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  • 1
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    Journal of the American Chemical Society 74 (1952), S. 1977-1979 
    ISSN: 1520-5126
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    Chemical reviews 39 (1939), S. 79-135 
    ISSN: 1520-6890
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    Oxford, UK : Blackwell Publishing Ltd
    Annals of the New York Academy of Sciences 540 (1988), S. 0 
    ISSN: 1749-6632
    Source: Blackwell Publishing Journal Backfiles 1879-2005
    Topics: Natural Sciences in General
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    Journal of the American Chemical Society 57 (1935), S. 2347-2351 
    ISSN: 1520-5126
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    [s.l.] : Nature Publishing Group
    Nature 191 (1961), S. 1160-1161 
    ISSN: 1476-4687
    Source: Nature Archives 1869 - 2009
    Topics: Biology , Chemistry and Pharmacology , Medicine , Natural Sciences in General , Physics
    Notes: [Auszug] IN a recent paper1 we directed attention to the fact that values of both intrinsic viscosity [YJ] and the viscosity slope constant Jc', obtained in the usual way, may be significantly in error because of an apparent reduction in capillary radius. As Ohm2 has demonstrated, this apparent reduction in ...
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    [s.l.] : Nature Publishing Group
    Nature 196 (1962), S. 1197-1198 
    ISSN: 1476-4687
    Source: Nature Archives 1869 - 2009
    Topics: Biology , Chemistry and Pharmacology , Medicine , Natural Sciences in General , Physics
    Notes: [Auszug] (a) The third paragraph of the earlier communication should be replaced by the following: From this it follows that, in sufficiently dilute solutions: spC (2) and for in such solutions: ktfr = In (1 + tsp) = (3) Subtracting (3) from (2), we obtain: - - -- = -5- hn] 4- (TT -f k' ' -n c c R L ...
    Type of Medium: Electronic Resource
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  • 7
    Electronic Resource
    Electronic Resource
    New York : Wiley-Blackwell
    Journal of Bioluminescence and Chemiluminescence 3 (1989), S. 193-199 
    ISSN: 0884-3996
    Keywords: Gene regulation ; bacterial bioluminescence ; Vibrio fischeri ; Vibrio harveyi ; lux genes ; Chemistry ; Biochemistry and Biotechnology
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Biology , Chemistry and Pharmacology
    Notes: Comparison of the nucleotide sequences and gene organization of the lux systems from Vibrio harveyi and Vibrio fischeri has demonstrated that the location and order of the lux structural genes are highly conserved whereas considerable divergence has arisen in the location and/or presence of lux regulatory genes in the two marine bacteria. The order of the lux structural genes (luxCDABE) are identical in the two bacteria with the three fatty acid reductase genes (luxCDE) required for aldehyde biosynthesis flanking the luciferase genes (luxAB). Complementation in trans of the upstream V. fischeri DNA containing the luxC and luxD structural genes with the downstream luxA, B and E genes of V. harveyi resulted in luminescent Escherichia coli that did not require any exogenous aldehyde. These results indicate that the light-emitting systems are very similar in the two bacteria.However, the lux regulatory systems in these two bacteria appear to have clearly diverged. In V. harveyi, an open reading frame of 〉40 codons does not exist within 600 bp of the start of luxC in contrast to the luxl regulatory gene present in the V. fischeri lux system. An open reading frame of 615 bp is present farther upstream of luxC with the same direction of transcription and approximate location as the luxR regulatory gene of V. fischeri; however, apparent homologies do not exist between the two genes. The similarities in organization of the lux structural genes and the differences in the existence and/or location of lux regulatory genes in the two Vibrio species raises the question of how these marine bacteria can have a similar growth-dependent regulation of luminescence expression.
    Additional Material: 7 Ill.
