77.1106 - Battery-<span class="hlt">charging</span> stations; ventilation.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-07-01</p> <p>... 30 Mineral Resources 1 2014-07-01 2014-07-01 false Battery-<span class="hlt">charging</span> stations; ventilation. 77.1106... COAL MINES Fire Protection § 77.1106 Battery-<span class="hlt">charging</span> stations; ventilation. Battery-<span class="hlt">charging</span> stations shall be located in well-ventilated areas. Battery-<span class="hlt">charging</span> stations shall be equipped with reverse...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title30-vol1/pdf/CFR-2013-title30-vol1-sec77-1106.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title30-vol1/pdf/CFR-2013-title30-vol1-sec77-1106.pdf"><span>30 CFR 77.1106 - Battery-<span class="hlt">charging</span> stations; ventilation.</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>2013-07-01</p> <p>... 30 Mineral Resources 1 2013-07-01 2013-07-01 false Battery-<span class="hlt">charging</span> stations; ventilation. 77.1106... COAL MINES Fire Protection § 77.1106 Battery-<span class="hlt">charging</span> stations; ventilation. Battery-<span class="hlt">charging</span> stations shall be located in well-ventilated areas. Battery-<span class="hlt">charging</span> stations shall be equipped with reverse...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1407841-high-temperature-charge-density-wave-correlations-la1-without-spincharge-locking','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1407841-high-temperature-charge-density-wave-correlations-la1-without-spincharge-locking"><span>High-temperature <span class="hlt">charge</span> density wave correlations in La 1.875Ba 0.125CuO 4 without spin–<span class="hlt">charge</span> locking</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Miao, H.; Lorenzana, J.; Seibold, G.; ...</p> <p>2017-11-07</p> <p>Although all superconducting cuprates display <span class="hlt">charge</span>-ordering tendencies, their low-temperature properties are distinct, impeding efforts to understand the phenomena within a single conceptual framework. While some systems exhibit stripes of <span class="hlt">charge</span> and spin, with a locked periodicity, others host <span class="hlt">charge</span> density waves (CDWs) without any obviously related spin order. Here we use resonant inelastic X-ray scattering to follow the evolution of <span class="hlt">charge</span> correlations in the canonical stripe-ordered cuprate La 1.875Ba 0.125CuO 4 across its ordering transition. We find that high-temperature <span class="hlt">charge</span> correlations are unlocked from the wavevector of the spin correlations, signaling analogies to CDW phases in various other cuprates. Thismore » indicates that stripe order at low temperatures is stabilized by the coupling of otherwise independent <span class="hlt">charge</span> and spin density waves, with important implications for the relation between <span class="hlt">charge</span> and spin correlations in the cuprates.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5703287','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5703287"><span>High-temperature <span class="hlt">charge</span> density wave correlations in La1.875Ba0.125CuO4 without spin–<span class="hlt">charge</span> locking</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Lorenzana, J.; Seibold, G.; Peng, Y. Y.; Amorese, A.; Yakhou-Harris, F.; Kummer, K.; Brookes, N. B.; Konik, R. M.; Thampy, V.; Gu, G. D.; Ghiringhelli, G.; Braicovich, L.</p> <p>2017-01-01</p> <p>Although all superconducting cuprates display <span class="hlt">charge</span>-ordering tendencies, their low-temperature properties are distinct, impeding efforts to understand the phenomena within a single conceptual framework. While some systems exhibit stripes of <span class="hlt">charge</span> and spin, with a locked periodicity, others host <span class="hlt">charge</span> density waves (CDWs) without any obviously related spin order. Here we use resonant inelastic X-ray scattering to follow the evolution of <span class="hlt">charge</span> correlations in the canonical stripe-ordered cuprate La1.875Ba0.125CuO4 across its ordering transition. We find that high-temperature <span class="hlt">charge</span> correlations are unlocked from the wavevector of the spin correlations, signaling analogies to CDW phases in various other cuprates. This indicates that stripe order at low temperatures is stabilized by the coupling of otherwise independent <span class="hlt">charge</span> and spin density waves, with important implications for the relation between <span class="hlt">charge</span> and spin correlations in the cuprates. PMID:29114049</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1407841-high-temperature-charge-density-wave-correlations-la1-without-spincharge-locking','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1407841-high-temperature-charge-density-wave-correlations-la1-without-spincharge-locking"><span>High-temperature <span class="hlt">charge</span> density wave correlations in La 1.875Ba 0.125CuO 4 without spin–<span class="hlt">charge</span> locking</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>Miao, H.; Lorenzana, J.; Seibold, G.</p> <p></p> <p>Although all superconducting cuprates display <span class="hlt">charge</span>-ordering tendencies, their low-temperature properties are distinct, impeding efforts to understand the phenomena within a single conceptual framework. While some systems exhibit stripes of <span class="hlt">charge</span> and spin, with a locked periodicity, others host <span class="hlt">charge</span> density waves (CDWs) without any obviously related spin order. Here we use resonant inelastic X-ray scattering to follow the evolution of <span class="hlt">charge</span> correlations in the canonical stripe-ordered cuprate La 1.875Ba 0.125CuO 4 across its ordering transition. We find that high-temperature <span class="hlt">charge</span> correlations are unlocked from the wavevector of the spin correlations, signaling analogies to CDW phases in various other cuprates. Thismore » indicates that stripe order at low temperatures is stabilized by the coupling of otherwise independent <span class="hlt">charge</span> and spin density waves, with important implications for the relation between <span class="hlt">charge</span> and spin correlations in the cuprates.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3395871','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3395871"><span>Particle-based simulation of <span class="hlt">charge</span> transport in discrete-<span class="hlt">charge</span> nano-scale systems: the electrostatic problem</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>2012-01-01</p> <p>The fast and accurate computation of the electric forces that drive the motion of <span class="hlt">charged</span> particles at the nanometer scale represents a computational challenge. For this kind of system, where the discrete nature of the <span class="hlt">charges</span> cannot be neglected, boundary element methods (BEM) represent a better approach than finite differences/finite elements methods. In this article, we compare two different BEM approaches to a canonical electrostatic problem in a three-dimensional space with inhomogeneous dielectrics, emphasizing their suitability for particle-based simulations: the iterative method proposed by Hoyles et al. and the Induced <span class="hlt">Charge</span> Computation introduced by Boda et al. PMID:22338640</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22338640','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22338640"><span>Particle-based simulation of <span class="hlt">charge</span> transport in discrete-<span class="hlt">charge</span> nano-scale systems: the electrostatic problem.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Berti, Claudio; Gillespie, Dirk; Eisenberg, Robert S; Fiegna, Claudio</p> <p>2012-02-16</p> <p>The fast and accurate computation of the electric forces that drive the motion of <span class="hlt">charged</span> particles at the nanometer scale represents a computational challenge. For this kind of system, where the discrete nature of the <span class="hlt">charges</span> cannot be neglected, boundary element methods (BEM) represent a better approach than finite differences/finite elements methods. In this article, we compare two different BEM approaches to a canonical electrostatic problem in a three-dimensional space with inhomogeneous dielectrics, emphasizing their suitability for particle-based simulations: the iterative method proposed by Hoyles et al. and the Induced <span class="hlt">Charge</span> Computation introduced by Boda et al.</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/29683163','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29683163"><span>The effect of solvent relaxation time constants on free energy gap law for ultrafast <span class="hlt">charge</span> recombination following photoinduced <span class="hlt">charge</span> separation.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Mikhailova, Valentina A; Malykhin, Roman E; Ivanov, Anatoly I</p> <p>2018-05-16</p> <p>To elucidate the regularities inherent in the kinetics of ultrafast <span class="hlt">charge</span> recombination following photoinduced <span class="hlt">charge</span> separation in donor-acceptor dyads in solutions, the simulations of the kinetics have been performed within the stochastic multichannel point-transition model. Increasing the solvent relaxation time scales has been shown to strongly vary the dependence of the <span class="hlt">charge</span> recombination rate constant on the free energy gap. In slow relaxing solvents the non-equilibrium <span class="hlt">charge</span> recombination occurring in parallel with solvent relaxation is very effective so that the <span class="hlt">charge</span> recombination terminates at the non-equilibrium stage. This results in a crucial difference between the free energy gap laws for the ultrafast <span class="hlt">charge</span> recombination and the thermal <span class="hlt">charge</span> transfer. For the thermal reactions the well-known Marcus bell-shaped dependence of the rate constant on the free energy gap is realized while for the ultrafast <span class="hlt">charge</span> recombination only a descending branch is predicted in the whole area of the free energy gap exceeding 0.2 eV. From the available experimental data on the population kinetics of the second and first excited states for a series of Zn-porphyrin-imide dyads in toluene and tetrahydrofuran solutions, an effective rate constant of the <span class="hlt">charge</span> recombination into the first excited state has been calculated. The obtained rate constant being very high is nearly invariable in the area of the <span class="hlt">charge</span> recombination free energy gap from 0.2 to 0.6 eV that supports the theoretical prediction.