Journal of the Society of Materials Science, Japan
Online ISSN : 1880-7488
Print ISSN : 0514-5163
ISSN-L : 0514-5163
Visco-Elastic Behaviour of Plasticized PVC Sheet under Biaxial Large Deformation
Kazuhiko SAKAGUCHISueo KAWABATAHiromichi KAWAI
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1971 Volume 20 Issue 208 Pages 90-96

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Abstract
In this paper the report is made of the measurement performed of the stress relaxation of plasticized PVC sheet under biaxial large deformation by means of a biaxial tensile tester. It is assumed that the material is an isotropic, homogeneous and incompressible, and the strain energy function W may be described in the following equation.
W=W(I1, I2)
The function W can be represented as the function of time t with respect to the stress relaxation. That is
W=W(I1, I2, t).
The partial derivatives of the strain energy are given in the following equation as the function of invariants of deformation tensor and time from the theory of continuous media.
∂W/∂I1(I1, I2, t)=1/2H(λ1222)[λ13f1(t)/λ121-2λ2-223f2(t)/λ221-2λ2-2]
∂W/∂I2(I1, I2, t)=1/2H(λ2212)[λ1f1(t)/λ121-2λ2-22f2(t)/λ221-2λ2-2](1)
The force fi in formula (1) has been measured by the stress relaxation experiment as a function of time t, and ∂W/∂Ii can be obtained by substituting fi(t) in formula (1).
It is observed that the relation between log(∂W/∂Ii) and log t is approximately expressed as a stright line having slope k. According to the slope of the line ∂W/∂Ii(t) is approximately represented in the following equation as a function of time.
∂W/∂Ii(I1, I2, t)=At-ki
where i=1, 2, A=A (I1, I2, t=t0).
The value of k is not constant for all deformation measured and also for different temperature. Some contour maps representing the surfaces of ∂W/∂I1 and ∂W/∂I2 as function of I1 and I2 are obtained for this materials at some fixed time t. It follows that the shape of contour map has not been influenced by the time, but it has been remarkably influenced by the temperature.
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© by The Society of Materials Science, Japan
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