Math 2.0

Geophysics Gravity field of the Earth Proposition

Bruns formula

Builds on GeopotentialGeoidReference ellipsoid

Statement

Let WW be the geopotential of the Earth and let the geoid be the level surface W=W0W = W_0. Let UU be the normal potential of a reference ellipsoid, chosen so that U=W0U = W_0 on the ellipsoid. Let γ\gamma be the magnitude of normal gravity on the ellipsoid. Let T=W−UT = W - U be the disturbing potential. Let PP be a point of the geoid, and let QQ be the point of the ellipsoid on the ellipsoidal normal through PP. Let NN be the geoid height, the signed distance from QQ to PP. Then, to first order in NN, N=T(P)γ(Q).N = \frac{T(P)}{\gamma(Q)}.

Remarks

The proof is a one-term Taylor expansion of UU along the ellipsoidal normal. Normal gravity points inward along this normal, so U(P)≈U(Q)−γ(Q)N=W0−γ(Q)NU(P) \approx U(Q) - \gamma(Q) N = W_0 - \gamma(Q) N. Since W(P)=W0W(P) = W_0, this gives T(P)=W(P)−U(P)≈γ(Q)NT(P) = W(P) - U(P) \approx \gamma(Q) N. The neglected terms are of order N2N^2 times the second derivative of UU, which is negligible because NN is at most about 100100 m. Example: a disturbing potential T(P)=98 m2/s2T(P) = 98\ \mathrm{m^2/s^2} with γ≈9.8 m/s2\gamma \approx 9.8\ \mathrm{m/s^2} gives a geoid height of 1010 m.

Going deeper

For a student

Bruns formula turns the geoid problem into a problem about the harmonic function TT. Combined with the boundary condition ∂T/∂r+2T/R=−Δg\partial T/\partial r + 2T/R = -\Delta g for the gravity anomaly, it leads to the geodetic boundary value problem and to Stokes' formula. It is also used in reverse, to turn a global spherical harmonic model of TT into geoid heights.

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  1. Geoid concept
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Where this leads

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Further reading

  1. Web https://en.wikipedia.org/wiki/Physical_geodesy
About this page
Tag8GF20Z4KDC
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Kindstatement, proposition
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MSC86A30
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AboutGeoid
UsesGeopotential, Geoid, Reference ellipsoid
Changed3 November 2026

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