Science.gov

Sample records for maron tiina agan

  1. Rectal biopsy

    MedlinePlus

    ... References Fry RD, Mahmoud NN, Maron, Bleier JIS. Colon and rectum. ... MD, FACS, general surgery practice specializing in breast cancer, Virginia Mason Medical Center, Seattle, WA. Also reviewed ...

  2. Takotsubo (Stress) Cardiomyopathy

    MedlinePlus

    ... Circulation . 2005 ; 111 : 472 – 479 . OpenUrl Abstract / FREE Full Text Wittstein IS , Thiemann DR , Lima JA , Baughman KL , ... syndromes . Circulation . 2008 ; 118 : 397 – 409 . OpenUrl FREE Full Text Sharkey SW , Lesser JR , Maron MS , Maron BJ . ...

  3. 78 FR 20104 - Notice of Receipt of Requests for Amendments To Delete Uses in Certain Pesticide Registrations

    Federal Register 2010, 2011, 2012, 2013, 2014

    2013-04-03

    ... INFORMATION CONTACT: Christopher Green, Information Technology and Resources Management Division (7502P... Mold Fungicide. Pentachloronitrobenzene & farms, & other Turf Propiconazole. grown areas (athletic fields, cemeteries, parks & commercial turf). 11603-52 Agan Imazethapyr Imazethapyr Field...

  4. Total proctocolectomy and ileal - anal pouch

    MedlinePlus

    Restorative proctocolectomy; Ileal-anal resection; Ileal-anal pouch; J-pouch; S-pouch; Pelvic pouch; Ileal-anal pouch; Ileal ... RD, Mahmoud N, Maron DJ, Ross HM, Rombeau J. Colon and rectum. In: Townsend CM, Beauchamp RD, ...

  5. Properties of amorphous GaN from first-principles simulations

    NASA Astrophysics Data System (ADS)

    Cai, B.; Drabold, D. A.

    2011-08-01

    Amorphous GaN (a-GaN) models are obtained from first-principles simulations. We compare four a-GaN models generated by “melt-and-quench” and the computer alchemy method. We find that most atoms tend to be fourfold, and a chemically ordered continuous random network is the ideal structure for a-GaN albeit with some coordination defects. Where the electronic structure is concerned, the gap is predicted to be less than 1.0 eV, underestimated as usual by a density functional calculation. We observe a highly localized valence tail and a remarkably delocalized exponential conduction tail in all models generated. Based upon these results, we speculate on potential differences in n- and p-type doping. The structural origin of tail and defect states is discussed. The vibrational density of states and dielectric function are computed and seem consistent with experiment.

  6. PIALA 2004: Maron In Read Im Jeje Ej Ad Kojatdikdik, Library Ko Rej Jikin Kakurmool Kojatdikdik In Im Jolet Eo Ad Ej Bwinnid--Literacy Our Hope, Libraries Our Scope and Heritage Our Property (14th, Majuro Atoll, Marshall Islands, November 16-19, 2004) and PIALA 2005: Kasrpacsr Misenge Ac Etwack Lutu--Resources Today and Learning Tomorrow (15th, Tofol, Kosrae, Federated States of Micronesia, November 8-10, 2005). Selected Papers from the Pacific Islands Association of Libraries and Archives Annual Conferences

    ERIC Educational Resources Information Center

    Cohen, Arlene, Ed.

    2006-01-01

    This publication follows the tradition of publishing selected papers from PIALA annual conferences, however, for the first time, two PIALA conferences (PIALA 2004 and PIALA 2005) are published in one volume, containing papers from both events. Both conferences featured papers by local Micronesian and Pacific Islands experts, as well as presenters…

  7. The Developmental Course of Supportive Dyadic Coping in Couples

    ERIC Educational Resources Information Center

    Johnson, Matthew D.; Horne, Rebecca M.; Galovan, Adam M.

    2016-01-01

    Drawing from a relational developmental systems (RDS) perspective (Lerner, Agans, DeSouza, & Gasca, 2013) and data from 1,427 continuously partnered young adult and midlife mixed-sex couples over the first 5 years of the German Panel Analysis of Intimate Relationships and Family Dynamics (pairfam), this study examined the developmental course…

  8. 78 FR 40027 - Novaluron; Pesticide Tolerances

    Federal Register 2010, 2011, 2012, 2013, 2014

    2013-07-03

    ... peanut and soybean, seed. Makhteshim-Agan of North America requested these tolerances under the Federal... on peanuts at 0.01 parts per million (ppm) and soybean, seed at 0.06 ppm. That document referenced a... for soybean, seed. The reason for this change is explained in Unit IV.C. III. Aggregate...

  9. Commotio Cordis: Should Physical Educators and Coaches Be Concerned?

    ERIC Educational Resources Information Center

    Berhow, Katie J.; Hansen, Pamela J.; Terbizan, Donna J.

    2012-01-01

    A collapse and cardiac arrest from Commotio Cordis can occur instantaneously from a relatively modest and nonpenetrating blow to the chest in the absence of underlying cardiovascular disease or structural injury to the chest wall or heart itself (Maron, 1998). It is important to note that this collapse could be instantaneous or proceeded by brief…

  10. Evaluation of a Test Article in the Salmonella typhimurium/Ecscherichia coli Plate Incorporation Mutation Assay in the Presence and Absence of Induced Rat Liver S-9. Test Article: Ethylenediamine Dinitrate (EDDN)

    DTIC Science & Technology

    2009-02-25

    Sigma Chemical Company St. Louis, MO 63178 Storage Conditions: Room Temperature CAS No: 67-68-S Lot No.: 10S8SCH Expiration Date: January 31,2012...TISSUE: Liver REFERENCE: Maron. D & Ames, B, Mutot Res 113: 173. 1983 STORAGE: At orbelow-70oC INDUCING AGENT(s): Aroclor 1254 ( Monsanto KI..615

  11. 40 CFR 799.9510 - TSCA bacterial reverse mutation test.

    Code of Federal Regulations, 2011 CFR

    2011-07-01

    ... Mutagenicity Test. Mutation Research. 31, 347-364 (1975). (2) Maron, D.M. and Ames, B.N. Revised Methods for the Salmonella Mutagenicity Test. Mutation Research. 113, 173-215 (1983). (3) Gatehouse, D., Haworth..., E. Recommendations for the Performance of Bacterial Mutation Assays. Mutation Research. 312,...

  12. Tropical Cyclone Report, 1993

    DTIC Science & Technology

    1993-01-01

    Office of Naval Research (;rant AN00014-914J1721 STAFF JOINT TYPHOON WARNING CENTER LCDR ANTHONY A. MARTINEZ USN TDO. DEPUTY DIRECTOR LCDR TERESA M...OEJFN TDA. GRAPHICS AGAN ANDRESG.GRANT USN TDA, GRAPHICS UNIVERSITY OF GUAM / JTWC RESEARCH LIAISON DR MARK A. LANDER TROPICAL CYCLONE RESEARCH MR...CHARLES P. GUARD TROPICAL CYCLONE RESEARCH * TRANSFERRED DURING 1993 ** ACTIVE DUTY TRAINING S~ii FOREWORD The Annual Tropical Cyclone Report is past four

  13. Correlation Between the System Capabilities Analytic Process (SCAP) and the Missions and Means Framework (MMF)

    DTIC Science & Technology

    2013-05-01

    Correlation Between the System Capabilities Analytic Process (SCAP) and the Missions and Means Framework ( MMF ) by Kevin S. Agan ARL-TR...ARL-TR-6455 May 2013 Correlation Between the System Capabilities Analytic Process (SCAP) and the Missions and Means Framework ( MMF ) Kevin...Analytic Process (SCAP) and the Missions and Means Framework ( MMF ) 5a. CONTRACT NUMBER 5b. GRANT NUMBER 5c. PROGRAM ELEMENT NUMBER 6. AUTHOR(S

  14. Characterization of nonpolar a-plane InGaN/GaN multiple quantum well using double nanopillar SiO2 mask

    NASA Astrophysics Data System (ADS)

    Son, Ji-Su; Honda, Yoshio; Yamaguchi, Masahito; Amano, Hiroshi

    2014-01-01

    The characteristics of nonpolar a-plane (11\\bar{2}0) GaN (a-GaN) grown using single and double nanopillar SiO2 masks were investigated. The two nanopillar SiO2 masks were directly fabricated on an r-plane sapphire substrate and a-GaN by the epitaxial lateral overgrowth (ELOG) technique. Through the use of the single and double nanopillar SiO2 masks, the crystalline quality and optical properties of a-GaN were markedly improved because of the nanoscale ELOG effect and a number of voids in the single and double nanopillar SiO2 mask areas in comparison with the planar sample. The submicron pit densities of the planar, single, and double nanopillar mask samples were ˜2 × 109, ˜7 × 108, and ˜4 × 108 cm-2, respectively. The internal quantum efficiency (IQE) values at room temperature of three-period InGaN/GaN multiple quantum wells (MQWs) grown using the planar, single, and double nanopillar masks were 45, 60, and 68% at a carrier concentration of 1.0 × 1018 cm-3, respectively.

  15. Enhanced UV detection by non-polar epitaxial GaN films

    SciTech Connect

    Mukundan, Shruti; Chandan, Greeshma; Mohan, Lokesh; Krupanidhi, S. B.; Roul, Basanta; Shetty, Arjun

    2015-12-15

    Nonpolar a-GaN (11-20) epilayers were grown on r-plane (1-102) sapphire substrates using plasma assisted molecular beam epitaxy. High resolution x-ray diffractometer confirmed the orientation of the grown film. Effect of the Ga/N ratio on the morphology and strain of a-GaN epilayers was compared and the best condition was obtained for the nitrogen flow of 1 sccm. Atomic force microscopy was used to analyze the surface morphology while the strain in the film was quantitatively measured using Raman spectroscopy and qualitatively analyzed by reciprocal space mapping technique. UV photo response of a-GaN film was measured after fabricating a metal-semiconductor-metal structure over the film with gold metal. The external quantum efficiency of the photodetectors fabricated in the (0002) polar and (11-20) nonpolar growth directions were compared in terms of responsivity and nonpolar GaN showed the best sensitivity at the cost of comparatively slow response time.