</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 addition 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 additional <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://www.dtic.mil/docs/citations/ADA206946','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA206946"><span><span class="hlt">Charged</span> Slurry Droplet Research</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>1989-02-20</p> <p>IEEE/IAS annual meeting, Denver, CO, Sept. 28 - Oct. 3, 1986, p.1434. Accepted for publication IEEE Transactions on Industry Applications. 6. Lord...34Analysis of the Description of Evaporating <span class="hlt">Charged</span> Droplets, IEEE Transactions on Industry Applications, IA-19, 771, 1983. 9. H.M.A. Elghazaly, G.S.P. Castle...34Analysis of the Instability of Evaporating <span class="hlt">Charged</span> Liquid Drops", IEEE Transactions on Industry Applications, IA-22, 892, 1986. 10. H.M.A</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title31-vol2/pdf/CFR-2010-title31-vol2-sec206-9.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title31-vol2/pdf/CFR-2010-title31-vol2-sec206-9.pdf"><span>31 CFR 206.9 - <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>2010-07-01</p> <p>... 31 Money and Finance: Treasury 2 2010-07-01 2010-07-01 false <span class="hlt">Charges</span>. 206.9 Section 206.9 Money and Finance: Treasury Regulations Relating to Money and Finance (Continued) FISCAL SERVICE, DEPARTMENT... effective date of the <span class="hlt">charge</span> or the appeals decision, an agency must submit appropriate accounting...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title32-vol5/pdf/CFR-2013-title32-vol5-sec776-81.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title32-vol5/pdf/CFR-2013-title32-vol5-sec776-81.pdf"><span>32 CFR 776.81 - <span class="hlt">Charges</span>.</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>2013-07-01</p> <p>... 32 National Defense 5 2013-07-01 2013-07-01 false <span class="hlt">Charges</span>. 776.81 Section 776.81 National Defense Department of Defense (Continued) DEPARTMENT OF THE NAVY MISCELLANEOUS RULES PROFESSIONAL CONDUCT OF... <span class="hlt">charges</span>, together with the original complaint and any allied papers, as follows: (1) In cases involving...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title32-vol5/pdf/CFR-2010-title32-vol5-sec776-81.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title32-vol5/pdf/CFR-2010-title32-vol5-sec776-81.pdf"><span>32 CFR 776.81 - <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>2010-07-01</p> <p>... 32 National Defense 5 2010-07-01 2010-07-01 false <span class="hlt">Charges</span>. 776.81 Section 776.81 National Defense Department of Defense (Continued) DEPARTMENT OF THE NAVY MISCELLANEOUS RULES PROFESSIONAL CONDUCT OF... <span class="hlt">charges</span>, together with the original complaint and any allied papers, as follows: (1) In cases involving...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title32-vol5/pdf/CFR-2014-title32-vol5-sec776-81.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title32-vol5/pdf/CFR-2014-title32-vol5-sec776-81.pdf"><span>32 CFR 776.81 - <span class="hlt">Charges</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-07-01</p> <p>... 32 National Defense 5 2014-07-01 2014-07-01 false <span class="hlt">Charges</span>. 776.81 Section 776.81 National Defense Department of Defense (Continued) DEPARTMENT OF THE NAVY MISCELLANEOUS RULES PROFESSIONAL CONDUCT OF... <span class="hlt">charges</span>, together with the original complaint and any allied papers, as follows: (1) In cases involving...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title32-vol5/pdf/CFR-2012-title32-vol5-sec776-81.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title32-vol5/pdf/CFR-2012-title32-vol5-sec776-81.pdf"><span>32 CFR 776.81 - <span class="hlt">Charges</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-07-01</p> <p>... 32 National Defense 5 2012-07-01 2012-07-01 false <span class="hlt">Charges</span>. 776.81 Section 776.81 National Defense Department of Defense (Continued) DEPARTMENT OF THE NAVY MISCELLANEOUS RULES PROFESSIONAL CONDUCT OF... <span class="hlt">charges</span>, together with the original complaint and any allied papers, as follows: (1) In cases involving...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title32-vol5/pdf/CFR-2011-title32-vol5-sec776-81.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title32-vol5/pdf/CFR-2011-title32-vol5-sec776-81.pdf"><span>32 CFR 776.81 - <span class="hlt">Charges</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-07-01</p> <p>... 32 National Defense 5 2011-07-01 2011-07-01 false <span class="hlt">Charges</span>. 776.81 Section 776.81 National Defense Department of Defense (Continued) DEPARTMENT OF THE NAVY MISCELLANEOUS RULES PROFESSIONAL CONDUCT OF... <span class="hlt">charges</span>, together with the original complaint and any allied papers, as follows: (1) In cases involving...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title42-vol1/pdf/CFR-2012-title42-vol1-sec7-4.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title42-vol1/pdf/CFR-2012-title42-vol1-sec7-4.pdf"><span>42 CFR 7.4 - Schedule of <span class="hlt">charges</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-10-01</p> <p>... REFERENCE BIOLOGICAL STANDARDS AND BIOLOGICAL PREPARATIONS § 7.4 Schedule of <span class="hlt">charges</span>. The <span class="hlt">charges</span> imposed in... ingredients. <span class="hlt">Charges</span> may vary over time and between different biological standards or biological preparations... is available from the Biological Products Branch, Center for Infectious Diseases, Centers for Disease...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title47-vol1/pdf/CFR-2010-title47-vol1-sec3-45.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title47-vol1/pdf/CFR-2010-title47-vol1-sec3-45.pdf"><span>47 CFR 3.45 - Amount of <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>... 47 Telecommunication 1 2010-10-01 2010-10-01 false Amount of <span class="hlt">charges</span>. 3.45 Section 3.45... <span class="hlt">charges</span>. Accounting Authorities may <span class="hlt">charge</span> any reasonable fee for their settlement services. Settlements... International Telecommunication Regulations (ITR) taking into account the applicable ITU-T Recommendations and...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title42-vol1/pdf/CFR-2010-title42-vol1-sec7-4.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title42-vol1/pdf/CFR-2010-title42-vol1-sec7-4.pdf"><span>42 CFR 7.4 - Schedule of <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>... REFERENCE BIOLOGICAL STANDARDS AND BIOLOGICAL PREPARATIONS § 7.4 Schedule of <span class="hlt">charges</span>. The <span class="hlt">charges</span> imposed in... ingredients. <span class="hlt">Charges</span> may vary over time and between different biological standards or biological preparations... is available from the Biological Products Branch, Center for Infectious Diseases, Centers for Disease...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70025298','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70025298"><span>Determination of layer-<span class="hlt">charge</span> characteristics of smectites</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Christidis, G.E.; Eberl, D.D.</p> <p>2003-01-01</p> <p>A new method for calculation of layer <span class="hlt">charge</span> and <span class="hlt">charge</span> distribution of smectites is proposed. The method is based on comparisons between X-ray diffraction (XRD) patterns of K-saturated, ethylene glycol-solvated, oriented samples and calculated XRD patterns for three-component, mixed-layer systems. For the calculated patterns it is assumed that the measured patterns can be modeled as random interstratifications of fully expanding 17.1 Å layers, partially expanding 13.5 Å layers and non-expanding 9.98 Å layers. The technique was tested using 29 well characterized smectites. According to their XRD patterns, smectites were classified as group 1 (low-<span class="hlt">charge</span> smectites) and group 2 (high-<span class="hlt">charge</span> smectites). The boundary between the two groups is at a layer <span class="hlt">charge</span> of −0.46 equivalents per half unit-cell. Low-<span class="hlt">charge</span> smectites are dominated by 17.1 Å layers, whereas high-<span class="hlt">charge</span> smectites contain only 20% fully expandable layers on average. Smectite properties and industrial applications may be dictated by the proportion of 17.1 Å layers present. Non-expanding layers may control the behavior of smectites during weathering, facilitating the formation of illite layers after subsequent cycles of wetting and drying. The precision of the method is better than 3.5% at a layer <span class="hlt">charge</span> of −0.50; therefore the method should be useful for basic research and for industrial purposes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1109487','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1109487"><span>Integrated exhaust gas recirculation and <span class="hlt">charge</span> cooling system</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Wu, Ko-Jen</p> <p>2013-12-10</p> <p>An intake system for an internal combustion engine comprises an exhaust driven turbocharger configured to deliver compressed intake <span class="hlt">charge</span>, comprising exhaust gas from the exhaust system and ambient air, through an intake <span class="hlt">charge</span> conduit and to cylinders of the internal combustion engine. An intake <span class="hlt">charge</span> cooler is in fluid communication with the intake <span class="hlt">charge</span> conduit. A cooling system, independent of the cooling system for the internal combustion engine, is in fluid communication with the intake <span class="hlt">charge</span> cooler through a cooling system conduit. A coolant pump delivers a low temperature cooling medium from the cooling system to and through the intake <span class="hlt">charge</span> cooler for the transfer of heat from the compressed intake <span class="hlt">charge</span> thereto. A low temperature cooler receives the heated cooling medium through the cooling system conduit for the transfer or heat therefrom.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title29-vol7/pdf/CFR-2010-title29-vol7-sec1917-157.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title29-vol7/pdf/CFR-2010-title29-vol7-sec1917-157.pdf"><span>29 CFR 1917.157 - Battery <span class="hlt">charging</span> and changing.</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>2010-07-01</p> <p>... 29 Labor 7 2010-07-01 2010-07-01 false Battery <span class="hlt">charging</span> and changing. 1917.157 Section 1917.157..., DEPARTMENT OF LABOR (CONTINUED) MARINE TERMINALS Related Terminal Operations and Equipment § 1917.157 Battery <span class="hlt">charging</span> and changing. (a) Only designated persons shall change or <span class="hlt">charge</span> batteries. (b) Battery <span class="hlt">charging</span>...