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Newmark-beta method : ウィキペディア英語版
Newmark-beta method
The Newmark-beta method is a method of numerical integration used to solve differential equations. It is widely used in numerical evaluation of the dynamic response of structures and solids such as in finite element analysis to model dynamic systems. The method is named after Nathan M. Newmark,〔Newmark, N. M. (1959) A method of computation for structural dynamics. Journal of Engineering Mechanics, ASCE, 85 (EM3) 67-94.〕 former Professor of Civil Engineering at the University of Illinois, who developed it in 1959 for use in structural dynamics.
Using Taylor's theorem with Lagrange remainder, along with the intermediate value theorem, the Newmark-''β'' method states that the first time derivative (velocity in the equation of motion) can be solved as,
:\dot_=\dot_n+ \Delta t~\ddot_\gamma \,
where
:\ddot_\gamma = (1 - \gamma)\ddot_n + \gamma \ddot_~~~~0\leq \gamma \leq 1
therefore
:\dot_=\dot_n + (1 - \gamma) \Delta t~\ddot_n + \gamma \Delta t~\ddot_.
Because acceleration also varies with time, however, those two theorems must also be applied to the second time derivative to obtain the correct displacement. Thus,
:u_=u_n + \Delta t~\dot_n+\begin \frac 1 2 \end \Delta t^2~\ddot_\beta
where again
:\ddot_\beta = (1 - 2\beta)\ddot_n + 2\beta\ddot_~~~~0\leq 2\beta\leq 1
Newmark showed that a reasonable value of \gamma is 0.5, therefore the update rules are,
:\dot_=\dot_n + \begin\frac\end~(\ddot_n + \ddot_)
:u_=u_n + t~\dot_n + \begin\frac\end \Delta t^2 \ddot_n + \beta t^2 \ddot_
Setting ''β'' to various values between 0 and 1 can give a wide range of results. Typically ''β'' = 1/4, which yields the constant average acceleration method, is used.
==References==



抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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