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  • Superfluidity and superconductivity  (9)
  • Polymer and Materials Science  (6)
  • Drosophila melanogaster  (3)
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  • 1
    Electronic Resource
    Electronic Resource
    Springer
    Molecular genetics and genomics 224 (1990), S. 303-308 
    ISSN: 1617-4623
    Keywords: Transposable elements ; Genetic instability ; Drosophila melanogaster ; gypsy (mdg4)
    Source: Springer Online Journal Archives 1860-2000
    Topics: Biology
    Notes: Summary The laboratory imitator strain (MS) of Drosophila melanogaster is characterized by an elevated frequency of spontaneous mutation (10−3–10−4). Mutations occur in both sexes at premeiotic stages of germ cell development. The increased mutability is a characteristic feature of MS itself, since it appears in the absence of outcrossing. Most of the mutations arising in this strain are unstable: reversions to wild type, high frequency mutation to new mutant states and replicating instability were observed. We have investigated the localization of the transposable genetic elements mdg1, 412, mdg3, gypsy (mdg4), copia and P in the X chromosomes of the MS and in the mutant lines y, ct, sbt derived from it by in situ hybridization. The P element was not found in any of these strains. The distributions of mdg1, 412, mdg3 and copia were identical in the X chromosomes of the MS and its derivatives. However, the sites of hybridization with gypsy differ in the various lines tested. In the polytene chromosomes of MS animals significant variation in location and number of copies of the gypsy element was demonstrated between different larvae; copy numbers as high as 30–40 were observed. These results suggest autonomous transposition of gypsy in the MS genome while several other mobile elements remain stable.
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  • 2
    ISSN: 1617-4623
    Keywords: Drosophila melanogaster ; Transposition ; Genetic instability ; gypsy (mdg4) ; hobo
    Source: Springer Online Journal Archives 1860-2000
    Topics: Biology
    Notes: Summary Using the in situ hybridization technique, we have analysed the distribution of mobile elements in the X chromosomes of male offspring of individual mutator strain (MS) males crossed to attached-X females. The experiments demonstrate varying cytological localization of the mobile elements gypsy (mdg4) and hobo among different individuals. The other mobile elements investigated (mdgl, mdg3, 412, 297, copia, 17.6, Doc, H.M.S. Beagle, Springer, FB) display no changes in insertion sites. Such an experiment is equivalent to analysis of separate gametes of an MS individual. Thus, the ability of gypsy and hobo to transpose in germ-line cells is demonstrated directly. Transpositions occur at premeiotic stages of germ cell development, since they appear in clusters. Analysis of gypsy and hobo transposition events shows that they occur independently. The same experiment demonstrates that gypsy localization varies significantly between different salivary gland cells of an MS individual. Two types of gypsy hybridization sites can be distinguished: “permanent” sites, common to all cells, and “additional” ones varying between neighbouring salivary gland cells. These additional sites indicate gypsy transposition in somatic cells of the MS. Transposition of the hobo element in somatic cells has also been observed.
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  • 3
    Electronic Resource
    Electronic Resource
    Springer
    Genetica 85 (1991), S. 13-22 
    ISSN: 1573-6857
    Keywords: Drosophila melanogaster ; genetic instability ; gypsy ; mobile elements ; retrotransposons
    Source: Springer Online Journal Archives 1860-2000
    Topics: Biology
    Notes: Abstract The laboratory mutator strain (MS) has properties which can be characterized as genetic instability. It exhibits the high level of gypsy autonomous transposition in somatic and germ cells. This paper summarizes all the data concerning this system and gypsy itself that has been obtained in our works during the last years.
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  • 4
    Electronic Resource
    Electronic Resource
    New York : Wiley-Blackwell
    Biopolymers 28 (1989), S. 975-993 
    ISSN: 0006-3525
    Keywords: Chemistry ; Polymer and Materials Science
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology
    Notes: Electrostatic potentials around DNA are obtained by solving the nonlinear Poisson-Boltzmann (PB) equation. The detailed charge distribution of the DNA and the different polarizabilities of the macromolecule and solvent are included explicitly in the calculations. The PB equation is solved using extensions of a finite difference approach applied previously to proteins. Electrical potentials and ion concentrations are compared to those obtained with simpler models. It is found that the shape of the dielectric boundary between the macromolecule and solvent has significant effects on the calculated potentials near the surface, particularly in the grooves. Sequence-specific patterns are found, the most surprising result being the existence of positive regions of potential near the bases in both the major and minor grooves. The effect of solvent and ionic atmosphere screening of phosphate-phosphate repulsions is studied, and an effective dielectric function, appropriate for molecular mechanics simulations, is derived.