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title29-vol7/pdf/CFR-2011-title29-vol7-sec1917-157.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title29-vol7/pdf/CFR-2011-title29-vol7-sec1917-157.pdf"><span>29 CFR 1917.157 - Battery <span class="hlt">charging</span> and changing.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-07-01</p> <p>... 29 Labor 7 2011-07-01 2011-07-01 false Battery <span class="hlt">charging</span> and changing. 1917.157 Section 1917.157..., DEPARTMENT OF LABOR (CONTINUED) MARINE TERMINALS Related Terminal Operations and Equipment § 1917.157 Battery <span class="hlt">charging</span> and changing. (a) Only designated persons shall change or <span class="hlt">charge</span> batteries. (b) Battery <span class="hlt">charging</span>...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title29-vol7/pdf/CFR-2012-title29-vol7-sec1917-157.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title29-vol7/pdf/CFR-2012-title29-vol7-sec1917-157.pdf"><span>29 CFR 1917.157 - Battery <span class="hlt">charging</span> and changing.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-07-01</p> <p>... 29 Labor 7 2012-07-01 2012-07-01 false Battery <span class="hlt">charging</span> and changing. 1917.157 Section 1917.157..., DEPARTMENT OF LABOR (CONTINUED) MARINE TERMINALS Related Terminal Operations and Equipment § 1917.157 Battery <span class="hlt">charging</span> and changing. (a) Only designated persons shall change or <span class="hlt">charge</span> batteries. (b) Battery <span class="hlt">charging</span>...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title29-vol7/pdf/CFR-2014-title29-vol7-sec1917-157.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title29-vol7/pdf/CFR-2014-title29-vol7-sec1917-157.pdf"><span>29 CFR 1917.157 - Battery <span class="hlt">charging</span> and changing.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-07-01</p> <p>... 29 Labor 7 2014-07-01 2014-07-01 false Battery <span class="hlt">charging</span> and changing. 1917.157 Section 1917.157..., DEPARTMENT OF LABOR (CONTINUED) MARINE TERMINALS Related Terminal Operations and Equipment § 1917.157 Battery <span class="hlt">charging</span> and changing. (a) Only designated persons shall change or <span class="hlt">charge</span> batteries. (b) Battery <span class="hlt">charging</span>...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title29-vol7/pdf/CFR-2013-title29-vol7-sec1917-157.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title29-vol7/pdf/CFR-2013-title29-vol7-sec1917-157.pdf"><span>29 CFR 1917.157 - Battery <span class="hlt">charging</span> and changing.</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>2013-07-01</p> <p>... 29 Labor 7 2013-07-01 2013-07-01 false Battery <span class="hlt">charging</span> and changing. 1917.157 Section 1917.157..., DEPARTMENT OF LABOR (CONTINUED) MARINE TERMINALS Related Terminal Operations and Equipment § 1917.157 Battery <span class="hlt">charging</span> and changing. (a) Only designated persons shall change or <span class="hlt">charge</span> batteries. (b) Battery <span class="hlt">charging</span>...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5660303','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5660303"><span>Prise en <span class="hlt">charge</span> des orbitopathies dysthyroidiennes modérées et sévères: à propos de 22 cas</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Daldoul, Nadia; Knani, Leila; Gatfaoui, Faten; Mahjoub, Hechmi</p> <p>2017-01-01</p> <p>Décrire la prise en <span class="hlt">charge</span> thérapeutique des orbitopathies dysthyroidiennes modérées et sévères et évaluer par une étude statistique les facteurs associés à la neuropathie optique ainsi que les facteurs de mauvais pronostic visuel. Nous avons mené une étude rétrospective sur 22 patients présentant une ophtalmopathie dysthyroidienne modérée à sévère sur au moins un oeil, hospitalisés au service d'ophtalmologie du CHU Farhat Hached Sousse, sur une période s'étalant de 1998 à 2015. Les indications thérapeutiques sont basées sur les critères d'activité et de sévérité de l'Eugogo ainsi que l'évaluation des facteurs de mauvais pronostic visuel. L'âge moyen de nos patients était de 40 ans avec une légère prédominance masculine (54.5%). 68.2% des patients étaient en euthyroidie, 18.2% étaient tabagique. Le facteur le plus associé significativement à la neuropathie est la compression au niveau de l'apex orbitaire (P = 0.03). Le traitement était basé sur la corticothérapie intraveineuse et/ou la décompression orbitaire en fonction de l'activité et la sévérité de la maladie. L'évolution globale <span class="hlt">apr</span>ès traitement a été marquée par une amélioration des signes inflammatoires, réduction de l'exophtalmie. Le pronostic visuel était plus mauvais chez les patients plus âgés (P = 0.0001), de sexe masculin (P = 0.03) et traités par irathérapie (P = 0.04). Dans les limites d'une étude rétrospective, nos résultats étaient globalement concordants avec la littérature. L'orbitopathie dysthyroidienne reste une maladie dont l'évaluation et la prise en <span class="hlt">charge</span> thérapeutique sont non encore bien élucidées. Des études de cohortes, probablement multicentriques, sont à envisager pour améliorer la prise en <span class="hlt">charge</span>. PMID:29187926</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('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 addition, <span class="hlt">charged</span> particles heavier than protons have substantial potential clinical advantages because of their additional 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.osti.gov/biblio/1211442-optimal-decentralized-protocol-electric-vehicle-charging','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1211442-optimal-decentralized-protocol-electric-vehicle-charging"><span>Optimal Decentralized Protocol for Electric Vehicle <span class="hlt">Charging</span></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>Gan, LW; Topcu, U; Low, SH</p> <p></p> <p>We propose a decentralized algorithm to optimally schedule electric vehicle (EV) <span class="hlt">charging</span>. The algorithm exploits the elasticity of electric vehicle loads to fill the valleys in electric load profiles. We first formulate the EV <span class="hlt">charging</span> scheduling problem as an optimal control problem, whose objective is to impose a generalized notion of valley-filling, and study properties of optimal <span class="hlt">charging</span> profiles. We then give a decentralized algorithm to iteratively solve the optimal control problem. In each iteration, EVs update their <span class="hlt">charging</span> profiles according to the control signal broadcast by the utility company, and the utility company alters the control signal to guidemore » their updates. The algorithm converges to optimal <span class="hlt">charging</span> profiles (that are as "flat" as they can possibly be) irrespective of the specifications (e.g., maximum <span class="hlt">charging</span> rate and deadline) of EVs, even if EVs do not necessarily update their <span class="hlt">charging</span> profiles in every iteration, and use potentially outdated control signal when they update. Moreover, the algorithm only requires each EV solving its local problem, hence its implementation requires low computation capability. We also extend the algorithm to track a given load profile and to real-time implementation.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19910023410','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19910023410"><span>On <span class="hlt">charging</span> of snow particles in blizzard</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Shio, Hisashi</p> <p>1991-01-01</p> <p>The causes of the <span class="hlt">charge</span> polarity on the blizzard, which consisted of fractured snow crystals and ice particles, were investigated. As a result, the <span class="hlt">charging</span> 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 <span class="hlt">charge</span>, while those drifting at higher area (height 2 m) from the surface of snow field had negative <span class="hlt">charge</span>. However, during the series of blizzards two kinds of particles positively and negatively <span class="hlt">charged</span> 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 (<span class="hlt">charged</span> 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 <span class="hlt">charge</span> 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.</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 addition, 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('http://hdl.handle.net/2060/20050217199','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20050217199"><span>Lithium-Ion Cell <span class="hlt">Charge</span>-Control Unit Developed</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Reid, Concha M.; Manzo, Michelle A.; Buton, Robert M.; Gemeiner, Russel</p> <p>2005-01-01</p> <p>A lithium-ion (Li-ion) cell <span class="hlt">charge</span>-control unit was developed as part of a Li-ion cell verification program. This unit manages the complex <span class="hlt">charging</span> scheme that is required when Li-ion cells are <span class="hlt">charged</span> in series. It enables researchers to test cells together as a pack, while allowing each cell to <span class="hlt">charge</span> individually. This allows the inherent cell-to-cell variations to be addressed on a series string of cells and reduces test costs substantially in comparison to individual cell testing.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/21308448-doubly-charged-higgsinos-tevatron','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/21308448-doubly-charged-higgsinos-tevatron"><span>Doubly <span class="hlt">charged</span> Higgsinos at the Tevatron</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>Demir, Durmus A.; Frank, Mariana; Turan, Ismail</p> <p>2009-05-01</p> <p>Several supersymmetric models with extended gauge structures, motivated by either grand unification or by neutrino mass generation, predict light doubly <span class="hlt">charged</span> Higgsinos. In this work we study the signals of doubly <span class="hlt">charged</span> Higgsinos at the Tevatron in both pair- and single-production modes, and show that it is possible, especially from the events containing same-sign same-flavor isolated leptons, to disentangle the effects of doubly <span class="hlt">charged</span> Higgsinos in the Tevatron data.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/20637103-summary-update-astm-guide-charge-control-charge-referencing-techniques-ray-photoelectron-spectroscopy','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/20637103-summary-update-astm-guide-charge-control-charge-referencing-techniques-ray-photoelectron-spectroscopy"><span>Summary: Update to ASTM guide E 1523 to <span class="hlt">charge</span> control and <span class="hlt">charge</span> referencing techniques in x-ray photoelectron spectroscopy</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>Baer, D.R.