| |
| | Introduction |
 | | Under assumptions such as the affine deformation of junction points and the additivity of individual strand entropy, the end-to-end distribution fuction directly leads to the network elasticity through either a finite-chain average or a network average [1, 8, 9]. |
 | | However, their agreement with experiments is incomplete, and many alternative theoretical models of elasticity have been proposed, ranging from the constrained fluctuation [10] and primitive path [11, 12] to sliplink [13, 14] and tube models [15, 16]. |
 | | The gradual breakdown of the affine assumption with increasing strain accounts for the eventual failure of the affine model and the necessity of other alternative ones. |
| www.tcm.phy.cam.ac.uk /~ym101/rubber/node1.html (547 words) |
|