  16. Neuro-Linguistic Programming: Eye Movements as Indicators of Representational Systems.

    DTIC Science & Technology

    1984-09-01

    Elizabeth A. Beck, "Test of the Eye Movement Hypothesis of Neurolinguistic Programing : A Rebuttal of Conclu- sions," Perceptual and Motor Skills, 58: 175...Meta Publications, 1980. 64 .. .] .! S ~ ~ ~ ~ 1 - ----. 14. Maron, Davida, " Neurolinguistic Programming : The Answer to Change? Training and Development... Neurolinguistic Programming ," Perceptual and Motor Skills, 51: 230 (April 1980). 65 VITA Captain William H. Moore was born on 22 October 1949. He

  17. Differences in Cardiac Parameters Among Elite Rowers and Subelite Rowers

    DTIC Science & Technology

    2010-01-01

    changes in cardiac structure and function. Left ventricular (LV) hyper- trophy and dilation (6,26), right ventricular (RV) dilation (9,35), and left...athletes relevance to differentiating physiologic left ventricular hypertrophy from hyper- trophic cardiomyopathy . J Am Coll Cardiol. 2008;51(23):2256–62...6): 700–2, A9. 27. Pelliccia A, Culasso F, Di Paolo FM, Maron BJ. Physiologic left ventricular cavity dilatation in elite athletes. Ann Intern Med

  18. The U.S. Footprint on the Arabian Peninsula: Can We Avoid a Repeat of the Pullout from Saudi Arabia?

    DTIC Science & Technology

    2009-12-01

    Arabia? 6. AUTHOR( S ) David Paul Marone Jr. 5. FUNDING NUMBERS 7. PERFORMING ORGANIZATION NAME( S ) AND ADDRESS(ES) Naval Postgraduate School Monterey...CA 93943-5000 8. PERFORMING ORGANIZATION REPORT NUMBER 9. SPONSORING /MONITORING AGENCY NAME( S ) AND ADDRESS(ES) N/A 10. SPONSORING...was that U.S. troops had desecrated Saudi holy lands. American women driving automobiles, service members seen urinating in public, and shirts

  19. Evaluation of a Test Article in the Salmonella typhimurium/Escherichia coli Plate Incorporation Mutation Assay in the Presence and Absence of Induced Rat Liver S-9. Test Article 3-Nitro-1,2,4-Triazol-5-one (NTO)

    DTIC Science & Technology

    2008-10-17

    controls are presented below: Source: Sigma Chemical Company St. Louis, MO 63178 Storage Conditions: Room Temperature CAS No: 67-68-5 Lot No...8217; INDUCING AGEN1’Oj’fA:toOI6r 1254 ( Monsanto ,KL61S) 500 mg/kgi.p; ltEFERENCE: Maron. P -& Ames B MUtat Resl13:173.1983 S’l’ORAGEI At or below" 70°C

  20. Morphological and microstructural evolution in the two-step growth of nonpolar a-plane GaN on r-plane sapphire

    NASA Astrophysics Data System (ADS)

    Sun, Qian; Kong, Bo Hyun; Yerino, Christopher D.; Ko, Tsung-Shine; Leung, Benjamin; Cho, Hyung Koun; Han, Jung

    2009-12-01

    In this paper, we report a detailed study on the evolution of surface morphology and microstructure of nonpolar a-plane GaN (a-GaN) through controlled growth interruptions. Microscopy imaging shows that the two-step a-GaN growth went through a roughening-recovery process. The first-step growth (under high V/III and high pressure) produced a rough surface with tall mesas separated by voids. The second-step growth (under low V/III and low pressure) promoted the lateral growth and filled up the voids. Striations that formed during the island coalescence persisted throughout the second-step growth, but could be relieved by an additional third-step growth. The morphological evolution was explained according to the kinetic Wulff plots. The microstructure of the a-GaN films was investigated by transmission electron microscopy (TEM) and x-ray rocking curve analysis. Most of the extended defects observed in the plan-view TEM images were I1 type basal-plane stacking faults (BSFs) and their associated partial dislocations (PDs). It is found that the bending of PDs (at the inclined/vertical growth fronts) within the basal plane toward the m-axes was responsible for the substantial reduction in threading PDs and the increase in BSF dimension. Based on a careful correlation between the morphological evolution and the microstructure development, we proposed a model explaining the possible mechanisms for the great reduction in defect density during the two-step growth process.

  1. L-Leucyl-L-Leucine Methyl Ester Treatment of Canine Marrow and Peripheral Blood Cells

    DTIC Science & Technology

    1988-11-01

    comple- OMe or MeOll treament of 7-day B-MIX generated CTL (day 7). merit, and incubated agan for 60 run. After washing twice in medium, CThe "mt mixed...Gir A-vermea-bost disease in dogs and man: C 5 10 15 20 25 30 3 the Seattlesexprience. lmmusiRevlSSSSft21&. Day post Trensplant 2. Stosh I. Critical...with Lsu-Leu-OMe-treate mtologous marrow. 3. Koragol R. Sprant J. LAWla graft-vermin-boat disease after bone The ordiinate indicte the absolute

  2. Intense Ion Beam Generation, Plasma Radiation Source and Plasma Opening Switch Research

    DTIC Science & Technology

    1989-04-01

    ion source on the 150 kV, ls pulse , ifl LONG- SHOT pulsed power generator under NRL support. The completion of this task 2 will demonstrate both higher...following paragraph. This research is continuing under a new NRL-supported grant. 3 The POS system is pulsed by a 1.9MAF Scyllac capacitor charged to 50 kV...electric field measurements made in a surface flashover MID using emission spectroscopy by Maron et al.’ This LIF potential measuring technique could

  3. The genetic basis of hypertrophic cardiomyopathy in cats and humans.

    PubMed

    Kittleson, Mark D; Meurs, Kathryn M; Harris, Samantha P

    2015-12-01

    Mutations in genes that encode for muscle sarcomeric proteins have been identified in humans and two breeds of domestic cats with hypertrophic cardiomyopathy (HCM). This article reviews the history, genetics, and pathogenesis of HCM in the two species in order to give veterinarians a perspective on the genetics of HCM. Hypertrophic cardiomyopathy in people is a genetic disease that has been called a disease of the sarcomere because the preponderance of mutations identified that cause HCM are in genes that encode for sarcomeric proteins (Maron and Maron, 2013). Sarcomeres are the basic contractile units of muscle and thus sarcomeric proteins are responsible for the strength, speed, and extent of muscle contraction. In people with HCM, the two most common genes affected by HCM mutations are the myosin heavy chain gene (MYH7), the gene that encodes for the motor protein β-myosin heavy chain (the sarcomeric protein that splits ATP to generate force), and the cardiac myosin binding protein-C gene (MYBPC3), a gene that encodes for the closely related structural and regulatory protein, cardiac myosin binding protein-C (cMyBP-C). To date, the two mutations linked to HCM in domestic cats (one each in Maine Coon and Ragdoll breeds) also occur in MYBPC3 (Meurs et al., 2005, 2007). This is a review of the genetics of HCM in both humans and domestic cats that focuses on the aspects of human genetics that are germane to veterinarians and on all aspects of feline HCM genetics.

  4. Control of Nanostructues in Ultrahigh-Strength Steels

    DTIC Science & Technology

    1990-08-31

    1.0 at 16 hr. tempering. 400 W4) .E ____________________Measured Composition (a/ o ) Nominal Composition (a/ o ) C 0.656 + 0.15 0.73 Mo 0.054 + 0.14 0.62 Cr ...UMOSIR -- 0650-520-H407 ~ ( AFOSR-TR 9 01 0 NAME Of WEUFORMiNG ORGANILOTION 6 OPPICESYMSOO 7g. NAMS O .,%0Q06RaNZ .AGAN- AVIN Northwestern University Air...D.C. 20332-6448 NAMEt 00 UO𔃾ONOIO. 00!9 ’CC SYMSOO. S. e~CIIt ,NIT~t.MINV 109S~TICATION Nt.IM6EA ORGANIZATION itY o 𔃺ule) ps -- it AFOSR-89-0356

  5. Nonpolar GaN grown on Si by hydride vapor phase epitaxy using anodized Al nanomask

    NASA Astrophysics Data System (ADS)

    Polyakov, A. Y.; Markov, A. V.; Mezhennyi, M. V.; Govorkov, A. V.; Pavlov, V. F.; Smirnov, N. B.; Donskov, A. A.; D'yakonov, L. I.; Kozlova, Y. P.; Malakhov, S. S.; Yugova, T. G.; Osinsky, V. I.; Gorokh, G. G.; Lyahova, N. N.; Mityukhlyaev, V. B.; Pearton, S. J.

    2009-01-01

    GaN growth by the hydride vapor phase technique on (100) Si substrates masked by porous Al anodic oxide is described. The masks were prepared by vacuum deposition of Al with subsequent anodic oxidation in dilute sorrel acid. The grown GaN layer is nonpolar, with (112¯0) a-orientation and a full width at half maximum of the (112¯0) reflection below 500 arc sec and showing small anisotropy. This result is comparable with the results obtained for a-GaN growth using selective epitaxy or advanced buffer growth routines. Microcathodoluminescence spectra of the grown films confirm a low density of stacking faults. Possible growth mechanisms are discussed.

  6. Effects of size at birth, childhood growth patterns and growth hormone treatment on leukocyte telomere length

    PubMed Central

    Smeets, Carolina C. J.; Codd, Veryan; Denniff, Matthew; Samani, Nilesh J.; Hokken-Koelega, Anita C. S.

    2017-01-01

    Background Small size at birth and rapid growth in early life are associated with increased risk of cardiovascular disease in later life. Short children born small for gestational age (SGA) are treated with growth hormone (GH), inducing catch-up in length. Leukocyte telomere length (LTL) is a marker of biological age and shorter LTL is associated with increased risk of cardiovascular disease. Objectives To investigate whether LTL is influenced by birth size, childhood growth and long-term GH treatment. Methods We analyzed LTL in 545 young adults with differences in birth size and childhood growth patterns. Previously GH-treated young adults born SGA (SGA-GH) were compared to untreated short SGA (SGA-S), SGA with spontaneous catch-up to a normal body size (SGA-CU), and appropriate for gestational age with a normal body size (AGA-NS). LTL was measured using a quantitative PCR assay. Results We found a positive association between birth length and LTL (p = 0.04), and a trend towards a positive association between birth weight and LTL (p = 0.08), after adjustments for gender, age, gestational age and adult body size. Weight gain during infancy and childhood and fat mass percentage were not associated with LTL. Female gender and gestational age were positively associated with LTL, and smoking negatively. After adjustments for gender, age and gestational age, SGA-GH had a similar LTL as SGA-S (p = 0.11), SGA-CU (p = 0.80), and AGA-NS (p = 0.30). Conclusions Larger size at birth is positively associated with LTL in young adulthood. Growth patterns during infancy and childhood are not associated with LTL. Previously GH-treated young adults born SGA have similar LTL as untreated short SGA, SGA with spontaneous catch-up and AGA born controls, indicating no adverse effects of GH-induced catch-up in height on LTL. PMID:28178350

  7. Electrons and phonons in amorphous semiconductors

    NASA Astrophysics Data System (ADS)

    Prasai, Kiran; Biswas, Parthapratim; Drabold, D. A.

