{"title":"Elastic modulus formulae for a crosslinked network","authors":"A. Charlesby","doi":"10.1016/1359-0197(92)90068-Q","DOIUrl":null,"url":null,"abstract":"<div><p>The usual formula for the elastic modulus <em>E</em> of a crosslinked highly elastic network <em>E</em> = 3 <em>ρ</em>R<em>T</em>/<em>M</em><sub>c</sub> involves molecular weight between crosslinks <em>M</em><sub>c</sub>. It has to be modified by several factors such as the fraction not involved in any external stress and the initial molecular weight distribution. Several correction terms have been proposed. In this paper a fuller calculation is made for two initial molecular weight distributions, uniform and random, to see how far these corrections are valid. Even at high degrees of crosslinking a very significant proportion of the network does not participate in this elastic deformation.</p><p>It may appear preferable to relate the elastic modulus <em>E</em> to the number of effective segments between crosslinks, independent of their molecular weight <em>M</em><sub>c</sub><em>E</em> = 3<em>ρkTQ</em>(1 − <em>s</em><sup>2</sup>)<em>p</em> where <em>Q</em> is the number of crosslinked monomer units per unit volume, and (1 − <em>s</em><sup>2</sup>)<em>p</em> is a correction factor to allow for segments which are ineffective in an elastic deformation.</p></div>","PeriodicalId":14262,"journal":{"name":"International Journal of Radiation Applications and Instrumentation. Part C. Radiation Physics and Chemistry","volume":"40 2","pages":"Pages 117-120"},"PeriodicalIF":0.0000,"publicationDate":"1992-08-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/1359-0197(92)90068-Q","citationCount":"9","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"International Journal of Radiation Applications and Instrumentation. Part C. Radiation Physics and Chemistry","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/135901979290068Q","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 9

Abstract

The usual formula for the elastic modulus E of a crosslinked highly elastic network E = 3 ρRT/Mc involves molecular weight between crosslinks Mc. It has to be modified by several factors such as the fraction not involved in any external stress and the initial molecular weight distribution. Several correction terms have been proposed. In this paper a fuller calculation is made for two initial molecular weight distributions, uniform and random, to see how far these corrections are valid. Even at high degrees of crosslinking a very significant proportion of the network does not participate in this elastic deformation.

It may appear preferable to relate the elastic modulus E to the number of effective segments between crosslinks, independent of their molecular weight McE = 3ρkTQ(1 − s2)p where Q is the number of crosslinked monomer units per unit volume, and (1 − s2)p is a correction factor to allow for segments which are ineffective in an elastic deformation.

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交联网络的弹性模量公式
交联高弹性网络弹性模量E的常用公式E = 3 ρRT/Mc涉及交联间的分子量Mc,需要通过不受任何外力影响的比例和初始分子量分布等因素进行修正。提出了几个修正术语。本文对均匀和随机两种初始分子量分布进行了更全面的计算,以了解这些修正在多大程度上是有效的。即使在高度交联的情况下,也有相当大比例的网络不参与这种弹性变形。将弹性模量E与交联之间的有效段数联系起来,与它们的分子量无关,似乎是可取的。McE = 3ρkTQ(1−s2)p,其中Q是每单位体积交联单体单位的数量,(1−s2)p是一个校正因子,允许在弹性变形中无效的段。
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