quantity

radial coordinate

radial coordinate — from formula anatomy
7 related articles · 6 formulas

Description

The radial coordinate is a spatial variable that measures distance from a chosen origin or axis in a coordinate system. In spherical coordinates, it is typically denoted r and ranges from 0 to infinity, while in cylindrical coordinates it is often ρ (or r) and measures perpendicular distance from a central axis. It is fundamental in describing systems with spherical or cylindrical symmetry, such as planetary orbits, atomic orbitals, and electromagnetic fields around point charges.

History

Radial coordinates have been used since ancient Greek astronomy, but their formal mathematical treatment in physics was developed by Leonhard Euler and others in the 18th century, particularly in the context of celestial mechanics and potential theory.

How it works

In a radial coordinate system, position is specified by the radial distance plus angular coordinates (e.g., θ and φ in spherical, z in cylindrical). The radial coordinate appears in the Laplacian operator, which governs many physical equations, and in radial distribution functions that describe how properties vary with distance from a center. For central forces, the radial coordinate often separates from angular variables in the Schrödinger equation, leading to radial wavefunctions.

In practice

Radial coordinates are essential in quantum mechanics for describing hydrogen-like atoms, in astrophysics for modeling stellar structure, and in engineering for analyzing stress in cylindrical or spherical vessels.

Fun fact

In general relativity, the radial coordinate does not always correspond to physical distance; for a Schwarzschild black hole, the radial coordinate r has a horizon at r = 2GM/c², where the coordinate becomes singular even though the curvature is finite.

Concept graph →

Formulas

$$ds^2 = -e^{2\rho} dt^2 + e^{2\lambda} dr^2 + r^2 d\Omega^2$$
Metric for spherically symmetric spacetime in general coordinates.
What is in the formula
ds^2variablespacetime interval — spacetime interval metre squared
dtvariablecoordinate time differential — time differential second
drvariableradial coordinate differential — radial coordinate differential metre
dΩ^2variablesolid angle element squared — solid angle element squared
ρvariablemetric function of r and t — metric function
λvariablemetric function of r and t — metric function
rvariableradial coordinate — radial coordinate metre
$$\partial_v r = 0$$
Condition defining a black hole horizon in null coordinates.
What is in the formula
vvariablenull coordinate (e.g., advanced time) — null coordinate metre
rvariableradial coordinate — radial coordinate metre
∂_voperatordifferentiates with respect to the null coordinate — partial derivative
$$ds^2 = -e^{2\Phi(r)} dt^2 + \left(1 - \frac{b(r)}{r}\right)^{-1} dr^2 + r^2 d\Omega^2$$
A static wormhole metric with shape function b(r) and redshift function Φ(r).
What is in the formula
ds^2variableSpacetime interval squared — spacetime interval metre squared
\Phi(r)variableRedshift function — redshift function
b(r)variableShape function — shape function metre
rvariableRadial coordinate — radial coordinate metre
tvariableTime coordinate — time coordinate second
d\Omega^2variableSolid angle element squared — solid angle element
doperatorExterior derivative — differential operator
$$\frac{d^2 r}{dz^2} = \frac{b - r b'}{2b^2} > 0$$
Geometric condition for wormhole throat existence violating null energy condition.
What is in the formula
rvariableradial coordinate of the throat — radial coordinate metre
zvariableproper distance along the throat — proper distance metre
bvariableshape function of the wormhole — shape function metre
d/dzoperatorderivative with respect to proper distance — ordinary derivative
d/droperatorderivative with respect to radial coordinate — ordinary derivative
$$ds^2 = -\left(1 - \frac{2GM}{c^2 r}\right) c^2 dt^2 + \left(1 - \frac{2GM}{c^2 r}\right)^{-1} dr^2 + r^2 d\Omega^2$$
Describes spacetime around a spherically symmetric mass.
What is in the formula
ds^2variablespacetime interval — spacetime interval metre squared
dtvariablecoordinate time differential — time differential second
drvariableradial coordinate differential — radial coordinate differential metre
dΩ^2variablesolid angle element squared — solid angle element squared
rvariableradial coordinate — radial coordinate metre
tvariablecoordinate time — coordinate time second
GconstantNewton's constant of universal gravitation — gravitational constant = 6.67430e-11 cubic metre per kilogram per second squared
cconstantspeed of light in vacuum — speed of light = 299792458 metre per second
Mconstantmass of the central object — mass kilogram
doperatorinfinitesimal change — differential
$$\Delta(r) = r^2 - 2Mr + a^2$$
Horizon function for Kerr black holes with mass M and spin a.
What is in the formula
\Delta(r)variableHorizon function of the Kerr metric — horizon function square metre
rvariableRadial coordinate (Boyer-Lindquist) — radial coordinate metre
MvariableBlack hole mass — mass kilogram
avariableSpecific angular momentum (spin parameter) — specific angular momentum metre

Related articles · 7

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