</p> <p>2005-05-01</p> <p>An updated version of the American Society for Testing and Materials (ASTM) guide E 1523 to the methods to <span class="hlt">charge</span> control and <span class="hlt">charge</span> referencing techniques in x-ray photoelectron spectroscopy has been released by ASTM [Annual Book of ASTM Standards Surface Analysis (American Society for Testing and Materials, West Conshohocken, PA, 2004), Vol. 03.06]. The guide is meant to acquaint x-ray photoelectron spectroscopy (XPS) users with the various <span class="hlt">charge</span> control and <span class="hlt">charge</span> referencing techniques that are and have been used in the acquisition and interpretation of XPS data from surfaces of insulating specimens. The current guide has been expanded to includemore » new references as well as recommendations for reporting information on <span class="hlt">charge</span> control and <span class="hlt">charge</span> referencing. The previous version of the document had been published in 1997 [D. R. Baer and K. D. Bomben, J. Vac. Sci. Technol. A 16, 754 (1998)].« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=sockets&id=EJ561539','ERIC'); return false;" href="https://eric.ed.gov/?q=sockets&id=EJ561539"><span>Safeguarding Digital Library Contents: <span class="hlt">Charging</span> for Online Content.</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>Herzberg, Amir</p> <p>1998-01-01</p> <p>Investigates the need for mechanisms for <span class="hlt">charging</span> by digital libraries and other providers of online content, in particular for micropayments, i.e., <span class="hlt">charging</span> for small amounts. The SSL (Secure Socket Layer) and SET (Secure Electronic Transactions) protocols for <span class="hlt">charge</span> card payments and the MiniPay micropayment mechanism for <span class="hlt">charging</span> small amounts…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.afdc.energy.gov/fuels/electricity_stations.html','SCIGOVWS'); return false;" href="https://www.afdc.energy.gov/fuels/electricity_stations.html"><span>Alternative Fuels Data Center: Electric Vehicle <span class="hlt">Charging</span> Stations</span></a></p> <p><a target="_blank" href="http://www.science.gov/aboutsearch.html">Science.gov Websites</a></p> <p></p> <p></p> <p>Electric <em>Vehicle</em> <span class="hlt">Charging</span> Stations to someone by E-mail Share Alternative Fuels Data Center : Electric <em>Vehicle</em> <span class="hlt">Charging</span> Stations on Facebook Tweet about Alternative Fuels Data Center: Electric <em>Vehicle</em> <span class="hlt">Charging</span> Stations on Twitter Bookmark Alternative Fuels Data Center: Electric <em>Vehicle</em> <span class="hlt">Charging</span> Stations on</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title50-vol7/pdf/CFR-2010-title50-vol7-sec260-69.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title50-vol7/pdf/CFR-2010-title50-vol7-sec260-69.pdf"><span>50 CFR 260.69 - Payment fees and <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>... 50 Wildlife and Fisheries 7 2010-10-01 2010-10-01 false Payment fees and <span class="hlt">charges</span>. 260.69 Section... Fishery Products for Human Consumption Fees and <span class="hlt">Charges</span> § 260.69 Payment fees and <span class="hlt">charges</span>. Fees and... services rendered. All fees and <span class="hlt">charges</span> for any inspection service, performed pursuant to the regulations...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014NIMPB.338..101S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014NIMPB.338..101S"><span>Anatomy of <span class="hlt">charge</span>-exchange straggling</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sigmund, P.; Osmani, O.; Schinner, A.</p> <p>2014-11-01</p> <p>We have studied <span class="hlt">charge</span>-exchange straggling theoretically for swift krypton and silicon ions and five target gases in the MeV/u energy regime. We find a pronounced two-peak structure for all ion-target combinations. The peak at the highest energy appears around the velocity where the bare ion and the one-electron ion are equally abundant in the equilibrium <span class="hlt">charge</span> distribution. Correspondingly, the low-energy peak appears near the cross-over between the <span class="hlt">charge</span> fractions of the two- and the three-electron ion. The possibility of further peaks at lower energies is discussed. Our findings are compared with recent experimental results on straggling of krypton beams.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1984STIN...8632625S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1984STIN...8632625S"><span>Methods to characterize <span class="hlt">charging</span> effects</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Slots, H.</p> <p>1984-08-01</p> <p>Methods to characterize <span class="hlt">charging</span> in insulating material under high voltage dc stress, leading to electrical breakdown, are reviewed. The behavior of the <span class="hlt">charges</span> can be studied by ac loss angle measurements after application or removal of dc bias. Measurements were performed on oil-paper and oil-Mylar systems. The poor reproducibility of the measurements makes it impossible to draw more than qualitative conclusions about the <span class="hlt">charging</span> effects. With an ultrasound pressure wave the electric field distribution in a material can be determined. An alternative derivation for the transient response of a system which elucidates the influence of several parameters in a simple way is given.</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 additional 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 additional 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.gpo.gov/fdsys/pkg/CFR-2012-title29-vol4/pdf/CFR-2012-title29-vol4-sec1626-13.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title29-vol4/pdf/CFR-2012-title29-vol4-sec1626-13.pdf"><span>29 CFR 1626.13 - Withdrawal of <span class="hlt">charge</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-07-01</p> <p>... 29 Labor 4 2012-07-01 2012-07-01 false Withdrawal of <span class="hlt">charge</span>. 1626.13 Section 1626.13 Labor Regulations Relating to Labor (Continued) EQUAL EMPLOYMENT OPPORTUNITY COMMISSION PROCEDURES-AGE DISCRIMINATION IN EMPLOYMENT ACT § 1626.13 Withdrawal of <span class="hlt">charge</span>. <span class="hlt">Charging</span> parties may request withdrawal of a...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title29-vol4/pdf/CFR-2010-title29-vol4-sec1626-13.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title29-vol4/pdf/CFR-2010-title29-vol4-sec1626-13.pdf"><span>29 CFR 1626.13 - Withdrawal of <span class="hlt">charge</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>2010-07-01</p> <p>... 29 Labor 4 2010-07-01 2010-07-01 false Withdrawal of <span class="hlt">charge</span>. 1626.13 Section 1626.13 Labor Regulations Relating to Labor (Continued) EQUAL EMPLOYMENT OPPORTUNITY COMMISSION PROCEDURES-AGE DISCRIMINATION IN EMPLOYMENT ACT § 1626.13 Withdrawal of <span class="hlt">charge</span>. <span class="hlt">Charging</span> parties may request withdrawal of a...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title29-vol4/pdf/CFR-2013-title29-vol4-sec1626-13.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title29-vol4/pdf/CFR-2013-title29-vol4-sec1626-13.pdf"><span>29 CFR 1626.13 - Withdrawal of <span class="hlt">charge</span>.</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>2013-07-01</p> <p>... 29 Labor 4 2013-07-01 2013-07-01 false Withdrawal of <span class="hlt">charge</span>. 1626.13 Section 1626.13 Labor Regulations Relating to Labor (Continued) EQUAL EMPLOYMENT OPPORTUNITY COMMISSION PROCEDURES-AGE DISCRIMINATION IN EMPLOYMENT ACT § 1626.13 Withdrawal of <span class="hlt">charge</span>. <span class="hlt">Charging</span> parties may request withdrawal of a...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title29-vol4/pdf/CFR-2014-title29-vol4-sec1626-13.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title29-vol4/pdf/CFR-2014-title29-vol4-sec1626-13.pdf"><span>29 CFR 1626.13 - Withdrawal of <span class="hlt">charge</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-07-01</p> <p>... 29 Labor 4 2014-07-01 2014-07-01 false Withdrawal of <span class="hlt">charge</span>. 1626.13 Section 1626.13 Labor Regulations Relating to Labor (Continued) EQUAL EMPLOYMENT OPPORTUNITY COMMISSION PROCEDURES-AGE DISCRIMINATION IN EMPLOYMENT ACT § 1626.13 Withdrawal of <span class="hlt">charge</span>. <span class="hlt">Charging</span> parties may request withdrawal of a...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title29-vol4/pdf/CFR-2011-title29-vol4-sec1626-13.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title29-vol4/pdf/CFR-2011-title29-vol4-sec1626-13.pdf"><span>29 CFR 1626.13 - Withdrawal of <span class="hlt">charge</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-07-01</p> <p>... 29 Labor 4 2011-07-01 2011-07-01 false Withdrawal of <span class="hlt">charge</span>. 1626.13 Section 1626.13 Labor Regulations Relating to Labor (Continued) EQUAL EMPLOYMENT OPPORTUNITY COMMISSION PROCEDURES-AGE DISCRIMINATION IN EMPLOYMENT ACT § 1626.13 Withdrawal of <span class="hlt">charge</span>. <span class="hlt">Charging</span> parties may request withdrawal of a...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title18-vol2/pdf/CFR-2010-title18-vol2-sec420-42.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title18-vol2/pdf/CFR-2010-title18-vol2-sec420-42.pdf"><span>18 CFR 420.42 - Contracts; minimum <span class="hlt">charge</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>2010-04-01</p> <p>... 18 Conservation of Power and Water Resources 2 2010-04-01 2010-04-01 false Contracts; minimum <span class="hlt">charge</span>. 420.42 Section 420.42 Conservation of Power and Water Resources DELAWARE RIVER BASIN COMMISSION ADMINISTRATIVE MANUAL BASIN REGULATIONS-WATER SUPPLY <span class="hlt">CHARGES</span> <span class="hlt">Charges</span>; Exemptions § 420.42 Contracts; minimum...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29153243','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29153243"><span>The pH dependent surface <span class="hlt">charging</span> and points of zero <span class="hlt">charge</span>. VII. Update.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kosmulski, Marek</p> <p>2018-01-01</p> <p>The pristine points of zero <span class="hlt">charge</span> (PZC) and isoelectric points (IEP) of metal oxides and IEP of other materials from the recent literature, and a few older results (overlooked in previous searches) are summarized. This study is an update of the previous compilations by the same author [Surface <span class="hlt">Charging</span> and Points of Zero <span class="hlt">Charge</span>, CRC, Boca Raton, 2009; J. Colloid Interface Sci. 337 (2009) 439; 353 (2011) 1; 426 (2014) 209]. The field has been very active, but most PZC and IEP are reported for materials, which are very well-documented already (silica, alumina, titania, iron oxides). IEP of (nominally) Gd 2 O 3 , NaTaO 3 , and SrTiO 3 have been reported in the recent literature. Their IEP were not reported in older studies. Copyright © 2017 Elsevier B.V. All rights reserved.