    Type of Medium: Electronic Resource
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  • 8
    ISSN: 0022-3832
    Keywords: Chemistry ; Polymer and Materials Science
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology , Physics
    Notes: The viscosity slope constant k′, i.e., \documentclass{article}\pagestyle{empty}\begin{document}$ \mathop {\lim }\limits_{c \to 0} \frac{{d\left( {{{\eta _{sp} } \mathord{\left/ {\vphantom {{\eta _{sp} } c}} \right. \kern-\nulldelimiterspace} c}} \right)}}{{dc}}\frac{1}{{[\eta ]^2 }} $\end{document}, is shown to be of increasing significance in polymer science as a molecular-weight-independent criterion of solvent power and as a parameter sensitive to various changes in polymer structure, such as long-chain branching. Ideally, it is a dimensionless parameter, independent of molecular size, which arises only from the mutual hydrodynamic interaction of polymer molecules and depends, therefore, on the intrinsic flexibility of the polymer chain and on the polymer density in the coiled molecule. In real systems, however, other interactions may contribute, sometimes very significantly, to k′. For such real systems, the general expression: \documentclass{article}\pagestyle{empty}\begin{document}$ k' = k + a + \frac{K}{{[\eta ]^2 }}\left( {[\eta ]_{(2)} - [\eta ]_{(1)} } \right) $\end{document} is suggested. In ternary systems, polymer-polymer-solvent, ideal expressions for ηsp/c and k′ are developed, that for k′ being: \documentclass{article}\pagestyle{empty}\begin{document}$ k' = \sum\limits_i {\sum\limits_j {\surd \bar k_i [\eta ]_i w_i {{\surd \bar k_j [\eta ]_i w_i } \mathord{\left/ {\vphantom {{\surd \bar k_j [\eta ]_i w_i } {(\sum\limits_i {[\eta ]_i w_i } )^2 }}} \right. \kern-\nulldelimiterspace} {(\sum\limits_i {[\eta ]_i w_i } )^2 }}} } $\end{document} It is proposed that deviations from ideal behavior so defined are due to nonhydrodynamic polymer-polymer interactions and might be used to detect and measure the strength of such interactions. Some preliminary data for the system polystyrene-poly(methyl methacrylate)-m-xylene are presented and discussed.
    Additional Material: 3 Ill.
    Type of Medium: Electronic Resource
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  • 9
    ISSN: 0022-3832
    Keywords: Chemistry ; Polymer and Materials Science
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology , Physics
    Notes: The viscosity behavior of a high molecular weight fraction (M̄w = 9.8 × 106) of dextran (B-512) in aqueous solutions was studied at low and medium shear stresses, and its intrinsic viscosity was shown to be independent of shear stress. A convenient and precise multibulb Ubbelohde-type viscometer, especially designed for use with aqueous solutions is described. The calibration of the viscometer and the evaluation of surfacetension corrections of relative flow times measured in it are discussed in detail.
    Additional Material: 3 Ill.
    Type of Medium: Electronic Resource
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  • 10
    Electronic Resource
    Electronic Resource
    Hoboken, NJ : Wiley-Blackwell
    Journal of Polymer Science 13 (1954), S. 167-174 
    ISSN: 0022-3832
    Keywords: Chemistry ; Polymer and Materials Science
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology , Physics
    Notes: For the viscometric determination of the molecular weight of a flexible linear high polymer, a very “poor” solvent in which the osmotic slope constant B is zero (i.e., a so-called “ideal” solvent) has several advantages over the usually preferred good ones. For example, shear effects that are very troublesome with very high polymers in good solvents become negligible or easily manageable. Moreover, in an “ideal” solvent, the “contents” K and a in the equation relating [η] and M really are constant over a very wide range of molecular weights and, since a always has the value 0.50, are more easily determined. Because the advantages seem to outweigh considerably the disadvantages, the use of an “ideal” solvent should be given careful consideration, particularly when the molecular weights are very high or cover a wide range.
    Additional Material: 2 Ill.
    Type of Medium: Electronic Resource
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