    2016-07-01

    The coupling between lattice vibrations and electrons is one of the central concepts of condensed matter physics. The subject has been deeply studied for crystalline materials, but far less so for amorphous and glassy materials, which are among the most important for applications. In this paper, we explore the electron-lattice coupling using current tools of a first-principles computer simulation. We choose three materials to illustrate the phenomena: amorphous silicon (a-Si), amorphous selenium (a-Se) and amorphous gallium nitride (a-GaN). In each case, we show that there is a strong correlation between the localization of electron states and the magnitude of thermally induced fluctuations in energy eigenvalues obtained from the density-functional theory (i.e. Kohn-Sham eigenvalues). We provide a heuristic theory to explain these observations. The case of a-GaN, a topologically disordered partly ionic insulator, is distinctive compared to the covalent amorphous examples. Next, we explore the consequences of changing the charge state of a system as a proxy for tracking photo-induced structural changes in the materials. Where transport is concerned, we lend insight into the Meyer-Neldel compensation rule and discuss a thermally averaged Kubo-Greenwood formula as a means to estimate electrical conductivity and especially its temperature dependence. We close by showing how the optical gap of an amorphous semiconductor can be computationally engineered with the judicious use of Hellmann-Feynman forces (associated with a few defect states) using molecular dynamics simulations. These forces can be used to close or open an optical gap, and identify a structure with a prescribed gap. We use the approach with plane-wave density functional methods to identify a low-energy amorphous phase of silicon including several coordination defects, yet with a gap close to that of good quality a-Si models.

  8. Analysis of Hexanitrostilbene (HNS) and Dipicryethane (DPE) for Mutagenicity by the Ames/Salmonella Assay

    SciTech Connect

    Wu, R; Felton, J

    2007-10-12

    The Ames/Salmonella assay, developed by Professor Bruce Ames at the University of California, Berkeley, is a rapid and sensitive assay for detecting mutagenicity of various chemical compounds (Maron and Ames, 1983). It is a widely accepted short-term assay for detecting chemicals that induce mutations in the histidine (his) gene of Salmonella typhimurium. This is a reverse mutation assay that detects the mutational reversion of his-dependent Salmonella to the his-independent counterpart. Thereby, mutagenic compounds will increase the frequency of occurrence of his-independent bacterial colonies. The assay utilizes the specific genetically constructed strains of bacteria either with or without mammalian metabolic activation enzymes (S9), Aroclor induced rat liver homogenate to assess the mutagenicity of different compounds. In this study, we will use the Ames/Salmonella assay to investigate the mutagenicity of Hexanitrostilbene (HNS) from both Bofors and Pantex, and Dipicryethane (DPE).

  9. Candidates for Pulsars with Gigahertz-Peaked Spectra

    NASA Astrophysics Data System (ADS)

    Tarczewski, L.; Kijak, J.; Lewandowski, W.

    2012-12-01

    Kijak et al. (2011) provided a definite evidence for a new type of pulsar radio spectra. These spectra show the maximum flux above 1 GHz and their energy decreases below 1 GHz, producing a positive spectral index at lower frequencies. They called these objects the gigahertz-peaked spectra (GPS) pulsars. We study a spectrum of radio pulsars and try to find pulsars with the turn-over effect at high frequencies. We created a database of candidates for pulsars with GPS effect using Maron et al. (2000) and ATNF database (Manchester et al. 2005), and also using recent papers where flux measurements were published (for example Bates et al. 2011). As a result a set of 22 candidates for pulsars with GPS was found.

  10. Earthquake Simulator Finds Tremor Triggers

    SciTech Connect

    Johnson, Paul

    2015-03-27

    Using a novel device that simulates earthquakes in a laboratory setting, a Los Alamos researcher has found that seismic waves-the sounds radiated from earthquakes-can induce earthquake aftershocks, often long after a quake has subsided. The research provides insight into how earthquakes may be triggered and how they recur. Los Alamos researcher Paul Johnson and colleague Chris Marone at Penn State have discovered how wave energy can be stored in certain types of granular materials-like the type found along certain fault lines across the globe-and how this stored energy can suddenly be released as an earthquake when hit by relatively small seismic waves far beyond the traditional “aftershock zone” of a main quake. Perhaps most surprising, researchers have found that the release of energy can occur minutes, hours, or even days after the sound waves pass; the cause of the delay remains a tantalizing mystery.

  11. Earthquake Simulator Finds Tremor Triggers

    ScienceCinema

    Johnson, Paul

    2016-07-12

    Using a novel device that simulates earthquakes in a laboratory setting, a Los Alamos researcher has found that seismic waves-the sounds radiated from earthquakes-can induce earthquake aftershocks, often long after a quake has subsided. The research provides insight into how earthquakes may be triggered and how they recur. Los Alamos researcher Paul Johnson and colleague Chris Marone at Penn State have discovered how wave energy can be stored in certain types of granular materials-like the type found along certain fault lines across the globe-and how this stored energy can suddenly be released as an earthquake when hit by relatively small seismic waves far beyond the traditional “aftershock zone” of a main quake. Perhaps most surprising, researchers have found that the release of energy can occur minutes, hours, or even days after the sound waves pass; the cause of the delay remains a tantalizing mystery.

  12. Sediment yield from gullies, riparian mass wasting and bank erosion in the Upper Konto catchment, East Java, Indonesia

    NASA Astrophysics Data System (ADS)

    Rijsdijk, Anton; Bruijnzeel, L. A. (Sampurno); Prins, Th. M.

    2007-06-01

    Upland watershed rehabilitation programmes in Indonesia have faced increased scrutiny for not delivering the desired reductions in downstream sedimentation rates. Partly this reflects the fact that conservation measures have not been widely adopted or maintained by upland farmers, mainly for socio-economic reasons. Another potential explanation is that sediment contributions by gullying, (riparian) mass wasting and bank erosion have been seriously underestimated or even ignored. This paper presents estimates of sediment contributions by gullies, riparian mass wasting and bank erosion in the upland volcanic Konto catchment, East Java. Runoff and sediment yield from gullies were studied in two areas with contrasting soils and land use. Gullies in the Maron area (few gullies, Andic Cambisols, maize and rice cultivation on stable broad-based terraces) were related to improper drainage of trails, roads and yards. In the Binangsri area (more widespread gullying, Eutric Cambisols, onion cultivation on forward-sloping terraces), gullying was further enhanced by the practice of downslope furrowing to promote field drainage. Estimated annual sediment yields from the two areas were strikingly different at 22-26 and 50-87 Mg ha - 1 , respectively. Riparian mass wasting was estimated to contribute ca. 4% of total sediment yield at Maron and 8-19% in the main gully system at Binangsri, with the higher value in the latter case representing the effect of extreme rainfall in the latter half of the rainy season. Short-term wet season rates of gully wall retreat at Binangsri suggested a contribution by bank erosion of ca. 3% (8% including extreme events). As such, 11-27% of the annual sediment yield at Binangsri was estimated to have come from sources other than surface erosion. Substantial volumes of sediment (29-107 Mg km - 1 of river length) were also added to streams bordered by irrigated rice fields ( sawah) in non-gullied areas, mainly through the collapse of the lowermost

  13. Effect of temperature on frictional behavior of smectite and illite: Implication for the updip limit of seismogenic zone along subduction thrust

    NASA Astrophysics Data System (ADS)

    Kubo, T.; Katayama, I.

    2014-12-01

    Along plate boundary subduction thrusts, the transformation of smectite to illite within fault gouge at temperatures of ~150C is one of the key mineralogical changes thought to control the updip limit of seismicity. Saffer and Marone (2003) reported illite shale exhibited only velocity-strengthening behavior, whereas illite is widely expected to be velocity-weakening behavior. The limitation of their experiments were temperature, in which the frictional experiments were csrried out at room temperature, although the updip limit of seismogenic zone is thermally controlled that occurs at temperature around 150C. Therefore, in this study, we determined the effect of temperature of frictional properties of smectite and illite and discuss whether the smectite-illite transition accounts for the updip limit of seismogenic zone along subduction thrust. In the frictional experiments, we determined the velocity dependence of sliding friction, which is a key parameter for stable or unstable sliding. After steady-state sliding, the loading velocity of 3 μm/s was abruptly changed to 33 μm/s in each frictional experiments to determine the velocity dependence of these clay minerals. The velocity dependence of both smectite and illite at room temperature shows always positive at normal stress higher than 40 MPa, which is similar to the results of Saffer and Marone (2003). However, at temperature of 200C, illite shows negative values of (a-b), suggesting that illite exhibits unstable velocity-weakening behavior. den Hartog et al. (2012) also showed the velocity-weakening for illite gouge by high temperature ring shear experiments, but the transition from velocity strengthening to weakening occurs at temperature around 250C. These results explain that smectite is potentially aseismic for stable sliding at the subduction thrust, whereas illite becomes seismic due to a negative velocity dependence and unstable sliding at high temperatures. Thus, the smectite-illite transition has a

  14. Desensitization of the insulin receptor by antireceptor antibodies in vivo is blocked by treatment of mice with beta-adrenergic agonists.

    PubMed

    Elias, D; Rapoport, M; Cohen, I R; Shechter, Y

    1988-06-01

    In previous studies we reported that immunization of mice with ungulate insulins induced the development of antiinsulin antibodies, which include an idiotype that appeared to recognize the part of the insulin molecule recognized by the hormone receptor. The antiinsulin antibodies of this idiotype were replaced spontaneously by antiidiotypic antibodies. The antiidiotypic antibodies, which persisted for about 14 d, mimicked insulin and functioned as antibodies to the insulin receptor. They induced down regulation, desensitization and refractoriness of the insulin receptor and disturbances in glucose homeostasis in vivo (Shechter, Y., D. Elias, R. Maron, and I.R. Cohen., 1984; Elias, D., R. Maron, I.R. Cohen, and Y. Shechter. 1984, J. Biol. Chem. 259: 6411-6419). We now report that effects of the antiidiotypic antibodies on the insulin receptor effector system can be modified pharmacologically. Administration of the beta-adrenergic agonist isoproterenol during the period of insulin resistance (days 26-40 after primary immunization), largely restored fat cell responsiveness to insulin, and eliminated the appearance of fasting hyperglycemia. This restoration appeared to be caused by inhibition of both insulin receptor desensitization and refractoriness. In contrast, down regulation of insulin receptors was not reversed by isoproterenol treatment in vivo. The effects of treatment with isoproterenol persisted for 2-4 d after termination of treatment. The beta-antagonist, propranolol and more so, the beta 1a-antagonist metoprolol, specifically blocked the effect of isoproterenol at a molar ratio of 3-10:1. Oral administration of the cAMP phosphodiesterase inhibitor, aminophylline, was also effective in inhibiting the development of desensitization in fat cells. These results indicate that treatment with beta 1-adrenergic agonists in vivo, or other agents that elevate cellular cAMP levels, can inhibit the development of the "postbinding" defects induced by insulin

