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Elastic Losses in Some High Polymers as a Function of Frequency and Temperature
1.R. Simha, J. App. Phys. 13, 147 (1942);
1.T. Alfrey and P. Doty, J. App. Phys. 16, 700 (1945);
1.W. Kuhn, Zeits. f. Physik. Chemie B42, 1 (1939).
2.The relaxation theory can also be applied in cases where the relaxation is not due to a molecular rearrangement, but rather to heat flow. In this case the relaxation time is a function of the boundary conditions and therefore of the external shape of the body or of the grain structure of the substance. In this article we will refer only to relaxation phenomena which are governed by the motion of the molecules. C. Zener, Metals Tech. , 13 (1946).
2.K. Bennewitz and H. Rötger, Physik. Zeits. 37, 578 (1936);
2.K. Bennewitz and H. Rötger, 40, 416 (1939)., Phys. Z.
3.See e.g. P. Debye and H. Sack; Handb. Rad. (1934); Vol. VI, part 1, p. 141.
4.J. G. Kirkwood, J. Chem. Phys. 14, 180 (1946).
5.R. M. Fuoss and J. G. Kirkwood, J. Am. Chem. Soc. 63, 385 (1941).
6.The relaxation theory has been tested for nonperiodic motions, as for instance in the case of creep, etc.
7.R. M. Fuoss, J. Am. Ch. Soc. 63, 369 (1941).
8.We are obliged to Dr. Fuoss, at that time at General Electric, for providing us with these samples.
9.R. B. Stambaugh, Ind. Eng. Chem. 34, 1358 (1942).
10.H. S. Sack, J. Motz, and R. N. Work, J. App. Phys. 15, 396 (1944).
11.These samples were kindly given to us by the U.S. Rubber Company.
12.R. F. Boyer and R. S. Spencer, Advances in Colloid Sciences (Interscience Publishers, New York, 1946), Vol. II, p. 1.
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