</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('http://adsabs.harvard.edu/abs/2015AdSpR..55.1710J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AdSpR..55.1710J"><span>Rover wheel <span class="hlt">charging</span> on the lunar surface</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jackson, Telana L.; Farrell, William M.; Zimmerman, Michael I.</p> <p>2015-03-01</p> <p>The environment at the Moon is dynamic, with highly variable solar wind plasma conditions at the lunar dayside, terminator, and night side regions. Moving objects such as rover wheels will <span class="hlt">charge</span> due to contact electrification with the surface, but the degree of <span class="hlt">charging</span> is controlled by the local plasma environment. Using a dynamic <span class="hlt">charging</span> model of a wheel, it is demonstrated herein that moving tires will tribocharge substantially when venturing into plasma-current starved regions such as polar craters or the lunar nightside. The surface regolith distribution and the overall effect on <span class="hlt">charge</span> accumulation of grains cohesively sticking to the rover tire has been incorporated into the model. It is shown that dust sticking can limit the overall <span class="hlt">charge</span> accumulated on the system. However <span class="hlt">charge</span> dissipation times are greatly increased in shadowed regions and can present a potential hazard to astronauts and electrical systems performing extra-vehicular activities. We show that dissipation times change with wheel composition and overall system tribocharging is dependent upon wheel velocity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26472393','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26472393"><span>Influence of the shell thickness and <span class="hlt">charge</span> distribution on the effective interaction between two like-<span class="hlt">charged</span> hollow spheres.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Angelescu, Daniel G; Caragheorgheopol, Dan</p> <p>2015-10-14</p> <p>The mean-force and the potential of the mean force between two like-<span class="hlt">charged</span> spherical shells were investigated in the salt-free limit using the primitive model and Monte Carlo simulations. Apart from an angular homogeneous distribution, a discrete <span class="hlt">charge</span> distribution where point <span class="hlt">charges</span> localized on the shell outer surface followed an icosahedral arrangement was considered. The electrostatic coupling of the model system was altered by the presence of mono-, trivalent counterions or small dendrimers, each one bearing a net <span class="hlt">charge</span> of 9 e. We analyzed in detail how the shell thickness and the radial and angular distribution of the shell <span class="hlt">charges</span> influenced the effective interaction between the shells. We found a sequence of the potential of the mean force similar to the like-<span class="hlt">charged</span> filled spheres, ranging from long-range purely repulsive to short-range purely attractive as the electrostatic coupling increased. Both types of potentials were attenuated and an attractive-to-repulsive transition occurred in the presence of trivalent counterions as a result of (i) thinning the shell or (ii) shifting the shell <span class="hlt">charge</span> from the outer towards the inner surface. The potential of the mean force became more attractive with the icosahedrally symmetric <span class="hlt">charge</span> model, and additionally, at least one shell tended to line up with 5-fold symmetry axis along the longest axis of the simulation box at the maximum attraction. The results provided a basic framework of understanding the non-specific electrostatic origin of the agglomeration and long-range assembly of the viral nanoparticles.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010PhRvA..82f2901D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010PhRvA..82f2901D"><span><span class="hlt">Charging</span> of insulators by multiply-<span class="hlt">charged</span>-ion impact probed by slowing down of fast binary-encounter electrons</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>de Filippo, E.; Lanzanó, G.; Amorini, F.; Cardella, G.; Geraci, E.; Grassi, L.; La Guidara, E.; Lombardo, I.; Politi, G.; Rizzo, F.; Russotto, P.; Volant, C.; Hagmann, S.; Rothard, H.</p> <p>2010-12-01</p> <p>The interaction of ion beams with insulators leads to <span class="hlt">charging</span>-up phenomena, which at present are under investigation in connection with guiding phenomena in nanocapillaries with possible application in nanofocused beams. We studied the <span class="hlt">charging</span> dynamics of insulating foil targets [Mylar, polypropylene (PP)] irradiated with swift ion beams (C, O, Ag, and Xe at 40, 23, 40, and 30 MeV/u, respectively) via the measurement of the slowing down of fast binary-encounter electrons. Also, sandwich targets (Mylar covered with a thin Au layer on both surfaces) and Mylar with Au on only one surface were used. Fast-electron spectra were measured by the time-of-flight method at the superconducting cyclotron of Laboratori Nazionali del Sud (LNS) Catania. The <span class="hlt">charge</span> buildup leads to target-material-dependent potentials of the order of 6.0 kV for Mylar and 2.8 kV for PP. The sandwich targets, surprisingly, show the same behavior as the insulating targets, whereas a single Au layer on the electron and ion exit side strongly suppresses the <span class="hlt">charging</span> phenomenon. The accumulated number of projectiles needed for <span class="hlt">charging</span> up is inversely proportional to electronic energy loss. Thus, the <span class="hlt">charging</span> up is directly related to emission of secondary electrons.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title24-vol2/pdf/CFR-2010-title24-vol2-sec203-270.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title24-vol2/pdf/CFR-2010-title24-vol2-sec203-270.pdf"><span>24 CFR 203.270 - Open-end insurance <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>2010-04-01</p> <p>... 24 Housing and Urban Development 2 2010-04-01 2010-04-01 false Open-end insurance <span class="hlt">charges</span>. 203.270... SINGLE FAMILY MORTGAGE INSURANCE Contract Rights and Obligations Open-End Insurance <span class="hlt">Charges</span>-All Mortgages § 203.270 Open-end insurance <span class="hlt">charges</span>. (a) Required <span class="hlt">charge</span>. In the case of an insured open-end advance...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title24-vol2/pdf/CFR-2014-title24-vol2-sec203-270.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title24-vol2/pdf/CFR-2014-title24-vol2-sec203-270.pdf"><span>24 CFR 203.270 - Open-end insurance <span class="hlt">charges</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-04-01</p> <p>... 24 Housing and Urban Development 2 2014-04-01 2014-04-01 false Open-end insurance <span class="hlt">charges</span>. 203.270... SINGLE FAMILY MORTGAGE INSURANCE Contract Rights and Obligations Open-End Insurance <span class="hlt">Charges</span>-All Mortgages § 203.270 Open-end insurance <span class="hlt">charges</span>. (a) Required <span class="hlt">charge</span>. In the case of an insured open-end advance...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title24-vol2/pdf/CFR-2011-title24-vol2-sec203-270.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title24-vol2/pdf/CFR-2011-title24-vol2-sec203-270.pdf"><span>24 CFR 203.270 - Open-end insurance <span class="hlt">charges</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-04-01</p> <p>... 24 Housing and Urban Development 2 2011-04-01 2011-04-01 false Open-end insurance <span class="hlt">charges</span>. 203.270... SINGLE FAMILY MORTGAGE INSURANCE Contract Rights and Obligations Open-End Insurance <span class="hlt">Charges</span>-All Mortgages § 203.270 Open-end insurance <span class="hlt">charges</span>. (a) Required <span class="hlt">charge</span>. In the case of an insured open-end advance...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title24-vol2/pdf/CFR-2012-title24-vol2-sec203-270.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title24-vol2/pdf/CFR-2012-title24-vol2-sec203-270.pdf"><span>24 CFR 203.270 - Open-end insurance <span class="hlt">charges</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-04-01</p> <p>... 24 Housing and Urban Development 2 2012-04-01 2012-04-01 false Open-end insurance <span class="hlt">charges</span>. 203.270... SINGLE FAMILY MORTGAGE INSURANCE Contract Rights and Obligations Open-End Insurance <span class="hlt">Charges</span>-All Mortgages § 203.270 Open-end insurance <span class="hlt">charges</span>. (a) Required <span class="hlt">charge</span>. In the case of an insured open-end advance...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title24-vol2/pdf/CFR-2013-title24-vol2-sec203-270.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title24-vol2/pdf/CFR-2013-title24-vol2-sec203-270.pdf"><span>24 CFR 203.270 - Open-end insurance <span class="hlt">charges</span>.</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>2013-04-01</p> <p>... 24 Housing and Urban Development 2 2013-04-01 2013-04-01 false Open-end insurance <span class="hlt">charges</span>. 203.270... SINGLE FAMILY MORTGAGE INSURANCE Contract Rights and Obligations Open-End Insurance <span class="hlt">Charges</span>-All Mortgages § 203.270 Open-end insurance <span class="hlt">charges</span>. (a) Required <span class="hlt">charge</span>. In the case of an insured open-end advance...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009PhDT.......150C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009PhDT.......150C"><span>Diffusive <span class="hlt">charge</span> transport in graphene</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chen, Jianhao</p> <p></p> <p>The physical mechanisms limiting the mobility of graphene on SiO 2 are studied and printed graphene devices on a flexible substrate are realized. Intentional addition of <span class="hlt">charged</span> scattering impurities is used to study the effects of <span class="hlt">charged</span> impurities. Atomic-scale defects are created by noble-gas ions irradiation to study the effect of unitary scatterers. The results show that <span class="hlt">charged</span> impurities and atomic-scale defects both lead to conductivity linear in density in graphene, with a scattering magnitude that agrees quantitatively with theoretical estimates. While <span class="hlt">charged</span> impurities cause intravalley scattering and induce a small change in the minimum conductivity, defects in graphene scatter electrons between the valleys and suppress the minimum conductivity below the metallic limit. Temperature-dependent measurements show that longitudinal acoustic phonons in graphene produce a small resistivity which is linear in temperature and independent of carrier density; at higher temperatures, polar optical phonons of the SiO2 substrate give rise to an activated, carrier density-dependent resistivity. Graphene is also made into high mobility transparent and flexible field effect device via the transfer-printing method. Together the results paint a complete picture of <span class="hlt">charge</span> carrier transport in graphene on SiO2 in the diffusive regime, and show the promise of graphene as a novel electronic material that have potential applications not only on conventional inorganic substrates, but also on flexible substrates.