  15. A microphysical interpretation of the rate-and-state friction direct effect: implications for the seismic cycle

    NASA Astrophysics Data System (ADS)

    van den Ende, Martijn; Niemeijer, André; Spiers, Christopher

    2015-04-01

    For many years, empirical rate-and-state friction laws have been successfully applied to describe the transient frictional behaviour of fault zones, as observed in laboratory experiments and in nature. However, the rate-and-state friction parameters and equations are still poorly understood in terms of the underlying processes that operate at a micro-scale. In addition, there exist large discrepancies between lab-derived values and estimated values for natural fault zones. Because of these discrepancies, extrapolation of the frictional behaviour from sample-scale to the spatial and temporal scales of natural faults is non-trivial. Most notably, there is only a small theoretical basis for the near-instantaneous increase in friction after a sudden increase in sliding velocity (known as the direct effect). Marone et al. (1990) observed a positive relationship between the direct effect and dilatation in quartz gouges. However, the magnitude of the dilatation was significantly higher than expected based on the change in friction, which they explained by non-coaxial dilatation. In more recent years, Beeler et al. (2007) used a normalisation scheme to show that in the case of phyllosilicates, the magnitude of the direct effect is comparable to the stress required for dislocation glide. However, dislocation glide does not explain a-values for "hard" minerals such as quartz and calcite, especially when fluid-rock interactions are rapid. To address these issues, room temperature velocity stepping experiments have been conducted on granular calcite, and granular rock salt as an analogue for quartz under hydrothermal conditions. These experiments clearly demonstrate that the magnitude of the direct effect is much larger in gouges where pressure solution rates are high and deformation is distributed. A large contribution of dilatation to the magnitude of the direct effect becomes apparent in these gouges. In contrast, calcite gouges in which pressure solution is slow, show a

  16. Analog earthquakes: Friction experiments with bulk solids and implications for fault dynamics

    NASA Astrophysics Data System (ADS)

    Rosenau, M.; Klinkmueller, M.; Oppelt, A.; Kemnitz, H.; Oncken, O.; Schreurs, G.

    2008-12-01

    We report on friction experiments on dry bulk solids used to simulate slow ("aseismic") and fast ("seismic") slip in analog laboratory experiments. Ring shear tests have been performed at typical experimental conditions, i.e. in the very low stress regime (normal loads < 0.02 MPa, shear velocities 0.05 - 25 mm/min, T = 23°), and compared to similar tests at higher stresses (Mair and Marone 1999; Mair et al., 2002). Friction tests have been complemented with scanning electron microscope analysis to explore the control of particle characteristics (size, shape, sorting, roughness) on the strength and stability of frictional deformation. By varying the ratio between particle size and displacement we aim at simulating different brittle deformation mechanisms: Fine-grained material (sand, glass beads, sugar, salt) exposed to relatively fast shear undergoes distributed granular flow (DGF) including particle rotation, dilation and sliding. Rather slow shear of coarse material (rice) is accommodated mainly by localized particle boundary sliding (LBS). Both mechanisms are capable to produce frictional instabilities resulting in stick-slip motion. We found that frictional strength during DGF is controlled by particle shape: the frictional coefficient increases with the amount of angular particles consistent with previous findings by Mair et al. (2002) in the high stress regime (> 5 MPa). Also consistent with their work, unstable slip during DGF occurs if well-sorted and isometric particles dominate presumably controlled by the breakdown of force bridges. Frictional strength and stability during LBS seems to be controlled by surface roughness consistent with the concept of asperities. For particle surfaces with a scale-invariant roughness similar to natural faults, the critical distance over which slip has to accelerate to become unstable is not constant but increases with "interseismic" sliding velocity both during LBS (this study) and DGF (Mair and Marone, 1999). We found

  17. Current evidence for a modulation of low back pain by human genetic variants.

    PubMed

    Tegeder, Irmgard; Lötsch, Jörn

    2009-08-01

    The manifestation of chronic back pain depends on structural, psychosocial, occupational and genetic influences. Heritability estimates for back pain range from 30% to 45%. Genetic influences are caused by genes affecting intervertebral disc degeneration or the immune response and genes involved in pain perception, signalling and psychological processing. This inter-individual variability which is partly due to genetic differences would require an individualized pain management to prevent the transition from acute to chronic back pain or improve the outcome. The genetic profile may help to define patients at high risk for chronic pain. We summarize genetic factors that (i) impact on intervertebral disc stability, namely Collagen IX, COL9A3, COL11A1, COL11A2, COL1A1, aggrecan (AGAN), cartilage intermediate layer protein, vitamin D receptor, metalloproteinsase-3 (MMP3), MMP9, and thrombospondin-2, (ii) modify inflammation, namely interleukin-1 (IL-1) locus genes and IL-6 and (iii) and pain signalling namely guanine triphosphate (GTP) cyclohydrolase 1, catechol-O-methyltransferase, mu opioid receptor (OPMR1), melanocortin 1 receptor (MC1R), transient receptor potential channel A1 and fatty acid amide hydrolase and analgesic drug metabolism (cytochrome P450 [CYP]2D6, CYP2C9).

  18. Dislocation- and crystallographic-dependent photoelectrochemical wet etching of gallium nitride

    NASA Astrophysics Data System (ADS)

    Gao, Y.; Craven, M. D.; Speck, J. S.; Den Baars, S. P.; Hu, E. L.

    2004-04-01

    Polarity and dislocation dependence study of photoelectrochemical wet etching on GaN was carried out on lateral epitaxial overgrown nonpolar (112¯0)a-GaN/(11¯02)r-plane sapphire substrate. This LEO nonpolar GaN sample has low dislocation density Ga- and N-faces exposed horizontally in opposite directions, which can be exposed to identical etching conditions for both polarity and dislocation dependence study. It is observed that N-face GaN is essentially much chemically active than Ga-face GaN, which shows the hexagonal pyramids with {101¯1¯} facets on the etched N face. No obvious etching was observed on Ga face in the same etch condition. As for dislocation dependence, the "wing" (low dislocation density) region was etched faster than the "window" (high dislocation density) region. Smooth etched surfaces were formed with the (1¯1¯22¯) facet as an etch stop plane both on Ga and N-wing region.

  19. Defect reduction in (112_O) a-plane GaN by two-stage epitaxiallateral overgrowth

    SciTech Connect

    Ni, X.; Ozgur, U.; Fu, Y.; Biyikli, N.; Xie, J.; Baski, A.A.; Morkoc, H.; Liliental-Weber, Z.

    2006-10-20

    In the epitaxial lateral overgrowth (ELO) of (11{bar 2}0) a-plane GaN, the uneven growth rates of two opposing wings, Ga- and N-wings, makes the coalescence of two neighboring wings more difficult than that in c-plane GaN. We report a two-stage growth method to get uniformly coalesced epitaxial lateral overgrown a-plane GaN using metalorganic chemical vapor deposition (MOCVD) by employing relatively lower growth temperature in the first step followed by enhanced lateral growth in the second. Using this method, the height differences between Ga-polar and N-polar wings at the coalescence front could be reduced, thereby making the coalescence of two wings much easier. Transmission electron microscopy (TEM) showed that the threading dislocation density in the wing areas was 1.0x10{sup 8}cm{sup -2}, more than two orders of magnitude lower than that in the window areas (4.2x10{sup 10}cm{sup -2}). However, high density of basal stacking faults of 1.2x104 cm-1 was still observed in the wing areas as compared to c-plane GaN. Atomic force microscopy and photoluminescence measurements on the coalesced ELO a-GaN sample also indicated improved material quality.

  20. Anisotropic strain relaxation and the resulting degree of polarization by one- and two-step growth in nonpolar a-plane GaN grown on r-sapphire substrate

    SciTech Connect

    Feng, Shih-Wei Chen, Yu-Yu; Lai, Chih-Ming; Tu, Li-Wei; Han, Jung

    2013-12-21

    Anisotropic strain relaxation and the resulting degree of polarization of the electronic transition in nonpolar a-plane GaN using one- and two-step growth are studied. By using two-step growth, a slower coalescence and a longer roughening-recovery process lead to larger anisotropic strain relaxation, a less striated surface, and lower densities of basal stacking fault (BSF) and prismatic stacking fault (PSF). It is suggested that anisotropic in-plane strains, surface striation, and BSF and PSF densities in nonpolar a-GaN are consequences of the rate of coalescence, the period of roughening-recovery process, and the degree of anisotropic strain relaxation. In addition, the two-step growth mode can enhance the degree of polarization of the electronic transition. The simulation results of the k⋅p perturbation approach show that the oscillator strength and degree of polarization of the electronic transition strongly depend on the in-plane strains upon anisotropic in-plane strain relaxation. The research results provide important information for optimized growth of nonpolar III-nitrides. By using two-step growth and by fabricating the devices on the high-quality nonpolar free-standing GaN substrates, high-efficiency nonpolar a-plane InGaN LEDs can be realized. Nonpolar a-plane InGaN/GaN LEDs can exhibit a strongly polarized light to improve the contrast, glare, eye discomfort and eye strain, and efficiency in display application.

  1. Phytotoxic effects of leukamenin E (an ent-kaurene diterpenoid) on root growth and root hair development in Lactuca sativa L. seedlings.

    PubMed

    Ding, Lan; Qi, Linlin; Jing, Hongwei; Li, Juan; Wang, Wei; Wang, Tao

    2008-11-01

    Leukamenin E, an ent-kaurene diterpenoid isolated from Isodon racemosa (Hemsl) Hara, showed phytotoxic effects on root growth and root hair development of lettuce seedlings (Lactuca sativa L.). Lower concentrations (10 microM) of leukamenin E did not affect root growth, but at concentrations higher than 50 microM, the rate was inhibited. The influence of leukamenin E on root growth rate was closely correlated with alterations in the mitotic index. A low incidence of aberrant mitosis image was observed when lettuce roots were treated with higher concentrations (100 and 200 microM) of leukamenin E. This suggests that inhibition of root growth may be due to inhibition of cell division. All tested concentrations of the diterpenoid (10 microM or more) inhibited root hair development in a dose-dependent manner. At a concentration of 80 microM, leukamenin E completely blocked root hair initiation. Application of Ag(+)-an ethylene action inhibitor-to lettuce seedlings inhibited root hair elongation similar to the diterpenoid. Enhanced root hair length was stimulated by exogenous ethephon-an ethylene-releasing agent-and could be reversed by addition of leukamenin E. This suggests that leukamenin E may act as a potential ethylene action antagonist in the inhibition of lettuce root hair development. We conclude that leukamenin E may curb root hair development by interfering with ethylene action at concentrations above 10 microM and inhibits root growth via inhibition of cell division at concentrations above 50 microM.

