Cylindrical coordinate system
circular polar coordinates by adding a third coordinate (usually denoted <math>h<math>) which measures the height of a point above the plane.
A point P is given as <math>(r, \theta, h)<math>. In terms of the Cartesian coordinate system:
- <math>r<math> is the distance from O to P', the orthogonal projection of the point P onto the XY plane. This is the same as the distance of P to the z-axis.
- <math>\theta<math> is the angle between the positive x-axis and the line OP', measured anti-clockwise.
- <math>h<math> is the same as <math>z<math>.
Some mathematicians indeed use <math>(r, \theta, z)<math>.
Cylindrical coordinates are useful in analyzing surfaces that are symmetrical about an axis, with the z-axis chosen as the axis of symmetry. For example, the infinitely long circular cylinder that has the Cartesian equation x2 + y2 = c2 has the very simple equation r = c in cylindrical coordinates. Hence the name "cylindrical" coordinates.
Conversion from cylindrical to Cartesian coordinates
|
<math>x = r \cos\theta<math>
<math>y = r \sin\theta<math>
<math>z = h<math>
| |
<math>
\begin{vmatrix}dx\\dy\\dz\end{vmatrix}
=
\begin{vmatrix}
\cos\theta&-r\sin\theta&0\\
\sin\theta&r\cos\theta&0\\
0&0&1
\end{vmatrix}
\cdot
\begin{vmatrix}dr\\d\theta\\dh\end{vmatrix}
<math>
|
Conversion from Cartesian to cylindrical coordinates
|
<math>r = \sqrt{x^2 + y^2}<math>
<math>\theta = \arctan\frac{y}{x}<math>
<math>h = z\,<math>
| |
<math>
\begin{vmatrix}dr\\d\theta\\dh\end{vmatrix}
=
\begin{vmatrix}
\frac{x}{\sqrt{x^2+y^2}}&\frac{y}{\sqrt{x^2+y^2}}&0\\
\frac{-y}{x^2+y^2}&\frac{x}{x^2+y^2}&0\\
0&0&1
\end{vmatrix}
\cdot
\begin{vmatrix}dx\\dy\\dz\end{vmatrix}
<math>
|
Conversion from cylindrical to spherical coordinates
|
<math>{\rho} = \sqrt{r^2+h^2}<math>
<math>{\phi} = \theta \qquad <math>
<math>{\theta'} = \arctan\frac{h}{r} \qquad <math>
| |
<math>
\begin{vmatrix}d\rho\\d\phi\\d\theta' \end{vmatrix}
=
\begin{vmatrix}
\frac{r}{\sqrt{r^2+h^2}} & 0 & \frac{h}{\sqrt{r^2+h^2}} \\
0 & 1 & 0 \\
\frac{-h}{r^2+h^2} & 0 & \frac{r}{r^2+h^2}
\end{vmatrix}
\cdot
\begin{vmatrix}dr\\d\theta\\dh\end{vmatrix}
<math> |
where φ is the azimuth and θ' is the latitude.
Conversion from spherical to cylindrical coordinates
|
<math>{r} = \rho \cos \theta <math>
<math>{\theta'} = \phi <math>
<math>{h} = \rho \sin \theta <math>
| |
<math>
\begin{vmatrix}dr\\d\theta'\\dh\end{vmatrix}
=
\begin{vmatrix}
\cos \theta & 0 & - \rho \sin \theta \\
0 & 1 & 0 \\
\sin \theta & 0 & \rho \cos \theta
\end{vmatrix}
\cdot
\begin{vmatrix}d\rho\\d\phi\\d\theta\end{vmatrix}
<math>
|
where φ is azimuth and θ is latitude.
See also
