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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 ( r, \theta \,). The solution is such that the stress components are in the form of a Fourier series in \theta \, .
Michell showed that the general solution can be expressed in terms of an Airy stress function of the form
:
\begin
\varphi &= A_0~r^2 + B_0~r^2~\ln(r) + C_0~\ln(r) + D_0~\theta \\
& + \left(A_1~r + B_1~r^ + B_1^~r~\theta + C_1~r^3 +
D_1~r~\ln(r)\right) \cos\theta \\
& + \left(E_1~r + F_1~r^ + F_1^~r~\theta + G_1~r^3 +
H_1~r~\ln(r)\right) \sin\theta \\
& + \sum_^ \left(A_n~r^n + B_n~r^ + C_n~r^ + D_n~r^\right)\cos(n\theta) \\
& + \sum_^ \left(E_n~r^n + F_n~r^ + G_n~r^ + H_n~r^\right)\sin(n\theta)
\end

The terms A_1~r~\cos\theta\, and E_1~r~\sin\theta\, 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. 〕
\,
! \sigma_\,
|-
| r^2\,
| 2
| 0
| 2
|-
| r^2~\ln r
| 2~\ln r + 1
| 0
| 2~\ln r + 3
|-
| \ln r\,
| r^\,
| 0
| -r^\,
|-
| \theta\,
| 0
| r^\,
| 0
|-
|-
| r^3~\cos\theta \,
| 2~r~\cos\theta \,
| 2~r~\sin\theta \,
| 6~r~\cos\theta \,
|-
| r\theta~\cos\theta \,
| 2~r^~\sin\theta \,
| 0
| 0
|-
| r~\ln r~\cos\theta \,
| r^~\cos\theta \,
| r^~\sin\theta \,
| r^~\cos\theta \,
|-
| r^~\cos\theta \,
| -2~r^~\cos\theta \,
| -2~r^~\sin\theta \,
| 2~r^~\cos\theta \,
|-
|-
| r^3~\sin\theta \,
| 2~r~\sin\theta \,
| -2~r~\cos\theta \,
| 6~r~\sin\theta \,
|-
| r\theta~\sin\theta \,
| 2~r^~\cos\theta \,
| 0
| 0
|-
| r~\ln r~\sin\theta \,
| r^~\sin\theta \,
| -r^~\cos\theta \,
| r^~\sin\theta \,
|-
| r^~\sin\theta \,
| -2~r^~\sin\theta \,
| 2~r^~\cos\theta \,
| 2~r^~\sin\theta \,
|-
|-
| r^~\cos(n\theta) \,
| -(n+1)(n-2)~r^n~\cos(n\theta) \,
| n(n+1)~r^n~\sin(n\theta) \,
| (n+1)(n+2)~r^n~\cos(n\theta \,
|-
| r^~\cos(n\theta) \,
| -(n+2)(n-1)~r^~\cos(n\theta) \,
| -n(n-1)~r^~\sin(n\theta)\,
| (n-1)(n-2)~r^~\cos(n\theta)
|-
| r^n~\cos(n\theta) \,
| -n(n-1)~r^~\cos(n\theta) \,
| n(n-1)~r^~\sin(n\theta) \,
| n(n-1)~r^~\cos(n\theta) \,
|-
| r^~\cos(n\theta) \,
| -n(n+1)~r^~\cos(n\theta) \,
| -n(n+1)~r^~\sin(n\theta) \,
| n(n+1)~r^~\cos(n\theta) \,
|-
|-
| r^~\sin(n\theta) \,
| -(n+1)(n-2)~r^n~\sin(n\theta) \,
| -n(n+1)~r^n~\cos(n\theta) \,
| (n+1)(n+2)~r^n~\sin(n\theta \,
|-
| r^~\sin(n\theta) \,
| -(n+2)(n-1)~r^~\sin(n\theta) \,
| n(n-1)~r^~\cos(n\theta)\,
| (n-1)(n-2)~r^~\sin(n\theta)
|-
| r^n~\sin(n\theta) \,
| -n(n-1)~r^~\sin(n\theta) \,
| -n(n-1)~r^~\cos(n\theta) \,
| n(n-1)~r^~\sin(n\theta) \,
|-
| r^~\sin(n\theta) \,
| -n(n+1)~r^~\sin(n\theta) \,
| n(n+1)~r^~\cos(n\theta) \,
| n(n+1)~r^~\sin(n\theta) \,
|}

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
ウィキペディアで「Michell solution」の詳細全文を読む



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