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/865387','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/865387"><span>Electrostatic wire for stabilizing a <span class="hlt">charged</span> particle beam</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Prono, Daniel S.; Caporaso, George J.; Briggs, Richard J.</p> <p>1985-01-01</p> <p>In combination with a <span class="hlt">charged</span> particle beam generator and accelerator, apparatus and method are provided for stabilizing a beam of electrically <span class="hlt">charged</span> particles. A guiding means, disposed within the particle beam, has an electric <span class="hlt">charge</span> induced upon it by the <span class="hlt">charged</span> particle beam. Because the sign of the electric <span class="hlt">charge</span> on the guiding means and the sign of the particle beam are opposite, the particles are attracted toward and cluster around the guiding means to thereby stabilize the particle beam as it travels.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25858625','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25858625"><span><span class="hlt">Charge</span> transport in electrically doped amorphous organic semiconductors.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Yoo, Seung-Jun; Kim, Jang-Joo</p> <p>2015-06-01</p> <p>This article reviews recent progress on <span class="hlt">charge</span> generation by doping and its influence on the carrier mobility in organic semiconductors (OSs). The doping induced <span class="hlt">charge</span> generation efficiency is generally low in OSs which was explained by the integer <span class="hlt">charge</span> transfer model and the hybrid <span class="hlt">charge</span> transfer model. The ionized dopants formed by <span class="hlt">charge</span> transfer between hosts and dopants can act as Coulomb traps for mobile <span class="hlt">charges</span>, and the presence of Coulomb traps in OSs broadens the density of states (DOS) in doped organic films. The Coulomb traps strongly reduce the carrier hopping rate and thereby change the carrier mobility, which was confirmed by experiments in recent years. In order to fully understand the doping mechanism in OSs, further quantitative and systematic analyses of <span class="hlt">charge</span> transport characteristics must be accomplished. © 2015 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015JPhCS.635a2027G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015JPhCS.635a2027G"><span>Interaction of highly <span class="hlt">charged</span> ions with carbon nano membranes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gruber, Elisabeth; Wilhelm, Richard A.; Smejkal, Valerie; Heller, René; Facsko, Stefan; Aumayr, Friedrich</p> <p>2015-09-01</p> <p><span class="hlt">Charge</span> state and energy loss measurements of slow highly <span class="hlt">charged</span> ions (HCIs) after transmission through nanometer and sub-nanometer thin membranes are presented. Direct transmission measurements through carbon nano membranes (CNMs) show an unexpected bimodal exit <span class="hlt">charge</span> state distribution, accompanied by <span class="hlt">charge</span> exchange dependent energy loss. The energy loss of ions in CNMs with large <span class="hlt">charge</span> loss shows a quadratic dependency on the incident <span class="hlt">charge</span> state, indicating <span class="hlt">charge</span> state dependent stopping force values. Another access to the exit <span class="hlt">charge</span> state distribution is given by irradiating stacks of CNMs and investigating each layer of the stack with high resolution imaging techniques like transmission electron microscopy (TEM) and helium ion microscopy (HIM) independently. The observation of pores created in all of the layers confirms the assumption derived from the transmission measurements that the two separated <span class="hlt">charge</span> state distributions reflect two different impact parameter regimes, i.e. close collision with large <span class="hlt">charge</span> exchange and distant collisions with weak ion-target interaction.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title20-vol2/pdf/CFR-2010-title20-vol2-sec416-1565.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title20-vol2/pdf/CFR-2010-title20-vol2-sec416-1565.pdf"><span>20 CFR 416.1565 - Hearing on <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>2010-04-01</p> <p>... DISABLED Representation of Parties § 416.1565 Hearing on <span class="hlt">charges</span>. (a) Scheduling the hearing. If the Deputy... complete record of the proceedings at the hearing made. (l) Representation. The representative, as the... of <span class="hlt">charges</span>. The hearing officer may dismiss the <span class="hlt">charges</span> in the event of the death of the...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title20-vol2/pdf/CFR-2010-title20-vol2-sec404-1765.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title20-vol2/pdf/CFR-2010-title20-vol2-sec404-1765.pdf"><span>20 CFR 404.1765 - Hearing on <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>2010-04-01</p> <p>...- ) Representation of Parties § 404.1765 Hearing on <span class="hlt">charges</span>. (a) Scheduling the hearing. If the Deputy Commissioner... complete record of the proceedings at the hearing made. (l) Representation. The representative, as the... of <span class="hlt">charges</span>. The hearing officer may dismiss the <span class="hlt">charges</span> in the event of the death of the...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=syndrome&pg=2&id=EJ1165942','ERIC'); return false;" href="https://eric.ed.gov/?q=syndrome&pg=2&id=EJ1165942"><span>The Education of Learners with <span class="hlt">CHARGE</span> Syndrome</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>Deuce, Gail</p> <p>2017-01-01</p> <p><span class="hlt">CHARGE</span> syndrome, although a low incidence condition, is now recognised as a leading cause of congenital deafblindness among genetic conditions. Anecdotal reporting has suggested that learners with <span class="hlt">CHARGE</span> syndrome are distinct from the wider deafblind population. This study investigates the education of learners with <span class="hlt">CHARGE</span> syndrome, while also…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011JASMS..22.1052D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011JASMS..22.1052D"><span>Negative Ion CID Fragmentation of O-linked Oligosaccharide Aldoses—<span class="hlt">Charge</span> Induced and <span class="hlt">Charge</span> Remote Fragmentation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Doohan, Roisin A.; Hayes, Catherine A.; Harhen, Brendan; Karlsson, Niclas Göran</p> <p>2011-06-01</p> <p>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 <span class="hlt">charge</span> 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 <span class="hlt">charges</span> 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 <span class="hlt">charged</span> GalNAc residue followed by <span class="hlt">charge</span> remote fragmentation similar to the acidic oligosaccharides. In addition, A-type fragments generated by <span class="hlt">charge</span> induced fragmentation of neutral oligosaccharides were observed when the <span class="hlt">charge</span> 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.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22220767-quantum-classical-dissipation-charged-particles','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22220767-quantum-classical-dissipation-charged-particles"><span>Quantum and classical dissipation of <span class="hlt">charged</span> particles</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>Ibarra-Sierra, V.G.; Anzaldo-Meneses, A.; Cardoso, J.L.</p> <p>2013-08-15</p> <p>A Hamiltonian approach is presented to study the two dimensional motion of damped electric <span class="hlt">charges</span> in time dependent electromagnetic fields. The classical and the corresponding quantum mechanical problems are solved for particular cases using canonical transformations applied to Hamiltonians for a particle with variable mass. Green’s function is constructed and, from it, the motion of a Gaussian wave packet is studied in detail. -- Highlights: •Hamiltonian of a damped <span class="hlt">charged</span> particle in time dependent electromagnetic fields. •Exact Green’s function of a <span class="hlt">charged</span> particle in time dependent electromagnetic fields. •Time evolution of a Gaussian wave packet of a damped <span class="hlt">charged</span> particle.more » •Classical and quantum dynamics of a damped electric <span class="hlt">charge</span>.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014JAP...116a4902H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014JAP...116a4902H"><span>Polarization-induced surface <span class="hlt">charges</span> in hydroxyapatite ceramics</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Horiuchi, N.; Nakaguki, S.; Wada, N.; Nozaki, K.; Nakamura, M.; Nagai, A.; Katayama, K.; Yamashita, K.</p> <p>2014-07-01</p> <p>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 <span class="hlt">charge</span> on HAp would be a key advance in the development of the material for tissue engineering. We demonstrate here that surface <span class="hlt">charge</span> can be induced by an electrical poling process using the Kelvin method. Positive and negative <span class="hlt">charges</span> were induced on the HAp surface in response to the applied electric field in the poling process. The surface <span class="hlt">charging</span> is attributed to dipole polarization that is homogeneously distributed in HAp. Additionally, the surface <span class="hlt">charging</span> is considered to originate from the organization of OH- ions into a polar phase in the structure.