Infinite‐dilution viscoelastic properties of tobacco mosaic virus
Identifieur interne : 000B08 ( Istex/Corpus ); précédent : 000B07; suivant : 000B09Infinite‐dilution viscoelastic properties of tobacco mosaic virus
Auteurs : Norio Nemoto ; John L. Schrag ; John D. Ferry ; Robert W. FultonSource :
- Biopolymers [ 0006-3525 ] ; 1975-02.
English descriptors
- Teeft :
- Aggregated, Aggregated sample, Aqueous solvents, Asymptotic limit, Axial ratio, Characteristic relaxation time, Chem, Computerized data acquisition, Concentration range, Constant value, Electron micrographs, Frequency dependence, Frictional resistance, High frequencies, Higher frequencies, Infinite dilution, Intermolecular interaction, Intrinsic moduli, Intrinsic shear moduli, Intrinsic viscosity, Logarithmic plots, Loss shear moduli, Modulus, Mole fraction, Molecular weight, Phys, Polymer, Reasonable agreement, Resonator, Resonator housing, Rigid rodlike macromolecule, Rigid rods, Solid lines, Solvent viscosity, Theoretical curve, Theoretical value, Titanium resonator, Tobacco mosaic virus, Unaggregated sample, Viscoelastic properties.
Abstract
The storage and loss shear moduli, G′ and G″, have been measured for dilute solutions of unaggregated and aggregated tobacco mosaic virus samples in glycerol–water mixtures, by the Birnboim–Schrag multiple‐lumped resonator modified for use with aqueous solvents. The frequency range was 100–5800 Hz, the concentration range 0.6–2.1 × 10−3 g/ml, and the temperatures 25.0° and 37.8°C. The number‐average and weight‐average molecular weights of the aggregated sample were estimated as 1.4 and 2.0 × 108, respectively, from electron microscopy. The extrapolated intrinsic moduli [G′] and [G″] were compared with the predictions of the Kirkwood–Auer theory for rigid rodlike molecules. For the unaggregated sample, the frequency dependence of [G′] and [G″] agreed well with the theory assuming the intrinsic viscosity to be 27 ml/g, though the asymptotic limit of [G′]M/RT at higher frequencies was slightly larger than the theoretical value of 3/5. For the aggregated sample, the data agreed with theory for rigid rods as modified to account for molecular‐weight distribution.
Url:
DOI: 10.1002/bip.1975.360140213
Links to Exploration step
ISTEX:5E8866462DB60F8E132705F6A3209B53BA62C6F2Le document en format XML
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The extrapolated intrinsic moduli [G′] and [G″] were compared with the predictions of the Kirkwood–Auer theory for rigid rodlike molecules. For the unaggregated sample, the frequency dependence of [G′] and [G″] agreed well with the theory assuming the intrinsic viscosity to be 27 ml/g, though the asymptotic limit of [G′]M/RT at higher frequencies was slightly larger than the theoretical value of 3/5. 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type="institution">University of Wisconsin</orgName><address><addrLine>Madison</addrLine><addrLine>Wisconsin 53706</addrLine><country key="US" xml:lang="en">UNITED STATES</country></address></affiliation></author><author xml:id="author-0001"><persName><forename type="first">John L.</forename><surname>Schrag</surname></persName><affiliation><orgName type="division">Department of Chemistry</orgName><orgName type="institution">University of Wisconsin</orgName><address><addrLine>Madison</addrLine><addrLine>Wisconsin 53706</addrLine><country key="US" xml:lang="en">UNITED STATES</country></address></affiliation></author><author xml:id="author-0002"><persName><forename type="first">John D.</forename><surname>Ferry</surname></persName><affiliation><orgName type="division">Department of Chemistry</orgName><orgName type="institution">University of Wisconsin</orgName><address><addrLine>Madison</addrLine><addrLine>Wisconsin 53706</addrLine><country key="US" xml:lang="en">UNITED STATES</country></address></affiliation></author><author xml:id="author-0003"><persName><forename type="first">Robert W.</forename><surname>Fulton</surname></persName><affiliation><orgName type="department">Department of Plant Pathology</orgName><orgName type="institution">University of Wisconsin</orgName><address><addrLine>Madison</addrLine><addrLine>Wisconsin 53706</addrLine><country key="US" xml:lang="en">UNITED STATES</country></address></affiliation></author><idno type="istex">5E8866462DB60F8E132705F6A3209B53BA62C6F2</idno><idno type="ark">ark:/67375/WNG-3FG82KJJ-F</idno><idno type="DOI">10.1002/bip.1975.360140213</idno><idno type="unit">BIP360140213</idno><idno type="toTypesetVersion">file:BIP.BIP360140213.pdf</idno></analytic><monogr><title level="j" type="main">Biopolymers</title><title level="j" type="alt">BIOPOLYMERS</title><idno type="pISSN">0006-3525</idno><idno type="eISSN">1097-0282</idno><idno type="book-DOI">10.1002/(ISSN)1097-0282</idno><idno 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The extrapolated intrinsic moduli [<hi rend="italic">G</hi>′] and [<hi rend="italic">G</hi>″] were compared with the predictions of the Kirkwood–Auer theory for rigid rodlike molecules. For the unaggregated sample, the frequency dependence of [<hi rend="italic">G</hi>′] and [<hi rend="italic">G</hi>″] agreed well with the theory assuming the intrinsic viscosity to be 27 ml/g, though the asymptotic limit of [<hi rend="italic">G</hi>′]<hi rend="italic">M</hi>/<hi rend="italic">RT</hi> at higher frequencies was slightly larger than the theoretical value of 3/5. 