Cylindrical coordinate system
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The cylindrical coordinate system is a three-dimensional system which essentially extends circular polar coordinates by adding a third coordinate (usually denoted [h]) which measures the height of a point above the plane.
A point P is given as [(r, \theta, h)]. In terms of the Cartesian coordinate system:
- [r] 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.
- [\theta] is the angle between the positive x-axis and the line OP', measured anti-clockwise.
- [h] is the same as [z].
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.
Line and volume elements
In many problems involving cylindrical polar coordinates, it is useful to know the line and volume elements; these are used in integration to solve problems involving paths and volumes.
The line element is [dl\ = dr\ + r\,d\theta\ + dz].
The volume element is [dV\ = r\,dr\,d\theta\,dz].
It is also important in many cases to be able to find the gradient of a vector field in cylindrical polar coordinates. The gradient can be worked out from first principals, if one knows theta, r and z in terms of cartesian coordinates, but the general equation is given below.
[\nabla \equiv \mathbf\frac + \boldsymbol\frac\frac + \mathbf\frac].
See also
- List of canonical coordinate transformations
- Cartesian coordinate system
- Spherical coordinate system
- Parabolic coordinate system
- Vector fields in cylindrical and spherical coordinates
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