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20030002524&hterms=pixel+array+detector&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dpixel%2Barray%2Bdetector','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20030002524&hterms=pixel+array+detector&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dpixel%2Barray%2Bdetector"><span><span class="hlt">Charge</span> Sharing and <span class="hlt">Charge</span> Loss in a Cadmium-Zinc-Telluride Fine-Pixel Detector Array</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gaskin, J. A.; Sharma, D. P.; Ramsey, B. D.; Six, N. Frank (Technical Monitor)</p> <p>2002-01-01</p> <p>Because of its high atomic number, room temperature operation, low noise, and high spatial resolution a Cadmium-Zinc-Telluride (CZT) multi-pixel detector is ideal for hard x-ray astrophysical observation. As part of on-going research at MSFC (Marshall Space Flight Center) to develop multi-pixel CdZnTe detectors for this purpose, we have measured <span class="hlt">charge</span> sharing and <span class="hlt">charge</span> loss for a 4x4 (750micron pitch), lmm thick pixel array and modeled these results using a Monte-Carlo simulation. This model was then used to predict the amount of <span class="hlt">charge</span> sharing for a much finer pixel array (with a 300micron pitch). Future work will enable us to compare the simulated results for the finer array to measured values.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=planets&pg=4&id=EJ1015465','ERIC'); return false;" href="https://eric.ed.gov/?q=planets&pg=4&id=EJ1015465"><span>The Orbit of Water Droplets around <span class="hlt">Charged</span> Rod</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>Ferstl, Andrew; Burns, Andrew</p> <p>2013-01-01</p> <p>The motion of <span class="hlt">charges</span> around a centrally <span class="hlt">charged</span> object is often compared to gravitational orbits (such as satellites around planets). Recently, a video taken by astronaut Don Pettit onboard the International Space Station shows water droplets orbiting a <span class="hlt">charged</span> knitting needle. Here we attempt to model this motion and estimate the <span class="hlt">charges</span> on the…</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('https://www.osti.gov/biblio/22063892-charge-breeding-simulations-radioactive-ion-beam-production','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22063892-charge-breeding-simulations-radioactive-ion-beam-production"><span><span class="hlt">Charge</span> breeding simulations for radioactive ion beam production</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>Variale, V.; Raino, A. C.; Clauser, T.</p> <p>2012-02-15</p> <p>The <span class="hlt">charge</span> breeding technique is used for radioactive ion beam (RIB) production in order of optimizing the re-acceleration of the radioactive element ions produced by a primary beam in a thick target. <span class="hlt">Charge</span> breeding is achieved by means of a device capable of increasing the ion <span class="hlt">charge</span> state from 1+ to a desired value n+. In order to get high intensity RIB, experiments with <span class="hlt">charge</span> breeding of very high efficiency could be required. To reach this goal, the <span class="hlt">charge</span> breeding simulation could help to optimize the high <span class="hlt">charge</span> state production efficiency by finding more proper parameters for the radioactive 1+more » ions. In this paper a device based on an electron beam ion source (EBIS) is considered. In order to study that problem, a code already developed for studying the ion selective containment in an EBIS with RF quadrupoles, BRICTEST, has been modified to simulate the ion <span class="hlt">charge</span> state breeding rate for different 1+ ion injection conditions. Particularly, the <span class="hlt">charge</span> breeding simulations for an EBIS with a hollow electron beam have been studied.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140011783','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140011783"><span>An Investigation of Low Earth Orbit Internal <span class="hlt">Charging</span></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; Willis, Emily</p> <p>2014-01-01</p> <p>Internal <span class="hlt">charging</span> is not generally considered a threat in low Earth orbit due to the relatively short exposure times and low flux of electrons with energies of a few MeV encountered in typical orbits. There are configurations, however, where insulators and ungrounded conductors used on the outside of a spacecraft hull may <span class="hlt">charge</span> when exposed to much lower energy electrons of some 100's keV in a process that is better characterized as internal <span class="hlt">charging</span> than surface <span class="hlt">charging</span>. We investigate the conditions required for this internal <span class="hlt">charging</span> process to occur in low Earth orbit using a one-dimensional <span class="hlt">charging</span> model and evaluate the environments for which the process may be a threat to spacecraft.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title29-vol4/pdf/CFR-2012-title29-vol4-sec1626-11.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title29-vol4/pdf/CFR-2012-title29-vol4-sec1626-11.pdf"><span>29 CFR 1626.11 - Notice of <span class="hlt">charge</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-07-01</p> <p>... 29 Labor 4 2012-07-01 2012-07-01 false Notice of <span class="hlt">charge</span>. 1626.11 Section 1626.11 Labor Regulations Relating to Labor (Continued) EQUAL EMPLOYMENT OPPORTUNITY COMMISSION PROCEDURES-AGE DISCRIMINATION IN EMPLOYMENT ACT § 1626.11 Notice of <span class="hlt">charge</span>. Upon receipt of a <span class="hlt">charge</span>, the Commission shall promptly notify the...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title29-vol4/pdf/CFR-2013-title29-vol4-sec1626-11.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title29-vol4/pdf/CFR-2013-title29-vol4-sec1626-11.pdf"><span>29 CFR 1626.11 - Notice of <span class="hlt">charge</span>.</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>2013-07-01</p> <p>... 29 Labor 4 2013-07-01 2013-07-01 false Notice of <span class="hlt">charge</span>. 1626.11 Section 1626.11 Labor Regulations Relating to Labor (Continued) EQUAL EMPLOYMENT OPPORTUNITY COMMISSION PROCEDURES-AGE DISCRIMINATION IN EMPLOYMENT ACT § 1626.11 Notice of <span class="hlt">charge</span>. Upon receipt of a <span class="hlt">charge</span>, the Commission shall promptly notify the...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title29-vol4/pdf/CFR-2011-title29-vol4-sec1626-11.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title29-vol4/pdf/CFR-2011-title29-vol4-sec1626-11.pdf"><span>29 CFR 1626.11 - Notice of <span class="hlt">charge</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-07-01</p> <p>... 29 Labor 4 2011-07-01 2011-07-01 false Notice of <span class="hlt">charge</span>. 1626.11 Section 1626.11 Labor Regulations Relating to Labor (Continued) EQUAL EMPLOYMENT OPPORTUNITY COMMISSION PROCEDURES-AGE DISCRIMINATION IN EMPLOYMENT ACT § 1626.11 Notice of <span class="hlt">charge</span>. Upon receipt of a <span class="hlt">charge</span>, the Commission shall promptly notify the...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title29-vol4/pdf/CFR-2014-title29-vol4-sec1626-11.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title29-vol4/pdf/CFR-2014-title29-vol4-sec1626-11.pdf"><span>29 CFR 1626.11 - Notice of <span class="hlt">charge</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-07-01</p> <p>... 29 Labor 4 2014-07-01 2014-07-01 false Notice of <span class="hlt">charge</span>. 1626.11 Section 1626.11 Labor Regulations Relating to Labor (Continued) EQUAL EMPLOYMENT OPPORTUNITY COMMISSION PROCEDURES-AGE DISCRIMINATION IN EMPLOYMENT ACT § 1626.11 Notice of <span class="hlt">charge</span>. Upon receipt of a <span class="hlt">charge</span>, the Commission shall promptly notify the...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title29-vol4/pdf/CFR-2010-title29-vol4-sec1626-11.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title29-vol4/pdf/CFR-2010-title29-vol4-sec1626-11.pdf"><span>29 CFR 1626.11 - Notice of <span class="hlt">charge</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>2010-07-01</p> <p>... 29 Labor 4 2010-07-01 2010-07-01 false Notice of <span class="hlt">charge</span>. 1626.11 Section 1626.11 Labor Regulations Relating to Labor (Continued) EQUAL EMPLOYMENT OPPORTUNITY COMMISSION PROCEDURES-AGE DISCRIMINATION IN EMPLOYMENT ACT § 1626.11 Notice of <span class="hlt">charge</span>. Upon receipt of a <span class="hlt">charge</span>, the Commission shall promptly notify the...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title4-vol1/pdf/CFR-2012-title4-vol1-sec81-7.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title4-vol1/pdf/CFR-2012-title4-vol1-sec81-7.pdf"><span>4 CFR 81.7 - Fees and <span class="hlt">charges</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-01-01</p> <p>... noncommercial scientific institutions not seeking records for commercial use will be <span class="hlt">charged</span> only for document... ACCOUNTABILITY OFFICE RECORDS PUBLIC AVAILABILITY OF GOVERNMENT ACCOUNTABILITY OFFICE RECORDS § 81.7 Fees and <span class="hlt">charges</span>. (a) No fee or <span class="hlt">charge</span> will be made for: (1) Records provided under this part when the direct costs...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title48-vol1/pdf/CFR-2013-title48-vol1-sec32-608-1.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title48-vol1/pdf/CFR-2013-title48-vol1-sec32-608-1.pdf"><span>48 CFR 32.608-1 - Interest <span class="hlt">charges</span>.</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>2013-10-01</p> <p>... 48 Federal Acquisition Regulations System 1 2013-10-01 2013-10-01 false Interest <span class="hlt">charges</span>. 32.608-1... REQUIREMENTS CONTRACT FINANCING Contract Debts 32.608-1 Interest <span class="hlt">charges</span>. Unless specified otherwise in the clause at 52.232-17, Interest, interest <span class="hlt">charges</span> shall apply to any contract debt unpaid after 30 days...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title48-vol1/pdf/CFR-2011-title48-vol1-sec32-608-1.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title48-vol1/pdf/CFR-2011-title48-vol1-sec32-608-1.pdf"><span>48 CFR 32.608-1 - Interest <span class="hlt">charges</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-10-01</p> <p>... 48 Federal Acquisition Regulations System 1 2011-10-01 2011-10-01 false Interest <span class="hlt">charges</span>. 32.608-1... REQUIREMENTS CONTRACT FINANCING Contract Debts 32.608-1 Interest <span class="hlt">charges</span>. Unless specified otherwise in the clause at 52.232-17, Interest, interest <span class="hlt">charges</span> shall apply to any contract debt unpaid after 30 days...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title48-vol1/pdf/CFR-2012-title48-vol1-sec32-608-1.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title48-vol1/pdf/CFR-2012-title48-vol1-sec32-608-1.pdf"><span>48 CFR 32.608-1 - Interest <span class="hlt">charges</span>.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-10-01</p> <p>... 48 Federal Acquisition Regulations System 1 2012-10-01 2012-10-01 false Interest <span class="hlt">charges</span>. 