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7.1 Power Law

The Power Law model cannot be combined with a user-specified starting time [Vol. Analysis Procedures].

    (syntax)


\begin{figure}\centering
\begin{tabbing}
\texttt{'MATERI'}
\\ [-1.0ex]
\rule{14...
...extit{alpha}}\(_{r}\,\)
\texttt{\textit{d}}\(_{r}\,\) \end{tabbing} \end{figure}


POWER
specifies viscoelasticity with the Power Law model [§19.2.2].

J(t,$\displaystyle \tau$) = $\displaystyle {\frac{{1}}{{E(\tau)}}}$$\displaystyle \left(\vphantom{ 1 + \alpha \: \tau^{-d} ( t - \tau )^{p} }\right.$1 + $\displaystyle \alpha$ $\displaystyle \tau^{{-d}}_{}$(t - $\displaystyle \tau$)p$\displaystyle \left.\vphantom{ 1 + \alpha \: \tau^{-d} ( t - \tau )^{p} }\right)$ (7.1)

Parameter p is the power p (p > 0 )of the creep function part that depends on the loading time t - $ \tau$ . Parameter td is the development point td of the Taylor series approximation of the Power Law (dimension `time'). Best results are obtained if td is halfway the time interval. Parameter alpha is the creep coefficient $ \alpha$ . Parameter d is the power d of the part of the creep function that depends on the loading time. E($ \tau$) is the specified Young's modulus or the stiffness specified in §7.1.1.

    (file.dat)


'MATERI'
  1  YOUNG  2.E+4
     POISON 0.0
     POWER  0.3  84.0  3.0  0.35




Subsections
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DIANA-9.3 User's Manual - Material Library
First ed.

Copyright (c) 2008 by TNO DIANA BV.