Cylindrical coordinate system explained

A cylindrical coordinate system is a three-dimensional coordinate system that specifies point positions by the distance from a chosen reference axis (axis L in the image opposite), the direction from the axis relative to a chosen reference direction (axis A), and the distance from a chosen reference plane perpendicular to the axis (plane containing the purple section). The latter distance is given as a positive or negative number depending on which side of the reference plane faces the point.

The origin of the system is the point where all three coordinates can be given as zero. This is the intersection between the reference plane and the axis.The axis is variously called the cylindrical or longitudinal axis, to differentiate it from the polar axis, which is the ray that lies in the reference plane, starting at the origin and pointing in the reference direction.Other directions perpendicular to the longitudinal axis are called radial lines.

The distance from the axis may be called the radial distance or radius, while the angular coordinate is sometimes referred to as the angular position or as the azimuth. The radius and the azimuth are together called the polar coordinates, as they correspond to a two-dimensional polar coordinate system in the plane through the point, parallel to the reference plane. The third coordinate may be called the height or altitude (if the reference plane is considered horizontal), longitudinal position,^[1] or axial position.^[2]

Cylindrical coordinates are useful in connection with objects and phenomena that have some rotational symmetry about the longitudinal axis, such as water flow in a straight pipe with round cross-section, heat distribution in a metal cylinder, electromagnetic fields produced by an electric current in a long, straight wire, accretion disks in astronomy, and so on.

They are sometimes called "cylindrical polar coordinates"^[3] and "polar cylindrical coordinates",^[4] and are sometimes used to specify the position of stars in a galaxy ("galactocentric cylindrical polar coordinates").^[5]

Definition

The three coordinates of a point are defined as:

• The radial distance is the Euclidean distance from the -axis to the point .
• The azimuth is the angle between the reference direction on the chosen plane and the line from the origin to the projection of on the plane.
• The axial coordinate or height is the signed distance from the chosen plane to the point .

Unique cylindrical coordinates

As in polar coordinates, the same point with cylindrical coordinates has infinitely many equivalent coordinates, namely and where is any integer. Moreover, if the radius is zero, the azimuth is arbitrary.

In situations where someone wants a unique set of coordinates for each point, one may restrict the radius to be non-negative and the azimuth to lie in a specific interval spanning 360°, such as or .

Conventions

The notation for cylindrical coordinates is not uniform. The ISO standard 31-11 recommends, where is the radial coordinate, the azimuth, and the height. However, the radius is also often denoted or, the azimuth by or, and the third coordinate by or (if the cylindrical axis is considered horizontal), or any context-specific letter.

In concrete situations, and in many mathematical illustrations, a positive angular coordinate is measured counterclockwise as seen from any point with positive height.

Coordinate system conversions

The cylindrical coordinate system is one of many three-dimensional coordinate systems. The following formulae may be used to convert between them.

Cartesian coordinates

For the conversion between cylindrical and Cartesian coordinates, it is convenient to assume that the reference plane of the former is the Cartesian -plane (with equation), and the cylindrical axis is the Cartesian -axis. Then the -coordinate is the same in both systems, and the correspondence between cylindrical and Cartesian are the same as for polar coordinates, namelyin one direction, andin the other. The arcsine function is the inverse of the sine function, and is assumed to return an angle in the range = . These formulas yield an azimuth in the range .

By using the arctangent function that returns also an angle in the range =, one may also compute

\varphi without computing \rho first & \text x = 0 \text y \ne 0\\\arctan\left(\frac\right) & \mbox x > 0 \\\arctan\left(\frac\right)+\pi & \mbox x < 0 \text y \ge 0\\\arctan\left(\frac\right)-\pi & \mbox x < 0 \text y < 0\end \endFor other formulas, see the article Polar coordinate system.

Many modern programming languages provide a function that will compute the correct azimuth, in the range, given x and y, without the need to perform a case analysis as above. For example, this function is called by in the C programming language, and in Common Lisp.

Spherical coordinates

Spherical coordinates (radius, elevation or inclination, azimuth), may be converted to or from cylindrical coordinates, depending on whether represents elevation or inclination, by the following:

Conversion between spherical and cylindrical coordinates

Conversion to:	Coordinate	is elevation	is inclination
Cylindrical	=
=
=
Spherical	=	$\backslash sqrt$
=	$\backslash arctan\backslash left(\backslash frac\backslash right)$	$\backslash arctan\backslash left(\backslash frac\backslash right)$
=

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$$\backslash mathrm\backslash boldsymbol\; =\; \backslash mathrm\backslash rho\backslash ,\backslash boldsymbol\; +\; \backslash rho\backslash ,\backslash mathrm\backslash varphi\backslash ,\backslash boldsymbol\; +\; \backslash mathrmz\backslash ,\backslash boldsymbol.$$

The volume element is$$\backslash mathrmV\; =\; \backslash rho\backslash ,\backslash mathrm\backslash rho\backslash ,\backslash mathrm\backslash varphi\backslash ,\backslash mathrmz.$$

The surface element in a surface of constant radius (a vertical cylinder) is$$\backslash mathrmS\_\backslash rho\; =\; \backslash rho\backslash ,\backslash mathrm\backslash varphi\backslash ,\backslash mathrmz.$$

The surface element in a surface of constant azimuth (a vertical half-plane) is$$\backslash mathrmS\_\backslash varphi\; =\; \backslash mathrm\backslash rho\backslash ,\backslash mathrmz.$$