  2. Stability of stagnation via an expanding accretion shock wave

    NASA Astrophysics Data System (ADS)

    Velikovich, A. L.; Murakami, M.; Taylor, B. D.; Giuliani, J. L.; Zalesak, S. T.; Iwamoto, Y.

    2016-05-01

    Stagnation of a cold plasma streaming to the center or axis of symmetry via an expanding accretion shock wave is ubiquitous in inertial confinement fusion (ICF) and high-energy-density plasma physics, the examples ranging from plasma flows in x-ray-generating Z pinches [Maron et al., Phys. Rev. Lett. 111, 035001 (2013)] to the experiments in support of the recently suggested concept of impact ignition in ICF [Azechi et al., Phys. Rev. Lett. 102, 235002 (2009); Murakami et al., Nucl. Fusion 54, 054007 (2014)]. Some experimental evidence indicates that stagnation via an expanding shock wave is stable, but its stability has never been studied theoretically. We present such analysis for the stagnation that does not involve a rarefaction wave behind the expanding shock front and is described by the classic ideal-gas Noh solution in spherical and cylindrical geometry. In either case, the stagnated flow has been demonstrated to be stable, initial perturbations exhibiting a power-law, oscillatory or monotonic, decay with time for all the eigenmodes. This conclusion has been supported by our simulations done both on a Cartesian grid and on a curvilinear grid in spherical coordinates. Dispersion equation determining the eigenvalues of the problem and explicit formulas for the eigenfunction profiles corresponding to these eigenvalues are presented, making it possible to use the theory for hydrocode verification in two and three dimensions.

  3. Heat Transfer Capability of (Ethylene Glycol + Water)-Based Nanofluids Containing Graphene Nanoplatelets: Design and Thermophysical Profile

    NASA Astrophysics Data System (ADS)

    Cabaleiro, D.; Colla, L.; Barison, S.; Lugo, L.; Fedele, L.; Bobbo, S.

    2017-01-01

    This research aims at studying the stability and thermophysical properties of nanofluids designed as dispersions of sulfonic acid-functionalized graphene nanoplatelets in an (ethylene glycol + water) mixture at (10:90)% mass ratio. Nanofluid preparation conditions were defined through a stability analysis based on zeta potential and dynamic light scattering (DLS) measurements. Thermal conductivity, dynamic viscosity, and density were experimentally measured in the temperature range from 283.15 to 343.15 K and nanoparticle mass concentrations of up to 0.50% by using a transient plate source, a rotational rheometer, and a vibrating-tube technique, respectively. Thermal conductivity enhancements reach up to 5% without a clear effect of temperature while rheological tests evidence a Newtonian behavior of the studied nanofluids. Different equations such as the Nan, Vogel-Fulcher-Tamman (VFT), or Maron-Pierce (MP) models were utilized to describe the temperature or nanoparticle concentration dependences of thermal conductivity and viscosity. Finally, different figures of merit based on the experimental values of thermophysical properties were also used to compare the heat transfer capability and pumping power between nanofluids and base fluid.

  4. His+ reversions caused in Salmonella typhimurium by different types of ionizing radiation

    SciTech Connect

    Roos, H.; Thomas, W.H.; Fitzek, M.; Kellerer, A.M.

    1988-11-01

    The yield of his+ reversions in the Ames Salmonella tester strain TA2638 has been determined for 60Co gamma rays, 140 kV X rays, 5.4 keV characteristic X rays, 2.2 MeV protons, 3.1 MeV alpha particles, and 18 MeV/U Fe ions. Inactivation studies were performed with the same radiations. For both mutation and inactivation, the maximum effectiveness per unit absorbed dose was obtained for the characteristic X rays, which have a dose averaged linear energy transfer (LET) of roughly 10 keV/micron. The ratio of the effectiveness of this radiation to gamma rays was 2 for inactivation and about 1.4 for the his+ reversion. For both end points the effectiveness decreases substantially at high LET, i.e., for the alpha particles and the Fe ions. The composition of the bottom and the top agar was the one recommended by Maron and Ames for application in chemical mutagenicity tests. The experiments with the less penetrating radiations differed from the usual protocol by utilization of a technique of plating the bacteria on the surface of the top agar. As in an earlier study greatly enhanced yields of mutations, relative to the spontaneous reversion rate, were obtained in these experiments by performing the irradiations 6 h after plating, which differs from the conventional procedure to irradiate the bacteria shortly after plating.

  5. Heat Transfer Capability of (Ethylene Glycol + Water)-Based Nanofluids Containing Graphene Nanoplatelets: Design and Thermophysical Profile.

    PubMed

    Cabaleiro, D; Colla, L; Barison, S; Lugo, L; Fedele, L; Bobbo, S

    2017-12-01

    This research aims at studying the stability and thermophysical properties of nanofluids designed as dispersions of sulfonic acid-functionalized graphene nanoplatelets in an (ethylene glycol + water) mixture at (10:90)% mass ratio. Nanofluid preparation conditions were defined through a stability analysis based on zeta potential and dynamic light scattering (DLS) measurements. Thermal conductivity, dynamic viscosity, and density were experimentally measured in the temperature range from 283.15 to 343.15 K and nanoparticle mass concentrations of up to 0.50% by using a transient plate source, a rotational rheometer, and a vibrating-tube technique, respectively. Thermal conductivity enhancements reach up to 5% without a clear effect of temperature while rheological tests evidence a Newtonian behavior of the studied nanofluids. Different equations such as the Nan, Vogel-Fulcher-Tamman (VFT), or Maron-Pierce (MP) models were utilized to describe the temperature or nanoparticle concentration dependences of thermal conductivity and viscosity. Finally, different figures of merit based on the experimental values of thermophysical properties were also used to compare the heat transfer capability and pumping power between nanofluids and base fluid.

  6. Rainfall threshold for triggering debris flow on Merapi volcano area, Yogyakarta, Indonesia

    NASA Astrophysics Data System (ADS)

    Kusumawardani, Rini; Kurniadhi, Rizki; Mukhlisin, Muhammad; Legono, Djoko

    2017-03-01

    Eruption of Merapi volcano on 2010 produced around 130 million cubic meters of deposit material consisting of ash, sand, gravel, and stone. Potential hazards of Merapi eruption caused a massive damages and destructions for both of during and after eruption. Phenomenon of deposit material sedimentation in upstream area of volcano causes debris flow occurrences induced by heavy rainfall. Ranfall intensity and its duration are important parameters which trigger the occurrence of debris flow. Another important parameters that effect of debris flow initiation are slope angle, surface water flow level, sediment concentration, density of soil, soil shear angle, grain size distribution of sediment deposit. This paper investigated the influence of rainfall triggering the debris occurrences located in Putih River, Magelang. The soil properties were collected from the river, while the rainfall data was obtained from three rain gauge stations (i.e., Station Maron, Mranggen and Ngepos). The results revealed the intensity maximum rainfall which was more than 40 mm/hour triggered the debris flow in Putih River Merapi. While, the critical basic slope (θ) and water depth (ho) were variables that greatly affect Takahashi Equation to predict the incidence of debris flow.

  7. Artificial tear adsorption on soft contact lenses: methods to test surfactant efficacy.

    PubMed

    Rebeix, V; Sommer, F; Marchin, B; Baude, D; Tran, M D

    2000-06-01

    Spoilage is a primary factor in the biocompatibility of soft contact lenses (SCL) within the lacrimal fluid. Tears are a complex mixture of proteins, lipids, natural surfactants and salts. The spoilation process is due to a contribution of all these components and of the nature of SCL materials themselves. The aim of this study was to set up methods to observe and quantify lacrimal deposits and to select efficient surfactants for preventing protein deposits. The present study was performed on PMMA-NVP SCL. The behaviour of SCL in presence of tears was studied by means of an in vitro artificial tear model consisting of the main tears components and quantified by a colorimetric technique (BCA) performed directly on the lenses. The nature of the deposit was observed directly by atomic force microscopy (AFM) in a liquid medium showing the same adsorption trend noticed in the quantitative results and identifying specific adsorption sites. The assessment of surfactant adsorption was performed using Maron's method, as a mean to evaluate the affinity of surfactant to the surface, while the action of selected surfactants on pre-treated SCL was assessed using the BCA method. Promising results were obtained with these two different methods which can be used easily for the pre-selection of surfactants for further cleaning solution formulation studies.

  8. Transovarial Effect of Novaluron on Tribolium castaneum (Coleoptera: Tenebrionidae) After Termination of Direct Contact.

    PubMed

    Trostanetsky, A; Kostyukovsky, M; Quinn, E

    2015-01-01

    The insect growth regulator novaluron (Rimon 10 EC, Makhteshim-Agan Ltd, Israel) is used against many field pests on corn, vegetables, orchards, forests, and cotton plantations. Previously, we studied various effects of novaluron on stored grain pests. Termination in Tribolium castaneum (Herbst) eggs hatching after treating adults with novaluron and following restoration after adult transfer to untreated media was observed. The objective of this study was to investigate the restoration of T. castaneum egg hatch following transfer of adults from treated media to untreated favorable and unfavorable media. The time needed for hatching restoration of 50% of eggs laid by adults transferred from novaluron (1 ppm) treated flour to untreated flour (RT50) was 2.7 d. RT50 for those transferred to untreated wheat grain was 4.1 d. RT90 in flour was 3.6 d, in grain--6.1 d. Varieties of RTs in grain and in flour with nonoverlapping confidence intervals indicate that RTs were significantly different. Delay of eggs hatching restoration for adults transferred from treated flour to unfavorable media (Petri dishes with limited amount of flour, lying of eggs not detected) was observed. RT50 in flour was 2.1 d and RT90--3.1 d, while RT50 in the unfavorable media was 3.4 d and RT90 6.5 d. Delayed effect of egg hatching restoration after adult transfer to unfavorable media provides evidence of the significant role of insect physiological state in novaluron excretion and (or) degradation by T. castaneum females.

  9. Scaling of micro-slip in tangentially loaded rock contact

    NASA Astrophysics Data System (ADS)

    Grzemba, Birthe; Pohrt, Roman; Teidelt, Elena; Popov, Valentin L.

