Key result
PDMS molecular weight dictates network small-strain modulus with a 0.16-MPa entanglement plateau.
Why the study?
Small-strain equilibrium modulus data of end-linked PDMS networks vary with crosslinking variables, but the influence of molecular weight and crosslinker functionality needed comprehensive review.
This review of PDMS networks confirms that molecular weight is the dominating variable for small-strain equilibrium modulus and supports the phantom and tube models.
Small-strain equilibrium modulus data of polydimethylsiloxane (PDMS) networks are reviewed. 58 different articles in the literature with values of the modulus of end-linked PDMS networks were found [1-58] including more than 250 values of the small-strain equilibrium modulus as function of variables in the crosslinking system. The dominating variable is shown to be the molecular weight of PDMS as expected, whereas the functionality of the crosslinker methylhydrosiloxane/ dimethylsiloxane copolymer is shown to be less important in good agreement with the phantom model. The data collected was fitted to the phenomenological model of Langley and Graessley including an entanglement contribution. The fitted entanglement plateau (0.16 MPa) is in good agreement with literature values and with the theoretical prediction of the tube model. Experimental data for the Mooney-Rivlin constants was found and it was shown that C2 is constant with increasing functionality. Furthermore it was found that trapped entanglements can be split into two categories, viz. locked entanglements contributing to the C1 term and traditionally trapped entanglements contributing to C2.
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Larsen et al. (2004) conducted a review in Polydimethylsiloxane (PDMS) networks. Polydimethylsiloxane (PDMS) networks was evaluated on Small-strain equilibrium modulus. Review of 58 articles showed the dominating variable for small-strain equilibrium modulus of PDMS networks is the molecular weight of PDMS, with the fitted entanglement plateau at 0.16 MPa.
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