32.608-1... REQUIREMENTS CONTRACT FINANCING Contract Debts 32.608-1 Interest <span class="hlt">charges</span>. Unless specified otherwise in the clause at 52.232-17, Interest, interest <span class="hlt">charges</span> shall apply to any contract debt unpaid after 30 days...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2001RPPh...64..383M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2001RPPh...64..383M"><span><span class="hlt">Charge</span> and spin in low-dimensional cuprates</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Maekawa, Sadamichi; Tohyama, Takami</p> <p>2001-03-01</p> <p>One of the central issues in the study of high-temperature superconducting cuprates which are composed of two-dimensional (2D) CuO2 planes is whether the 2D systems with strong electron correlation behave as a Fermi liquid or a non-Fermi-liquid-like one-dimensional (1D) system with electron correlation. In this article, we start with the detailed examination of the electronic structure in cuprates and study theoretically the spin and <span class="hlt">charge</span> dynamics in 1D and 2D cuprates. The theoretical background of spin-<span class="hlt">charge</span> separation in the 1D model systems including the Hubbard and t-J models is presented. The first direct observation of collective modes of spin and <span class="hlt">charge</span> excitations in a 1D cuprate, which are called spinons and holons respectively, in angle-resolved photoemission spectroscopy (ARPES) experiments is reviewed in the light of the theoretical results based on the numerically exact-diagonalization method. The <span class="hlt">charge</span> and spin dynamics in 1D insulating cuprates is also discussed in connection with the spin-<span class="hlt">charge</span> separation. The arguments are extended to the 2D cuprates, and the unique aspects of the electronic properties of high-temperature superconductors are discussed. Special emphasis is placed on the d-wave-like excitations in insulating 2D cuprates observed in ARPES experiments. We explain how the excitations are caused by the spin-<span class="hlt">charge</span> separation. The <span class="hlt">charge</span> stripes observed in the underdoped cuprates are examined in connection with spin-<span class="hlt">charge</span> separation in real space.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017MS%26E..184a2023H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017MS%26E..184a2023H"><span>Modelling of an advanced <span class="hlt">charging</span> system for electric vehicles</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hassan Jaafar, Abdul; Rahman, Ataur; Mohiuddin, A. K. M.; Rashid, Mahbubur</p> <p>2017-03-01</p> <p>Climate Change is recognized as one of the greatest environmental problem facing the World today and it has long been appreciated by governments that reducing the impact of the internal combustion (IC) engine powered motor vehicle has an important part to play in addressing this threat. In Malaysia, IC engine powered motor vehicle accounts almost 90% of the national greenhouse gas (GHG) emissions. The need to reduce the emission is paramount, as Malaysia has pledged to reduce 40% of CO2 intensity by 2020 from 2005 level by 25% of improvement in average fuel consumption. The introduction of electric vehicles (EVs) is one of the initiatives. However in terms of percentage, the electric vehicles have not been commonly used by people nowadays and one of the reasons is lack in <span class="hlt">charging</span> infrastructure especially when cars are on the road. The aim of this study is to simulate and model an advanced <span class="hlt">charging</span> system for the <span class="hlt">charging</span> infrastructure of EVs/HEVs all over the nation with slow <span class="hlt">charging</span> mode with <span class="hlt">charging</span> current 25 A, medium <span class="hlt">charging</span> mode with <span class="hlt">charging</span> current 50 A and fast <span class="hlt">charging</span> mode with <span class="hlt">charging</span> current 100 A. The slow <span class="hlt">charging</span> mode is proposed for residence, medium <span class="hlt">charging</span> mode for office parking lots, and fast <span class="hlt">charging</span> mode is called fast <span class="hlt">charging</span> track for <span class="hlt">charging</span> station on road. With three modes charger topology, consumers could choose a suitable mode for their car based on their need. The simulation and experiment of advanced <span class="hlt">charging</span> system has been conducted on a scale down battery pack of nominal voltage of 3.75 V and capacity of 1020 mAh. Result shows that the battery could be <span class="hlt">charging</span> less than 1 hour with fast <span class="hlt">charging</span> mode. However, due to limitation of Tenaga Nasional Berhad (TNB) power grid, the maximum 50 A current is considered to be the optimized passive mode for the EV’s battery <span class="hlt">charging</span> system. The developed advanced charger prototype performance has been compared with the simulation result and conventional charger performance, the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.afdc.energy.gov/case/2809','SCIGOVWS'); return false;" href="https://www.afdc.energy.gov/case/2809"><span>Alternative Fuels Data Center: Workplace <span class="hlt">Charging</span> at Leased Facilities</span></a></p> <p><a target="_blank" href="http://www.science.gov/aboutsearch.html">Science.gov Websites</a></p> <p></p> <p></p> <p><span class="hlt">Charges</span> Up Tenants and <em>Property</em> Managers</A> Workplace <span class="hlt">Charging</span> at Leased Facilities <span class="hlt">Charges</span> Up Tenants and <em>Property</em> Managers to someone by E-mail Share Alternative Fuels Data Center: Workplace <span class="hlt">Charging</span> at Leased Facilities <span class="hlt">Charges</span> Up Tenants and <em>Property</em> Managers on Facebook Tweet about Alternative</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title25-vol2/pdf/CFR-2010-title25-vol2-sec700-105.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title25-vol2/pdf/CFR-2010-title25-vol2-sec700-105.pdf"><span>25 CFR 700.105 - Utility <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>2010-04-01</p> <p>... Policies and Instructions Definitions § 700.105 Utility <span class="hlt">charges</span>. Utility <span class="hlt">charges</span> means the cost for heat, lighting, hot water, electricity, natural gas, butane, propane, wood, coal or other fuels water, sewer and...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25743890','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25743890"><span>Surface <span class="hlt">charge</span> effects in protein adsorption on nanodiamonds.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Aramesh, M; Shimoni, O; Ostrikov, K; Prawer, S; Cervenka, J</p> <p>2015-03-19</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 negatively (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 negatively <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.</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 negative 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 negative 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.osti.gov/biblio/22390853-first-charge-breeding-results-caribu-ebis','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22390853-first-charge-breeding-results-caribu-ebis"><span>First <span class="hlt">charge</span> breeding results at CARIBU EBIS</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>Kondrashev, S., E-mail: kondrashev@anl.gov; Barcikowski, A., E-mail: kondrashev@anl.gov; Dickerson, C., E-mail: kondrashev@anl.gov</p> <p></p> <p>The Electron Beam Ion Source (EBIS) developed to breed CARIBU radioactive beams at ATLAS is currently in the off-line commissioning stage. The beam commissioning is being performed using a low emittance surface ionization source producing singly-<span class="hlt">charged</span> cesium ions. The primary goal of the off-line commissioning is the demonstration of high-efficiency <span class="hlt">charge</span> breeding in the pulsed injection mode. An overview of the final design of the CARIBU EBIS <span class="hlt">charge</span> breeder, the off-line commissioning installation and the first results on <span class="hlt">charge</span> breeding of stable cesium ions are presented and discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20060047792&hterms=scintillator&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dscintillator','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20060047792&hterms=scintillator&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dscintillator"><span>Enhancing the ATIC <span class="hlt">Charge</span> Resolution</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Guzik, T. G.; Adams, J. H., Jr.; Ahn, H. S.; Bashindzhagyan, G. L.; Batkov, K. E.; Chang, J.; Christl, M.; Fazely, A. R.; Ganel, O.; Gunashingha, R. M.</p> <p>2006-01-01</p> <p>The Advanced Thin Ionization Calorimeter (ATIC) experiment measures the energy spectra of elements, from H to Fe, in the energy region from about 100 GeV to tens of TeV. The ATIC instrument was flown twice in long-duration balloon flights around the South Pole; the ATIC-1 test flight during Dec. 2000 - Jan. 2001 and the ATIC-2 science flight during Dec. 2002 - Jan. 2003. Analyses of both datasets have, to date, relied upon the highly segmented Silicon Matrix (SiM) detector to separate the incident cosmic ray from the calorimeter backscatter and to identify the <span class="hlt">charge</span>. This method has worked well, enabling ATIC to separate protons from helium and to resolve all the major species up through iron. This <span class="hlt">charge</span> resolution can be significantly improved by restricting the analysis to particle trajectories that pass through two SiM pixels at the cost of using only a fraction of the potential instrument geometry. However, immediately below the SiM is the two layer SI hodoscope (x, y) consisting of Bicron BC-408 plastic scintillator 2 cm wide, 1 cm thick, 88.2 cm long strips viewed by Hamamatsu R5611 photomultiplier tubes on each end of each strip. The primary purpose of the ATIC hodoscopes is to provide a fast trigger, and each hodoscope includes two crossed layers of strips (42 per layer in the case of Sl) providing supplemental particle trajectory information. The hodoscope readout electronics were designed to provide reasonable <span class="hlt">charge</span> resolution over the dynamic range from protons through iron. This presentation discusses the S 1 hodoscope energy deposit calibrations, examines the <span class="hlt">charge</span> resolution possible with this detector and investigates combining the S1 and SiM <span class="hlt">charge</span> measurements to improve the overall ATIC <span class="hlt">charge</span> resolution while minimizing degradation of the instrument geometry.</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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