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Michell solution : ウィキペディア英語版 | Michell solution The Michell solution is a general solution to the elasticity equations in polar coordinates (). The solution is such that the stress components are in the form of a Fourier series in . Michell showed that the general solution can be expressed in terms of an Airy stress function of the form : The terms and define a trivial null state of stress and are ignored. == Stress components == The stress components can be obtained by substituting the Michell solution into the equations for stress in terms of the Airy stress function (in cylindrical coordinates). A table of stress components is shown below.〔 J. R. Barber, 2002, ''Elasticity: 2nd Edition'', Kluwer Academic Publishers. 〕 \, ! |- | | | | |- | | | | |- | | | | |- | | | | |- |- | | | | |- | | | | |- | | | | |- | | | | |- |- | | | | |- | | | | |- | | | | |- | | | | |- |- | | | | |- | | | | |- | | | | |- | | | | |- |- | | | | |- | | | | |- | | | | |- | | | | |}
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