The surface element in a surface of constant height (a horizontal plane) is$$\backslash mathrmS\_z\; =\; \backslash rho\backslash ,\backslash mathrm\backslash rho\backslash ,\backslash mathrm\backslash varphi.$$

The del operator in this system leads to the following expressions for gradient, divergence, curl and Laplacian:

\nabla \cdot \boldsymbol &= \frac\frac\left(\rho A_\rho\right) + \frac \frac + \frac \\[8px]

\nabla \times \boldsymbol &= \left(\frac\frac - \frac\right)\boldsymbol + \left(\frac - \frac\right)\boldsymbol + \frac\left(\frac\left(\rho A_\varphi\right) - \frac\right) \boldsymbol \\[8px]

\nabla^2 f &= \frac \frac \left(\rho \frac\right) + \frac \frac + \frac\end

Cylindrical harmonics

The solutions to the Laplace equation in a system with cylindrical symmetry are called cylindrical harmonics.

Kinematics

In a cylindrical coordinate system, the position of a particle can be written as^[6] $$\backslash boldsymbol\; =\; \backslash rho\backslash ,\backslash boldsymbol\; +\; z\backslash ,\backslash boldsymbol.$$The velocity of the particle is the time derivative of its position,$$\backslash boldsymbol\; =\; \backslash frac\; =\; \backslash dot\backslash ,\backslash boldsymbol\; +\; \backslash rho\backslash ,\backslash dot\backslash varphi\backslash ,\backslash hat\; +\; \backslash dot\backslash ,\backslash hat,$$where the term

\rho • \varphi\hat\varphi comes from the Poisson formula (d\hat\rho)/(dt) = • \varphi\hat z x \hat\rho . Its acceleration is^[6] $$\backslash boldsymbol\; =\; \backslash frac\; =\; \backslash left(\backslash ddot\; -\; \backslash rho\backslash ,\backslash dot\backslash varphi^2\; \backslash right)\backslash boldsymbol\; +\; \backslash left(2\backslash dot\backslash ,\backslash dot\backslash varphi\; +\; \backslash rho\backslash ,\backslash ddot\backslash varphi\; \backslash right)\; \backslash hat\; +\; \backslash ddot\backslash ,\backslash hat$$

See also

• List of canonical coordinate transformations
• Vector fields in cylindrical and spherical coordinates
• Del in cylindrical and spherical coordinates

Further reading

• Book: Morse . Philip M. . Philip M. Morse . Feshbach . Herman . Herman Feshbach . 1953 . Methods of Theoretical Physics, Part I . . . 0-07-043316-X . 52011515 . 656–657.
• Book: Margenau . Henry . Henry Margenau . Murphy . George M. . 1956 . The Mathematics of Physics and Chemistry . registration . D. van Nostrand . New York City . 178 . 55010911 . 9780882754239 . 3017486.
• Book: Korn . Granino A. . Korn . Theresa M. . Theresa M. Korn . 1961 . Mathematical Handbook for Scientists and Engineers . registration . McGraw-Hill . New York City . ASIN B0000CKZX7 . 174–175 . 59014456.
• Book: Sauer . Robert . Szabó . István . 1967 . Mathematische Hilfsmittel des Ingenieurs . . New York City . 95 . 67025285.
• Book: Zwillinger, Daniel . 1992 . Handbook of Integration . . . 0-86720-293-9 . 113 . 25710023.
• Book: Moon . P. . Spencer . D. E. . 1988 . Circular-Cylinder Coordinates (r, ψ, z) . Field Theory Handbook, Including Coordinate Systems, Differential Equations, and Their Solutions . corrected 2nd . Springer-Verlag . New York City . 12–17, Table 1.02 . 978-0-387-18430-2.

External links

• • MathWorld description of cylindrical coordinates
• Cylindrical Coordinates Animations illustrating cylindrical coordinates by Frank Wattenberg

Notes and References

1. Krafft . C. . Volokitin . A. S. . Resonant electron beam interaction with several lower hybrid waves . Physics of Plasmas . 1 January 2002 . 9 . 6 . 2786–2797 . 10.1063/1.1465420 . 9 February 2013 . 1089-7674 . ...in cylindrical coordinates ... and is the longitudinal position... . 2002PhPl....9.2786K . https://archive.today/20130414005110/http://pop.aip.org/resource/1/phpaen/v9/i6/p2786_s1?isAuthorized=no . 14 April 2013 . dead .
2. Groisman . Alexander . Steinberg . Victor . 1997 . Solitary Vortex Pairs in Viscoelastic Couette Flow . Physical Review Letters . 78 . 8. 1460–1463 . 10.1103/PhysRevLett.78.1460 . 1997PhRvL..78.1460G . ...where,, and are cylindrical coordinates ... as a function of axial position.... patt-sol/9610008 . 54814721 .
3. Book: Szymanski, J. E. . Basic Mathematics for Electronic Engineers: models and applications . Tutorial Guides in Electronic Engineering (no. 16) . Taylor & Francis . 1989 . 978-0-278-00068-1 . 170.
4. Book: Nunn, Robert H.. Intermediate Fluid Mechanics . Taylor & Francis . 1989 . 978-0-89116-647-4 . 3.
5. Book: Linda Siobhan . Sparke . Linda Sparke. John Sill . Gallagher . Galaxies in the Universe: An Introduction . 2nd . Cambridge University Press . 2007 . 978-0-521-85593-8 . 37.
6. Book: Taylor . John R. . Classical Mechanics . 2005 . University Science Books . Sausalito, California . 29.