Abstract

The dynamical behavior of an viscoelastic body is known to be well described by fractional derivatives of the amount of deformation. The physical reason of this fact is the underlying fractal nature of the molecular structure of such materials. By using the Schiessel-Blumen ladder of mechanical system, it has been shown that the fractal structure would produce the asymptotic power law decay of the deformation, which is the most distinguished characteristics of fractional derivatives. So far, this has been shown by asymptotic behavior of the Laplace transform of the impulse response of the relaxation. Here, we generalize this result, and show that the exact solution of the impulse response function is obtained for a large class of parameter values in terms of confluent hypergeometric functions. The asymptotic expression is then readily obtained which shows the power law decay.

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