List of equations in gravitation


This article summarizes equations in the theory of gravitation.

Definitions

Gravitational mass and inertia

A common misconception occurs between centre of mass and centre of gravity. They are defined in similar ways but are not exactly the same quantity. Centre of mass is the mathematical description of placing all the mass in the region considered to one position, centre of gravity is a real physical quantity, the point of a body where the gravitational force acts. They are equal if and only if the external gravitational field is uniform.
Quantity symbol/sDefining equationSI unitsDimension
Centre of gravityrcog ith moment of mass
Centre of gravity for a set of discrete masses:

Centre of gravity for a continuum of mass:
m
Standard gravitational parameter of a massμN m2 kg−13 −2

Newtonian gravitation

Quantity symbol/sDefining equationSI unitsDimension
Gravitational field, field strength, potential gradient, accelerationgN kg−1 = m s−2−2
Gravitational fluxΦGm3 s−23−2
Absolute gravitational potentialΦ, φ, U, VJ kg−12−2
Gravitational potential differenceΔΦ, Δφ, ΔU, ΔVJ kg−12−2
Gravitational potential energyEpJ2−2
Gravitational torsion fieldΩHz = s−1−1

Gravitoelectromagnetism

In the weak-field and slow motion limit of general relativity, the phenomenon of gravitoelectromagnetism occurs, creating a parallel between gravitation and electromagnetism. The gravitational field is the analogue of the electric field, while the gravitomagnetic field, which results from circulations of masses due to their angular momentum, is the analogue of the magnetic field.
Quantity symbol/sDefining equationSI unitsDimension
Gravitational torsion fluxΦΩN m s kg−1 = m2 s−12 −1
Gravitomagnetic fieldH, Bg, B, ξHz = s−1−1
Gravitomagnetic fluxΦξN m s kg−1 = m2 s−12 −1
Gravitomagnetic vector potentialhm s−1 −1

Equations

Newtonian gravitational fields

It can be shown that a uniform spherically symmetric mass distribution generates an equivalent gravitational field to a point mass, so all formulae for point masses apply to bodies which can be modelled in this way.
Physical situationNomenclatureEquations
Gravitational potential gradient and field
Point mass
At a point in a local array of point masses
Gravitational torque and potential energy due to non-uniform fields and mass moments
  • V = volume of space occupied by the mass distribution
  • m = mr is the mass moment of a massive particle
Gravitational field for a rotating body
  • = zenith angle relative to rotation axis
  • = unit vector perpendicular to rotation axis, radial from it

Gravitational potentials

General classical equations.
Physical situationNomenclatureEquations
Potential energy from gravity, integral from Newton's law
Escape speed
  • M = Mass of body to escape from
  • r = radius of body
Orbital energy

Weak-field relativistic equations

Physical situationNomenclatureEquations
Gravitomagnetic field for a rotating bodyξ = gravitomagnetic field