    2014-05-01

    -slip preceding a global slip event in a stick-slip regime, including the maximum micro-slip. 1. Dieterich, James H. Time Dependent Friction and the Mechanics of Stick-Slip. 1978, Pure and Applied Geophysics, Vol. 116, pp. 790-806. 2. Scholz, C. H. The Critical Slip Distance for Seismic Faulting. 22/29, 1988, Nature, Vol. 336, pp. 761-763. 3. Ohnaka, M. A constitutive scaling law and a unified comprehension for frictional slip failure, shear fracture of intact rock, and earthquake rupture.B2, 2003, Journal of Geophysical Research: Solid Earth, Vol. 108, p. 2080. 4. Marone, C. and Kilgore, B. Scaling of critical slip distance for seismic faulting with shear strain in fault zones. 1993, Nature, Vol. 362, pp. 618-621. 5. Marone, C. and Cox, S.J.D. Scaling of Rock Friction Constitutive Parameters: The Effects of Surface Roughness and Cumulative Offset on Friction of Gabbro. 1994, Pure and Applied Geophysics, Vol. 143, pp. 359-385. 6. Pohrt, R. and Popov, V.L. Normal Contact Stiffness of Elastic Solids with Fractal Rough Surfaces. 2012, Physical Review Letters, Vol. 108, p. 104301. 7. Grzemba, B., et al. Maximum micro-slip in tangential contact of randomly rough self-affine surfaces. 2014, Wear, Vol. 309, pp. 256-258.

  10. Up-regulation of the mammalian target of rapamycin complex 1 subunit Raptor by aldosterone induces abnormal pulmonary artery smooth muscle cell survival patterns to promote pulmonary arterial hypertension.

    PubMed

    Aghamohammadzadeh, Reza; Zhang, Ying-Yi; Stephens, Thomas E; Arons, Elena; Zaman, Paula; Polach, Kevin J; Matar, Majed; Yung, Lai-Ming; Yu, Paul B; Bowman, Frederick P; Opotowsky, Alexander R; Waxman, Aaron B; Loscalzo, Joseph; Leopold, Jane A; Maron, Bradley A

    2016-07-01

    Activation of the mammalian target of rapamycin complex 1 (mTORC1) subunit Raptor induces cell growth and is a downstream target of Akt. Elevated levels of aldosterone activate Akt, and, in pulmonary arterial hypertension (PAH), correlate with pulmonary arteriole thickening, which suggests that mTORC1 regulation by aldosterone may mediate adverse pulmonary vascular remodeling. We hypothesized that aldosterone-Raptor signaling induces abnormal pulmonary artery smooth muscle cell (PASMC) survival patterns to promote PAH. Remodeled pulmonary arterioles from SU-5416/hypoxia-PAH rats and monocrotaline-PAH rats with hyperaldosteronism expressed increased levels of the Raptor target, p70S6K, which provided a basis for investigating aldosterone-Raptor signaling in human PASMCs. Aldosterone (10(-9) to 10(-7) M) increased Akt/mTOR/Raptor to activate p70S6K and increase proliferation, viability, and apoptosis resistance in PASMCs. In PASMCs transfected with Raptor-small interfering RNA or treated with spironolactone/eplerenone, aldosterone or pulmonary arterial plasma from patients with PAH failed to increase p70S6K activation or to induce cell survival in vitro Optimal inhibition of pulmonary arteriole Raptor was achieved by treatment with Staramine-monomethoxy polyethylene glycol that was formulated with Raptor-small interfering RNA plus spironolactone in vivo, which decreased arteriole muscularization and pulmonary hypertension in 2 experimental animal models of PAH in vivo Up-regulation of mTORC1 by aldosterone is a critical pathobiologic mechanism that controls PASMC survival to promote hypertrophic vascular remodeling and PAH.-Aghamohammadzadeh, R., Zhang, Y.-Y., Stephens, T. E., Arons, E., Zaman, P., Polach, K. J., Matar, M., Yung, L.-M., Yu, P. B., Bowman, F. P., Opotowsky, A. R., Waxman, A. B., Loscalzo, J., Leopold, J. A., Maron, B. A. Up-regulation of the mammalian target of rapamycin complex 1 subunit Raptor by aldosterone induces abnormal pulmonary artery smooth

  11. Anisotropic Shear-wave Velocity Structure of East Asian Upper Mantle from Waveform Tomography

    NASA Astrophysics Data System (ADS)

    Chong, J.; Yuan, H.; French, S. W.; Romanowicz, B. A.; Ni, S.

    2012-12-01

    East Asia is a seismically active region featuring active tectonic belts, such as the Himalaya collision zone, western Pacific subduction zones and the Tianshan- Baikal tectonic belt. In this study, we applied full waveform time domain tomography to image 3D isotropic, radially and azimuthally anisotropic upper mantle shear velocity structure of East Asia. High quality teleseismic waveforms were collected for both permanent and temporary stations in the target and its adjacent regions, providing good ray path coverage of the study region. Fundamental and overtone wave packets, filtered down to 60 sec, were inverted for isotropic and radially anisotropic shear wave structure using normal mode asymptotic coupling theory (NACT: Li and Romanowicz, 1995). Joint inversion of SKS measurements and seismic waveforms was then carried out following the methodology described in (Marone and Romanowicz, 2007). The 3D velocity model shows strong lateral heterogeneities in the target region, which correlate well with the surface geology in East Asia. Our model shows that Indian lithosphere has subducted beneath Tibet with a different northern reach from western to eastern Tibet,. We also find variations of the slab geometry in Western Pacific subduction zones. Old and stable regions, such as, Indian shield, Siberia platform, Tarim and Yangtze blocks are found to have higher shear wave velocity in the upper mantle. Lower velocity anomalies are found in regions like Baikal rift, Tienshan, Indochina block, and the regions along Japan island-Ryukyu Trench and Izu-bonin Trench. The dominant fast and slow velocity boundaries in the study region are well correlated with tectonic belts, such as the central Asian orogenic belt and Alty/Qilian-Qinling/Dabie orogenic belt. Our radially anisotropic model shows Vsh> Vsv in oceanic regions and at larger depths(>300km), and Vsv > Vsh in some orogenic zones.. We'll show preliminary results of azimuthally anisotropic joint inversion of SKS

  12. Shear Wave Splitting Beneath the New Madrid Seismic Zone and Adjacent Areas

    NASA Astrophysics Data System (ADS)

    Moidaki, M.; Liu, K. H.; Gao, S. S.; Hogan, J. P.; Abdelsalam, M. G.

    2007-12-01

    Teleseismic shear-wave splitting parameters are determined at 15 permanent and portable broadband stations within and around the New Madrid seismic zone (NMSZ) in order to map the direction and strength of mantle fabrics and to explore the origin of seismic anisotropy. Both the splitting times and fast polarization directions of the fast shear-wave show significant spatial variations. The observed splitting times range from 0.7 to 1.7s with a mean value of 1.0s which is the same as the global average. The resulting fast directions range from 34 to 118 degrees from north with a mean of 65 degrees which is consistent with the motion direction of the North American plate in a hot-spot frame. Fast directions with ray-piercing points in the NMSZ are oblique to the rift axis. In the vicinity of the Ozarks Plateau, the split times range from 0.7s to 1.1s with a mean of 0.9s. The observed fast directions show a striking clockwise rotating pattern in which these change systematically from nearly N-S in the St. Francois Mountains to approximately NE-SW further north to be concordant to that of North American Craton. The area with anomalous fast directions has recently been suggested to be a downward asthenospheric flow as a result of the sinking of the Farallon slab in the lower mantle (Forte et al 2007). The observed anisotropy will be discussed in relation to the lower mantle flow, and the recently-proposed two-layer model of Marone and Romanowicz (2007).

  13. Current Status of the Late Triassic and Early Jurassic APTS from Continental Sediments and Correlation with Standard Marine Stages

    NASA Astrophysics Data System (ADS)

    Kent, D. V.; Olsen, P. E.; Muttoni, G.

    2014-12-01

    A reproducible geomagnetic polarity template for the Late Triassic and earliest Jurassic continues to be that determined from ~5,000 meters of cored section in the Newark basin and ~2,500 meters of outcrop section in the Hartford basin, sampled at nominal ~20 kyr intervals according to a well-developed climate cyclicity that characterizes the lacustrine strata present in all but the fluviatile portions of the basins [Kent & Olsen, 1999, 2008 JGR]. The age model is based on the 405 kyr Milankovich climate cycle and pegging the sequence to high precision U-Pb dating of the Central Atlantic Magmatic Province (CAMP) at 201.6 to 200.9 Ma [Blackburn+2013 Science], the initiation of which is practically coincident with the end-Triassic extinction level (formerly set to 202 Ma) and within a climatic precession cycle after magnetochron E23r. The resulting astrochronostratigraphic polarity time scale (APTS) has 66 Poisson-distributed polarity intervals from chrons E8r (~225 Ma) to H27n (~199 Ma) with a constant sediment-accumulation rate extrapolation to chron E1r (~233 Ma). Magnetostratigraphic correlations from the most complete and usually the thickest Tethyan marine sections suggest that the Carnian/Norian boundary occurs within ~E7n [Channell+2003 PPP; Muttoni+2004 GSAB] at an APTS age of 227.5 Ma and for the Norian/Rhaetian boundary anywhere from E16n [Husing+2011 EPSL] at ~210.5 Ma to E20r [Maron+2014 Geology] at ~205.4 Ma depending on choice of conodont taxa, whereas the Hettangian/Sinemurian boundary can be placed at ~199.5 Ma within the marine equivalent of H25r [Husing+2014 EPSL]. These APTS ages are in substantive agreement with available high-precision dates in marine strata for the late Carnian [231 Ma: Furin+2006 Geology], latest Norian [205.5 Ma: Wotslaw+2014 Geology], and the boundaries of the Triassic/Jurassic [201.3 Ma: Guex+2012 PPP] and the Hettangian/Sinemurian [199.5 Ma: Schaltegger+2008 EPSL]. Carnian magnetostratigraphy needs to be improved but

  14. 2D Simulations of Earthquake Cycles at a Subduction Zone Based on a Rate and State Friction Law -Effects of Pore Fluid Pressure Changes-

    NASA Astrophysics Data System (ADS)

    Mitsui, Y.; Hirahara, K.

    2006-12-01

    There have been a lot of studies that simulate large earthquakes occurring quasi-periodically at a subduction zone, based on the laboratory-derived rate-and-state friction law [eg. Kato and Hirasawa (1997), Hirose and Hirahara (2002)]. All of them assume that pore fluid pressure in the fault zone is constant. However, in the fault zone, pore fluid pressure changes suddenly, due to coseismic pore dilatation [Marone (1990)] and thermal pressurization [Mase and Smith (1987)]. If pore fluid pressure drops and effective normal stress rises, fault slip is decelerated. Inversely, if pore fluid pressure rises and effective normal stress drops, fault slip is accelerated. The effect of pore fluid may cause slow slip events and low-frequency tremor [Kodaira et al. (2004), Shelly et al. (2006)]. For a simple spring model, how pore dilatation affects slip instability was investigated [Segall and Rice (1995), Sleep (1995)]. When the rate of the slip becomes high, pore dilatation occurs and pore pressure drops, and the rate of the slip is restrained. Then the inflow of pore fluid recovers the pore pressure. We execute 2D earthquake cycle simulations at a subduction zone, taking into account such changes of pore fluid pressure following Segall and Rice (1995), in addition to the numerical scheme in Kato and Hirasawa (1997). We do not adopt hydrostatic pore pressure but excess pore pressure for initial condition, because upflow of dehydrated water seems to exist at a subduction zone. In our model, pore fluid is confined to the fault damage zone and flows along the plate interface. The smaller the flow rate is, the later pore pressure recovers. Since effective normal stress keeps larger, the fault slip is decelerated and stress drop becomes smaller. Therefore the smaller flow rate along the fault zone leads to the shorter earthquake recurrence time. Thus, not only the frictional parameters and the subduction rate but also the fault zone permeability affects the recurrence time of

  15. Dry and Wet Friction of Plagioclase: Pure Cataclastic Flow(CF) vs. CF with Concurrent Pressure Solution

    NASA Astrophysics Data System (ADS)

    He, C.; Tan, W.