    Additional Material: 5 Ill.
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  • 5
    Electronic Resource
    Electronic Resource
    New York : Wiley-Blackwell
    Biopolymers 36 (1995), S. 227-243 
    ISSN: 0006-3525
    Keywords: Chemistry ; Polymer and Materials Science
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology
    Notes: Using the nonlinear Poisson-Boltzmann (PB) equation, expressions for the nonspecific salt dependence of the free energy, and the entropic and enthalpic contributions to the electrostatic free energy of a polyelectrolyte are derived. The results are generalized for any number and valence of mobile ions, and now permit a more rigorous treatment of the salt dependence of polyelectrolyte-ligand binding using the PB equation. The salt dependence of the electrostatic free energy depends on an “osmotic pressure like” term identified previously [K. Sharp and B. Honig (1990), Journal of Physical Chemistry, Vol. 94, pp. 7684-7692], which in turn depends on the integrated excess/deficit of all mobile ion species around the polyelectrolyte. For the simple salt case (two ions only) this expression is equivalent to that derived previously [H. Eisenberg (1976), Biological Macromolecules and Polyelectrolytes in Solution, Clarendon. Oxford] in terms of Donnan, or preferential interaction coefficients. Moreover, since all ions enter into the PB expression for the salt dependence of the free energy in an identical way, it is equally applicable to polyelectrolytes with charge of one sign (e.g., nucleic acids), with oppositely charged groups (such as proteins), and even polyelectrolytes that have no net charge, for which the Donnan coefficient is ill-defined. The distribution of counterions around three simple polyelectrolyte geometries - spherical, cylindrical, and planar - was examined. In each case the excess number of counterions associated with the polyelectrolyte is not constant, but increases with decreasing salt. Although a limiting value is reached at low salt for a cylinder, in agreement with the limiting law condensation models, for the spherical geometry the number of associated counterions decreases to zero, while for the planar case it increases to 100%. For the cylindrical case Donnan coefficients agree closely with those computed previously by Monte Carlo simulations [M. C. Olmstead, C. F. Anderson, and M. T. Record (1991) Biopolymers, Vol. 31, pp. 1593-1604]. An all atom B-DNA model shows about 5% less accumulation of counterions than a cylinder, due to the helical charge arrangement and groove structure. The entropic and enthalpic contributions to the salt-dependent free energy of a cylinder were examined in the PB model. In addition to the well known ion cratic (redistribution) entropy, there are significant contributions from electrostatic enthalpy, and from dielectric entropy (water re-orientation due to the electrostatic field from polyelectrolyte charges and salt ions). The latter entropy contribution has not previously been taken into account in salt-dependent polyelectrolyte phenomena, but at higher salt concentrations (〉 0.01M), this can be as large as the cratic entropy contribution. © 1995 John Wiley & Sons, Inc.
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  • 6
    ISSN: 0006-3525
    Keywords: Chemistry ; Polymer and Materials Science
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology
    Notes: The theory for the salt dependence of the free energy, entropy, and enthalpy of a polyelectrolyte in the PB (PB) model is extended to treat the nonspecific salt dependence of polyelectrolyte-ligand binding reactions. The salt dependence of the binding constant (K) is given by the difference in osmotic pressure terms between the react ants and the products. For simple 1-1 salts it is shown that this treatment is equivalent to the general preferential interaction model for the salt dependence of binding [C. Anderson and M. Record (1993) Journal of Physical Chemistry, Vol. 97, pp. 7116-7126]. The salt dependence, entropy, and enthalpy are compared for the PB model and one specific form of the preferential interaction coefficient model that uses counterion condensation/limiting law (LL) behavior. The PB and LL models are applied to three ligand-polyelectrolyte systems with the same net ligand charge: a model sphere-cylinder binding reaction, a drug-DNA binding reaction, and a protein-DNA binding reaction. For the small ligands both the PB and limiting law models give (ln K vs. In [salt]) slopes close in magnitude to the net ligand charge. However, the enthalpy/entropy breakdown of the salt dependence is quite different. In the PB model there are considerable contributions from electrostatic enthalpy and dielectric (water reorientation) entropy, compared to the predominant ion cratic (release) entropy in the limiting law model. The relative contributions of these three terms in the PB model depends on the ligand: for the protein, ion release entropy is the smallest contribution to the salt dependence of binding. The effect of three approximations made in the LL model is examined: These approximations are (1) the ligand behaves ideally, (2) the preferential interaction coefficient of the polyelectrolyte is unchanged upon ligand binding, and (3) the polyelectrolyte preferential interaction coefficient is given by the limiting law/counterion-condensation value. Analysis of the PB model shows that assumptions 2 and 3 break down at finite salt concentrations. For the small ligands the effects on the slope cancel, however, giving net slopes that are similar in the PB and LL models, but with a different entropy/enthalpy breakdown. For the protein ligand the errors from assumptions 2 and 3 in the LL model do not cancel. In addition, the ligand no longer behaves ideally due to its complex structure and charge distribution. Thus for the protein the slope is no longer related simply to the net ligand charge, and the PB model gives a much larger slope than the LL model. Additionally, in the PB model most of the salt dependence of the protein binding comes from the change in ligand activity, i.e. from nonspecific anion effects, in contrast to the small ligand case. While the absolute binding is sensitive to polyelectrolyte length, little length effect is seen on the salt dependence for the small ligands at 0.1M salt, and for lengths 〉 60 Å. Almost no DNA length dependenceis seen in the salt dependence of the protein binding, since this is determined primarily by the protein, not the DNA. © 1995 John Wiley & Sons, Inc.
