In continuum mechanics, the Michell solution is a general solution to the elasticity equations in polar coordinates ( r , θ {\displaystyle r,\theta } ) developed by John Henry Michell in 1899. The solution is such that the stress components are in the form of a Fourier series in θ {\displaystyle \theta } .
In continuum mechanics, the Michell solution is a general solution to the elasticity equations in polar coordinates ( r , θ {\displaystyle r,\theta } ) developed by John Henry Michell in 1899. The solution is such that the stress components are in the form of a Fourier series in θ {\displaystyle \theta } .
Source: Wikipedia "Michell solution" · CC BY-SA 4.0
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