    2015-12-01

    To distinguish different deformation mechanisms at hydrothermal conditions, friction experiments of plagioclase under nominally dry conditions were compared with that at hydrothermal conditions documented in a previous study[He et al.,2013]. Preliminary result[Tan and He, 2008] shows that the rate dependence of plagioclase under confining pressure of 150MPa and nominally dry conditions is velocity strengthening at temperatures of 50-600oC, in contrast to the full velocity weakening at hydrothermal conditions. Here a) we conducted data fitting to the rate and state friction law to compare with the hydrothermal case; b) microstructural comparison was performed to understand the difference between the dry and wet conditions in the operative deformation mechanisms. The evolution effect (b value) under dry conditions exhibits much smaller values than that at wet conditions, and in contrast to the increasing trend at wet conditions, b values under dry conditions have a decreasing trend as temperature increases, from ~0.007 at 300oC down to 0 at 600oC. The direct effect (a value) at dry conditions has a peak of ~0.01 at 300oC and decreases to a level of 0.007-0.008 at higher temperatures, in contrast to the increasing trend seen at hydrothermal conditions. In the dry case, microstructure at temperatures of 300-600oC transitions gradually from a fabric characterized by localized Riedel shear zones to pervasive shear deformation, with the grain size reduced to a level of 1-3 micron in a submicron matrix in the latter case, corresponding to a lower porosity. The close association between porosity evolution and that of state variable revealed in previous studies[Morrow and Byerlee, 1989; Marone et al.,1990] suggests that the porosity change contributes largely to the evolution effect in addition to plasticity at intergranular contacts, probably due to gradual switching between different densities of packing. Our dry experiments indicate a cataclastic flow where the evolution

  16. Toward global waveform tomography of the whole mantle using SEM: Efficient simulation of the global wavefield using a homogenized crust

    NASA Astrophysics Data System (ADS)

    French, S. W.; Lekic, V.; Romanowicz, B. A.

    2010-12-01

    initially employ the hybrid scheme used in developing SEMum: highly accurate wavefield calculations using SEM, combined with sensitivity kernels from Nonlinear Asymptotic Coupling Theory (NACT: Li and Romanowicz, 1995). This approach balances computational cost of an “exact” measurement of waveform misfit with an approximate, though nonlinear, treatment of structural sensitivity appropriate for long-period body waves. Implementation of the homogenized crust follows easily for SEM, though multiple options exist in NACT, including the regionalized nonlinear treatment of Marone and Romanowicz (2007) and the efficient modified linear scheme of Lekic et al. (2010). Both are discussed in the context of structural variation in our crustal model.

  17. Re-examination of the postseismic deformation following the 2000 Western Tottori Earthquake, Southwest Japan

    NASA Astrophysics Data System (ADS)

    Hashimoto, M.; Takeo, I.

    2002-12-01

    Previously, we presented the results of the dual frequency observations following the Western Tottori earthquake of Oct. 6, 2000 and interpretations in terms of afterslip on the source fault. In this study, we report the results of a re-examination of the above data using a logarithmic decay function based on the rate-state dependent friction law. The 2000 Western Tottori earthquake is a typical inland earthquake in Japan with left-lateral strike-slip faulting on a NNW-SSE trending vertical fault plane. The Japanese University Consortium for GPS Research (JUNCO) studied the postseismic deformation immediately after the mainshock with a dense GPS network surrounding the source region. Most observations were carried out continuously until the end of October 2000, and some sites equipped with dual frequency receivers were reoccupied in March 2001. JUNCO observed a slowly decaying movement at every site. The spatial pattern shows left lateral motion across the source fault, similar to the coseismic displacements. We derived the amount of afterslip on a shallow part of the source fault from this spatial pattern. We fit exponentially decaying functions to the data from the sites occupied in March 2001 and obtained time constants of 20 to 40 days. However, this may be inconsistent with the idea of afterslip on the source fault or its extension, since an exponential decay function is closely related to the relaxation of stress in a viscoelasitc layer. Here we fit the temporal variation with the following logarithmic decay function proposed by Marone et al. (1991). Up(t) = αln\\{(β/α) t+1\\} + V0 t + Uref, where Up(t) is the displacement, t is time in days, α is the fault constitutive parameter in the velocity-strengthening layer, β is the coseismic velocity, V0 is the steady state velocity and Uref is the offset at the start of observation. In this nonlinear fitting, we assume a non-negative constraint on V0. We obtained positive α at 6 of 12 sites. The estimated

  18. Postseismic Deformations Following the 2000 Western Tottori Earthquake Detected by Dense GPS Observations

    NASA Astrophysics Data System (ADS)

    Tabei, T.; Ooba, K.; Hashimoto, M.; Ito, T.; Hoso, Y.

    2001-12-01

    The Japanese University Consortium for GPS Research (JUNCO) carried out observations of postseismic deformation immediately following the Western Tottori earthquake of October 6, 2000, with a dense GPS network surrounding the source region. This earthquake is a typical inland earthquake in Japan with a left-lateral strike-slip faulting on a NNW-SSE trending vertical fault plane. 16 dual frequency receivers (Ashtech Z12 and Z-Surveyor) and 11 single frequency receivers (Furuno MG-11, 21) were deployed in an area approximately 20km in the EW direction by 30km in the NS direction. Phase data were sampled every 30 seconds and the elevation mask was 15 degree. Most observations were done continuously until the end of October 2000, and some sites occupied with dual frequency receiver were reoccupied in March 2001. Daily solutions of each station were determined using Bernese 4.2, with reference to IGS sites and nearby GEONET sites. We present the results of the dual frequency observations and an interpretation in terms of afterslip on the source fault. We observed decaying motions at many sites, despite large fluctuations mainly due to meteorological disturbances. Some sites in the northwestern part of the network show step-like movements around Oct. 18. This movement might be related to a conjugate distribution of aftershocks recognized in this area. If we fit exponentially decaying functions to the data from the sites occupied in March 2001, we obtain time constants of 20 to 40 days. Unfortunately fitting with the logarithmic decaying function proposed by Marone et al. (1991) was so far unsuccessful, probably because of the lack of data between October 2000 and March 2001. The spatial pattern of displacements shows left lateral motion across the source fault, which is concordant with the mechanism of the mainshock. Stations on the NE side of the fault moved northwestward, and stations on the SW side moved southeastward. The largest displacement amounts to 2cm for half

  19. Transition from velocity weakening to strong velocity strengthening friction in dense granular shear experiments

    NASA Astrophysics Data System (ADS)

    Kuwano, O.; Ando, R.; Hatano, T.

    2009-12-01

    regime (larger than 100um per decade of sliding velocity) and this velocity dependence of dilatation is lager than that of usual rate- and state- dependent friction (Marone et al 1990, Beeler and Tullis 1997).

  20. “Radiational tides” as nonlinear effects: bispectral interpretation

    NASA Astrophysics Data System (ADS)

    Marone, Eduardo

    1996-07-01

    In this work it is shown that “radiational tides” could be interpreted as nonlinear effects by using the results of nonlinear tidal analysis. A one-year record (1979) of hourly sea level data from Ingeniero White, Argentina (38°47‧S, 62°16‧W) was analysed using spectral and bispectral methodologies (Marone and Mesquita, I994), in order to separate linear from nonlinear effects. The results show the same pattern observed when 1980s hourly data were analysed in the cited work. The concept of “radiational tides” was introduced to explain the extra terms used to fit the astronomical tidal potential onto real tidal records (Munk and Cartwright, 1966). Originally, it had a mathematical reasoning based on a physical hypothesis. Later it was proposed that “radiational tides” are a nonlinear effect due to the linkage of linear tidal constituents (Godin, 1986). The original physical interpretation based upon local solar radiational inputs was unsuitable, because one can find “radiational tides” being more important in high latitudes than in tropical or subtropical regions. The current hypothesis in this way relates the “radiational tide” with some global or meso-scale radiational effects of the sun. Anyway, this explanation seems to be incomplete, because the different values of theS2 constituents for narrow ports show that local effects are important. Godin (1986) suggested that nonlinear second order interactions are the most reasonable explanation for the unexpected large values of some tidal constituents, especially in the semidiurnal band. Using the bispectral analysis of sea-level records it was possible to show that a remarkable nonlinear interaction exists besides the diurnal band and that energy is transferred to the semidiurnal band. This fact justifies the interpretation of “radiational tides” as mainly a quadratic frictional linkage between the diurnal constituents. The results suggest that the term “radiational tides” must be

  1. Dynamic simulation of wavy-stratified two-phase flow with the one-dimensional two-fluid model

    NASA Astrophysics Data System (ADS)

    Fullmer, William D.

    conditions. This appears to result in non-convergence when particular solutions at a specific time are compared using different numerical discretizations. However, it is shown that the chaotic solutions exhibit an invariant spectrum in wavenumber space that can be used to assess the convergence of solutions. This concept is applied to a Kelvin-Helmholtz experiment of kerosene and liquid water in a tilted channel whereby many slightly different simulations are run and averaged to determine the mean behavior. Comparisons to experimental data are favorable; especially considering the limitations of applying a one-dimensional model to a dynamic simulation of wavy channel flow. When the analysis is extended to consider air-water flows, several additional challenges are encountered related to the long-wavelength inviscid Kelvin-Helmholtz instability, which is the instability inherent to the one-dimensional two-fluid model. The transition from stratified to wavy flow is significantly over-predicted, i.e., requires a larger velocity to become unstable than observed experimentally. The wave sheltering model of Brauner and Maron (1993) is included in the interfacial shear model and calibrated for flow in a rectangular channel. However, when the unstable flow regime is simulated a wavy flow pattern does not develop as in the liquid-liquid case. Due to the near absence of inertia in the lighter gas phase, viscosity and surface tension are unable to bound the growth of disturbances within the physical limitations of the channel geometry. Transitions to regions of single phase flow result, indicating a slug flow pattern where wavy flow should exist. A novel approach is taken where the instability mechanism, here the sheltering force, is adjusted based on local geometric conditions, namely the void fraction gradient. Comparison to data shows promising results, although a large degree of uncertainty in such an approach remains due to a lack of local experimental data.