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  • 7
    Electronic Resource
    Electronic Resource
    New York, NY [u.a.] : Wiley-Blackwell
    Journal of Applied Polymer Science 49 (1993), S. 885-892 
    ISSN: 0021-8995
    Keywords: Chemistry ; Polymer and Materials Science
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology , Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics , Physics
    Notes: The process-zone evolution strongly influences the crack growth of polycarbonate. A methodology for determination of the kinetics of the process-zone evolution by decoupling these two processes was developed. This was achieved using constant displacement (stress-re-laxation) conditions under which the crack length remained constant. The morphology of the process zone was characterized using optical microscopy of cross sections and fracture surfaces produced with liquid nitrogen. The kinetics of process-zone evolution and stress relaxation were monitored and analyzed. The kinetics vary significantly with the level of displacement imposed. Thus, the challenge remains to construct a master curve for the kinetics. © 1993 John Wiley & Sons, Inc.
    Additional Material: 11 Ill.
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  • 8
    Electronic Resource
    Electronic Resource
    New York, NY [u.a.] : Wiley-Blackwell
    Journal of Applied Polymer Science 49 (1993), S. 877-883 
    ISSN: 0021-8995
    Keywords: Chemistry ; Polymer and Materials Science
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology , Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics , Physics
    Notes: A thermodynamic model for the equilibrial process zone ahead of a crack in polycarbonate is developed from the recently proposed Chudnovsky model and experimental characterization of the process zone. Based on the model, the force for evolution of the process zone is proposed from the consideration of irreversible thermodynamics and chemical reaction theories. The experimental data reported in our previous paper are well described by the equilibrial process zone model and a new kinetic equation. © 1993 John Wiley & Sons, Inc.
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  • 9
    Electronic Resource
    Electronic Resource
    New York, NY [u.a.] : Wiley-Blackwell
    Journal of Applied Polymer Science 51 (1994), S. 1841-1848 
    ISSN: 0021-8995
    Keywords: Chemistry ; Polymer and Materials Science
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology , Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics , Physics
    Notes: The fracture toughness of polycarbonate specimens of 3-9 mm thickness obtained from an actual aircraft canopy, were studied under accelerated weathering conditions and different rates of loading. Although no significant effects of thickness and loading rate on the critical stress intensity factors were observed, two different failure modes, brittle fracture and ductile fracture triggered by “pop-in,” were observed. The mode of failure was a random event and the probability of ductile failure associated with pop-in increases with the weathering time. More insight to material characteristics are gained through analysis of the specific fracture energy (SFE). The average values of SFE decrease monotonically with accelerated weathering time. This effect is ascribed to physical aging of the PC in the weatherometer that was corroborated through increases in density. The values of SFE seem to correlate with the probability for ductile fracture. This information can be used to establish conservative critical stress values for design. © 1994 John Wiley & Sons, Inc.
    Additional Material: 10 Ill.
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  • 10
    Publication Date: 2012-04-10
    Description: Author(s): E. C. Blomberg, A. Kreyssig, M. A. Tanatar, R. M. Fernandes, M. G. Kim, A. Thaler, J. Schmalian, S. L. Bud'ko, P. C. Canfield, A. I. Goldman, and R. Prozorov The effect of uniaxial tensile stress and the resultant strain on the structural/magnetic transition in the parent compound of the iron arsenide superconductor BaFe 2 As 2 is characterized by temperature-dependent electrical resistivity, x-ray diffraction, and quantitative polarized light imaging. We s... [Phys. Rev. B 85, 144509] Published Mon Apr 09, 2012
    Keywords: Superfluidity and superconductivity
    Print ISSN: 1098-0121
    Electronic ISSN: 1095-3795
    Topics: Physics
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