Hu–Washizu principle

In continuum mechanics, and in particular in finite element analysis, the Hu–Washizu principle is a variational principle which says that the action

\int _{V^{e}}\left[{\frac {1}{2}}\varepsilon ^{T}C\varepsilon -\sigma ^{T}\varepsilon +\sigma ^{T}(\nabla u)-{\bar {p}}^{T}u\right]dV-\int _{S_{\sigma }^{e}}{\bar {T}}^{T}u\ dS

is stationary, where $C$ is the elastic stiffness tensor. The Hu–Washizu principle is used to develop mixed finite element methods.^[1] The principle is named after Hu Haichang and Kyūichirō Washizu.

References

↑ Jihuan, He (June 1997). "Equivalent theorem of Hellinger–Reissner and Hu–Washizu variational principles". Journal of Shanghai University. Shanghai University Press. 1 (1): 36–41. doi:10.1007/s11741-997-0041-1. ISSN 1007-6417. S2CID 119852325.

Further reading

K. Washizu: Variational Methods in Elasticity & Plasticity, Pergamon Press, New York, 3rd edition (1982)
O. C. Zienkiewicz, R. L. Taylor, J. Z. Zhu : The Finite Element Method: Its Basis and Fundamentals, Butterworth–Heinemann, (2005).

This article is issued from Wikipedia. The text is licensed under Creative Commons - Attribution - Sharealike. Additional terms may apply for the media files.