  2. An infrastructure for the integration of geoscience instruments and sensors on the Grid

    NASA Astrophysics Data System (ADS)

    Pugliese, R.; Prica, M.; Kourousias, G.; Del Linz, A.; Curri, A.

    2009-04-01

    ). In this paper i) we define the need for integration of instrumentation in the Grid, ii) we introduce the solution of the Instrument Element, iii) we demonstrate a suitable end-user web portal for accessing Grid resources, iv) we describe from the Grid-technological point of view the process of the integration to the Grid of two advanced environmental monitoring devices. References [1] M. Surridge, S. Taylor, D. De Roure, and E. Zaluska, "Experiences with GRIA—Industrial Applications on a Web Services Grid," e-Science and Grid Computing, First International Conference on e-Science and Grid Computing, 2005, pp. 98-105. [2] A. Chervenak, I. Foster, C. Kesselman, C. Salisbury, and S. Tuecke, "The data grid: Towards an architecture for the distributed management and analysis of large scientific datasets," Journal of Network and Computer Applications, vol. 23, 2000, pp. 187-200. [3] B. Allcock, J. Bester, J. Bresnahan, A.L. Chervenak, I. Foster, C. Kesselman, S. Meder, V. Nefedova, D. Quesnel, and S. Tuecke, "Data management and transfer in high-performance computational grid environments," Parallel Computing, vol. 28, 2002, pp. 749-771. [4] E. Frizziero, M. Gulmini, F. Lelli, G. Maron, A. Oh, S. Orlando, A. Petrucci, S. Squizzato, and S. Traldi, "Instrument Element: A New Grid component that Enables the Control of Remote Instrumentation," Proceedings of the Sixth IEEE International Symposium on Cluster Computing and the Grid (CCGRID'06)-Volume 00, IEEE Computer Society Washington, DC, USA, 2006. [5] R. Ranon, L. De Marco, A. Senerchia, S. Gabrielli, L. Chittaro, R. Pugliese, L. Del Cano, F. Asnicar, and M. Prica, "A Web-based Tool for Collaborative Access to Scientific Instruments in Cyberinfrastructures." 1 The DORII project is supported by the European Commission within the 7th Framework Programme (FP7/2007-2013) under grant agreement no. RI-213110. URL: http://www.dorii.eu 2 Istituto Nazionale di Oceanografia e di Geofisica Sperimentale. URL: http://www.ogs.trieste.it

  3. Bulk-friction modeling of afterslip and the modified Omori law

    USGS Publications Warehouse

    Wennerberg, Leif; Sharp, Robert V.

    1997-01-01

    Afterslip data from the Superstition Hills fault in southern California, a creep event on the same fault, the modified Omori law, and cumulative moments from aftershocks of the 1957 Aleutian Islands earthquake all indicate that the original formulation by Dieterich (1981) [Constitutive properties of faults with simulated gouge. AGU, Geophys. Monogr. 24, 103–120] for friction evolution is more appropriate for systems far from instability than the commonly used approximation developed by Ruina (1983) [Slip instability and state variable friction laws. J. Geophys. Res. 88, 10359–10370] to study instability. The mathematical framework we use to test the friction models is a one-dimensional, massless spring-slider under the simplifying assumption, proposed by Scholz (1990) [The Mechanics of Earthquakes and Faulting. Cambridge University Press] and used by Marone et al. (1991) [On the mechanics of earthquake afterslip. J. Geophys. Res., 96: 8441–8452], that the state variable takes on its velocity-dependent steady-state value throughout motion in response to a step in stress. This assumption removes explicit state-variable dependence from the model, obviating the need to consider state-variable evolution equations. Anti-derivatives of the modified Omori law fit our data very well and are very good approximate solutions to our model equations. A plausible friction model with Omori-law solutions used by Wesson (1988) [Dynamics of fault creep. J. Geophys. Res. 93, 8929–8951] to model fault creep and generalized by Rice (1983) [Constitutive relations for fault slip and earthquake instabilities. Pure Appl. Geophys. 121, 443–475] to a rate-and-state variable friction model yields exactly Omori's law with exponents greater than 1, but yields unstable solutions for Omori exponents less than 1. We estimate from the Dieterich formulation the dimensionless parameter a∗ which is equal to the product of the nominal coefficient of friction and the more commonly reported

  4. Along strike applicability of results from the Deep Fault Drilling Project, Alpine Fault, New Zealand

    NASA Astrophysics Data System (ADS)

    Boulton, C. J.; Toy, V. G.; Barth, N. C.; Carpenter, B. M.

    2012-12-01

    similar brown PSZ gouges also occur at localities north and south of Gaunt Creek, from Little Man River to Robinson Creek, an along strike distance of 120 km. Everywhere mapped, brown PSZ gouges form at the contact between Pacific Plate and Australian Plate-derived cataclasites, which, importantly, do not contain smectite. Smectite-bearing gouges are generally absent on shallow dipping dextral-reverse faults at the toes of large thrust sheets, where plate boundary cataclasites overlie Late Quaternary gravels in sharp contact. Our results suggest that PSZ gouges retrieved in the DFDP-1 cores are commonly present on moderately dipping (average orientation 043°/30°SE; Norris and Cooper, 2007) dextral-reverse faults along the central Alpine Fault, and we discuss modes of PSZ formation. References Boulton, C., B.M. Carpenter, V. Toy, and C. Marone (2012). Physical properties of surface outcrop cataclastic fault rocks, Alpine Fault, New Zealand. Geochem. Geophys. Geosyst., 13, doi:10.1029/2011GC003872. Norris, R.J., and A.F. Cooper (2007). The Alpine Fault, New Zealand: Surface Geology and Field Relationships, in A Continental Plate Boundary: Tectonics at South Island, New Zealand, edited by Okaya, D., Stern, T., and F. Davey, American Geophysical Union Monograph Vol 175, Washington, D.C., 159-178.

  5. Stress-weakening effect on friction and a major revision of evolution law for contact state

    NASA Astrophysics Data System (ADS)

    Nagata, K.; Nakatani, M.; Yoshida, S.

    2009-12-01

    Rate and State Friction (RSF) law comprehensively captures important aspects of rock friction and has explained various aspects of fault motion successfully. However, existing RSF laws are clearly incorrect in describing some aspects of friction firmly established by experiments [Beeler et al., 1994]. The shortfall is that the state evolution law which aptly represents time-dependent strengthening of virtually locked faults systematically mispredicts the slip distance required to complete the state evolution caused by changed slip velocity [Marone, 1998; Nakatani, 2001]. To address the problem of evolution law, we observed state variable in RSF continuously in friction experiments on rough granite surfaces. The observation of state variable was performed in the following two independent ways; 1) by subtracting direct effect from measured shear stress 2) by using an acoustic monitoring technique [Nagata et al., 2008]. The latter method is usable even when slip velocity is so low that the former method cannot be used. The former can be regarded as “semi-direct” measurements of state variable. This method strongly depends on the value of coefficient of direct effect a. Ideally, a is observed as the instantaneous change of applied shear stress (direct effect) upon velocity step. However, the measured shear stress change is much smaller than the real direct effect in reality because the state variable changes considerably before the stress peak. Correction by inferring the change of state using an evolution law is a routine procedure, but the evolution law is in doubt. Hence, before we tackled the evolution law issue, we have designed a special step test where the change of state is minimal and have established that a >0.03. Further, with help of acoustic method, we have identified that a ~0.05. The value is surprisingly large, but agrees very well with the activation volume of silicate lattice. We compared thus observed variation of frictional strength with the

  6. This Experiment Cried Out for a Different Interpretation

    NASA Astrophysics Data System (ADS)

    McSaveney, M. J.; Wang, G.

    2011-12-01

    and fragments of crystal-fragment agglomerates. In section perpendicular to Y-shear surfaces and parallel to shear direction, the cataclastic zone appeared to be a repeating series of R2 Riedel shears between repeating discontinuous Y-shears. Given the deformation required to open R2-shears, it was apparent that Y-shears would be ephemeral under conditions for continuing R2-shear generation. We did not measure the squeal pitch, but felt aural discomfort before any sound was heard. Our experiment cried out to us that weakening can come from microseismic (acoustic) lubrication of the Y-shear interface, from the vibration that resonates to make DPRI-6 squeal. Niemeijer, A; Marone, C; Elsworth, D. 2010. Frictional strength and strain weakening in simulated fault gouge: competition between geometrical weakening and chemical strengthening. J. Geophys. Res. 115, B10207, doi:10.1029/2009JB000838, 2010 Sassa, K.; Fukuoka, H.; Wang, G; Ishikawa, N. 2004. Undrained dynamic-loading ring-shear apparatus and its application to landslide dynamics. Landslides 1: 7-19.

  7. Improvement of barrier properties of poly(ethylene terephthalate)/organoclay nanocomposites

    NASA Astrophysics Data System (ADS)

    Dini, Maryam

    ( 1H NMR and 13C NMR) spectra showed the linear molecular structure of PET. The effect of organoclay concentration on the rheological, thermal, mechanical and barrier properties of the PET nanocomposites prepared by different methods was studied in the second part of this work. XRD, SEM and TEM analyses displayed intercalated/exfoliated morphology in all PET/C30B nanocomposites, with a higher degree of intercalation and delamination for the water-assisted process. Enhanced mechanical and barrier properties were obtained in PET-C30B nanocomposites compared to the neat PET. The nanocomposites exhibited higher tensile modulus and lower oxygen permeability after SSP. Elongation at break was significantly higher for SSP nanocomposites than for nanocomposites processed by conventional melt mixing. Elongation at break for conventional PET nanocomposites containing 2 wt% C30B was 6%, but for nanocomposites after SSP, the elongation at break was around 145%. Compared to the neat PET, improvements of 45% in tensile modulus and 42% in barrier behavior were found for nanocomposites containing 6 wt% C30B. The pseudo-inclusion model was used to predict the tensile modulus of PET nanocomposites and to determine the effect of intercalation microstructure on the model predictions. Moreover, the Nielsen and Bharadwaj models were employed for the prediction of permeability in the presence of organoclay. Studies of solid-state polymerization of PET and PET nanocomposites with different concentrations of Cloisite 30B and particle size were carried out at different reaction times in the third part of this work. Moreover, the effect of particle size on the rate of SSP was also investigated. Viscometry, titration, rheological and dynamic scanning calorimetry (DSC) measurements were used to analyze the samples from SSP. The weight-averaged molecular weight (MW) of PET was shown to increase significantly following SSP. The Maron-Pierce model was utilized to evaluate the molecular weight of PET