Special curvilinear coordinates

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1. Cylindrical coordinates (\rho, \phi, z)

Transformation equations:  x = \rho\cos\phi ,\ y = \rho\sin\phi ,\ z = z

where \rho \ge 0 ,  0 \le \phi \le 2\pi,  -\infty < z < \infty [/latex].    <em>Scale factors</em>: [latex]h_1 = 1,\ h_2 = 1,\ h_3 = 1

Element of arc length:  ds^2 = d\rho^2 + \rho^2 d\phi^2 + dz^2

Jacobian: \displaystyle \frac{\partial(x, y, z)}{\partial(\rho, \phi, z)} = \rho

Element of volume:  dV = \rho d\rho d\phi dz

Laplacian: \displaystyle \nabla^2U = \frac{1}{\rho}\frac{\partial}{\partial\rho}\left( \rho\frac{\partial U}{\partial\rho} \right) + \frac{1}{\rho^2}\frac{\partial^2U}{\partial\phi^2} + \frac{\partial^2U}{\partial z^2}   = \frac{\partial^2U}{\partial\rho^2} + \frac{1}{\rho}\frac{\partial U}{\partial\rho} + \frac{1}{\rho^2}\frac{\partial^2U}{\partial\phi^2} + \frac{\partial^2U}{\partial z^2}

Note that corresponding results can be obtained for polar coordinates in the plane by omitting z dependence. In such case for example, ds^2 = d\rho^2 + \rho^2d\phi^2, while the element of volume is replaced by the element of area, dA = \rho d\rho d\phi.

2. Spherical coordinates (r, \theta, \phi)

Transformation equations: x = r\sin\theta,\ y = r\sin\theta\sin\phi,\ z = r\cos\theta

where r \ge 0,\ 0 \le \theta \le \pi,\ 0 \le \phi \le 2\pi .

Scale factors: h_1 = 1,\ h_2 = r,\ h_3 = r\sin\theta

Element of arc length:  ds^2 = dr^2 + r^2d\theta^2 + r^2\sin^2\theta d\phi^2

Jacobian: \displaystyle \frac{\partial(x, y, z)}{\partial(r, \theta, \phi)} = r^2\sin\theta

Element of volume:  dV = r^2\sin\theta drd\theta d\phi

Laplacian: \displaystyle \nabla^2U = \frac{1}{r^2}\frac{\partial}{\partial r}\left(r^2\frac{\partial U}{\partial r}\right) + \frac{1}{r^2\sin\theta}\frac{\partial}{\partial\theta}\left(\sin\theta\frac{\partial U}{\partial\theta}\right) + \frac{1}{r^2\sin^2\theta}\frac{\partial^2U}{\partial\phi^2}

Other types of coordinate systems are possible.

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投稿者: admin

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