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affiliationRef="#af1"><personName><givenNames>John D.</givenNames><familyName>Ferry</familyName></personName></creator><creator xml:id="au4" creatorRole="author" affiliationRef="#af2"><personName><givenNames>Robert W.</givenNames><familyName>Fulton</familyName></personName></creator></creators><affiliationGroup><affiliation xml:id="af1" countryCode="US" type="organization"><unparsedAffiliation>Department of Chemistry, University of Wisconsin, Madison, Wisconsin 53706</unparsedAffiliation></affiliation><affiliation xml:id="af2" countryCode="US" type="organization"><unparsedAffiliation>Department of Plant Pathology, University of Wisconsin, Madison, Wisconsin 53706</unparsedAffiliation></affiliation></affiliationGroup><abstractGroup><abstract type="main" xml:lang="en"><title type="main">Abstract</title><p>The storage and loss shear moduli, <i>G</i>′ and <i>G</i>″, have been measured for dilute solutions of unaggregated and aggregated tobacco mosaic virus samples in glycerol–water mixtures, by the Birnboim–Schrag multiple‐lumped resonator modified for use with aqueous solvents. The frequency range was 100–5800 Hz, the concentration range 0.6–2.1 × 10<sup>−3</sup> g/ml, and the temperatures 25.0° and 37.8°C. The number‐average and weight‐average molecular weights of the aggregated sample were estimated as 1.4 and 2.0 × 10<sup>8</sup>, respectively, from electron microscopy. The extrapolated intrinsic moduli [<i>G</i>′] and [<i>G</i>″] were compared with the predictions of the Kirkwood–Auer theory for rigid rodlike molecules. For the unaggregated sample, the frequency dependence of [<i>G</i>′] and [<i>G</i>″] agreed well with the theory assuming the intrinsic viscosity to be 27 ml/g, though the asymptotic limit of [<i>G</i>′]<i>M</i>/<i>RT</i> at higher frequencies was slightly larger than the theoretical value of 3/5. For the aggregated sample, the data agreed with theory for rigid rods as modified to account for molecular‐weight distribution.</p></abstract></abstractGroup></contentMeta></header></component></istex:document></istex:metadataXml><mods version="3.6"><titleInfo lang="en"><title>Infinite‐dilution viscoelastic properties of tobacco mosaic virus</title></titleInfo><titleInfo type="abbreviated" lang="en"><title>VISCOELASTIC OF TOBACCO MOSAIC VIRUS</title></titleInfo><titleInfo type="alternative" contentType="CDATA" lang="en"><title>Infinite‐dilution viscoelastic properties of tobacco mosaic virus</title></titleInfo><name type="personal"><namePart type="given">Norio</namePart><namePart type="family">Nemoto</namePart><affiliation>Department of Chemistry, University of Wisconsin, Madison, Wisconsin 53706</affiliation><role><roleTerm type="text">author</roleTerm></role></name><name type="personal"><namePart type="given">John L.</namePart><namePart type="family">Schrag</namePart><affiliation>Department of Chemistry, University of Wisconsin, Madison, Wisconsin 53706</affiliation><role><roleTerm type="text">author</roleTerm></role></name><name type="personal"><namePart type="given">John D.</namePart><namePart type="family">Ferry</namePart><affiliation>Department of Chemistry, University of Wisconsin, Madison, Wisconsin 53706</affiliation><role><roleTerm type="text">author</roleTerm></role></name><name type="personal"><namePart type="given">Robert W.</namePart><namePart type="family">Fulton</namePart><affiliation>Department of Plant Pathology, University of Wisconsin, Madison, Wisconsin 53706</affiliation><role><roleTerm type="text">author</roleTerm></role></name><typeOfResource>text</typeOfResource><genre type="article" displayLabel="article" authority="ISTEX" authorityURI="https://content-type.data.istex.fr" valueURI="https://content-type.data.istex.fr/ark:/67375/XTP-6N5SZHKN-D">article</genre><originInfo><publisher>Wiley Subscription Services, Inc., A Wiley Company</publisher><place><placeTerm type="text">Hoboken</placeTerm></place><dateIssued encoding="w3cdtf">1975-02</dateIssued><dateCaptured encoding="w3cdtf">1974-09-20</dateCaptured><dateValid encoding="w3cdtf">1974-11-04</dateValid><copyrightDate encoding="w3cdtf">1975</copyrightDate></originInfo><language><languageTerm type="code" authority="rfc3066">en</languageTerm><languageTerm type="code" authority="iso639-2b">eng</languageTerm></language><physicalDescription><extent unit="figures">3</extent><extent unit="tables">3</extent><extent unit="references">22</extent></physicalDescription><abstract lang="en">The storage and loss shear moduli, G′ and G″, have been measured for dilute solutions of unaggregated and aggregated tobacco mosaic virus samples in glycerol–water mixtures, by the Birnboim–Schrag multiple‐lumped resonator modified for use with aqueous solvents. The frequency range was 100–5800 Hz, the concentration range 0.6–2.1 × 10−3 g/ml, and the temperatures 25.0° and 37.8°C. The number‐average and weight‐average molecular weights of the aggregated sample were estimated as 1.4 and 2.0 × 108, respectively, from electron microscopy. The extrapolated intrinsic moduli [G′] and [G″] were compared with the predictions of the Kirkwood–Auer theory for rigid rodlike molecules. For the unaggregated sample, the frequency dependence of [G′] and [G″] agreed well with the theory assuming the intrinsic viscosity to be 27 ml/g, though the asymptotic limit of [G′]M/RT at higher frequencies was slightly larger than the theoretical value of 3/5. 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