Geopotential spherical harmonic model explained

In geophysics and physical geodesy, a geopotential model is the theoretical analysis of measuring and calculating the effects of Earth's gravitational field (the geopotential).The Earth is not exactly spherical, mainly because of its rotation around the polar axis that makes its shape slightly oblate. However, a spherical harmonics series expansion captures the actual field with increasing fidelity.

If Earth's shape were perfectly known together with the exact mass density ρ = ρ(x, y, z), it could be integrated numerically (when combined with a reciprocal distance kernel) to find an accurate model for Earth's gravitational field. However, the situation is in fact the opposite: by observing the orbits of spacecraft and the Moon, Earth's gravitational field can be determined quite accurately. The best estimate of Earth's mass is obtained by dividing the product GM as determined from the analysis of spacecraft orbit with a value for the gravitational constant G, determined to a lower relative accuracy using other physical methods.

Background

See main article: Spherical harmonics. From the defining equations and it is clear (taking the partial derivatives of the integrand) that outside the body in empty space the following differential equations are valid for the field caused by the body:

Functions of the form

\phi = R(r) \Theta(\theta) \Phi(\varphi) where (r, θ, φ) are the spherical coordinates which satisfy the partial differential equation (the Laplace equation) are called spherical harmonic functions.

They take the forms:

where spherical coordinates (r, θ, φ) are used, given here in terms of cartesian (x, y, z) for reference:

also P⁰_n are the Legendre polynomials and P^m_n for are the associated Legendre functions.

The first spherical harmonics with n = 0, 1, 2, 3 are presented in the table below. [Note that the sign convention differs from the one in the page about the associated Legendre polynomials, here <math>P_2^1(x)=3x\sqrt{1-x^2}</math> whereas there <math>P_2^1(x)=-3x\sqrt{1-x^2}</math>.]

n	Spherical harmonics
0	(1)/(r)
1	(1)/(r ^{2}) P ^{0} _{1 (\sin\theta)} = (1)/(r ^{2}) \sin\theta
	(1)/(r ^{2}) P ^{1} _{1 (\sin\theta)} \cos\varphi = (1)/(r ^{2}) \cos\theta \cos\varphi
	(1)/(r ^{2}) P ^{1} _{1 (\sin\theta)} \sin\varphi = (1)/(r ^{2}) \cos\theta \sin\varphi
2	(1)/(r ^{3}) P ^{0} _{2 (\sin\theta)} = (1)/(r ^{3}) (1)/(2) ( 3 \sin ^{2\theta} - 1 )
	(1)/(r ^{3}) P ^{1} _{2 (\sin\theta)} \cos\varphi = (1)/(r ^{3}) 3 \sin\theta \cos\theta \cos\varphi
	(1)/(r ^{3}) P ^{1} _{2 (\sin\theta)} \sin\varphi = (1)/(r ^{3}) 3 \sin\theta \cos\theta \sin\varphi
	(1)/(r ^{3}) P ^{2} _{2 (\sin\theta)} \cos 2 \varphi = (1)/(r ^{3}) 3 \cos ^{2} \theta \cos 2 \varphi
	(1)/(r ^{3}) P ^{2} _{2 (\sin\theta)} \sin 2 \varphi = (1)/(r ^{3}) 3 \cos ^{2} \theta \sin 2 \varphi
3	(1)/(r ^{4}) P ^{0} _{3 (\sin\theta)} = (1)/(r ^{4}) (1)/(2) \sin\theta ( 5 \sin ^{2\theta} -3 )
	(1)/(r ^{4}) P ^{1} _{3 (\sin\theta)} \cos\varphi = (1)/(r ^{4}) (3)/(2) ( 5 \sin ^{2\theta} - 1 ) \cos\theta \cos\varphi
	(1)/(r ^{4}) P ^{1} _{3 (\sin\theta)} \sin\varphi = (1)/(r ^{4}) (3)/(2) ( 5 \sin ^{2\theta} - 1 ) \cos\theta \sin\varphi
	(1)/(r ^{4}) P ^{2} _{3 (\sin\theta)} \cos 2 \varphi = (1)/(r ^{4}) 15 \sin\theta \cos ^{2} \theta \cos 2 \varphi
	(1)/(r ^{4}) P ^{2} _{3 (\sin\theta)} \sin 2 \varphi = (1)/(r ^{4}) 15 \sin\theta \cos ^{2} \theta \sin 2 \varphi
	(1)/(r ^{4}) P ^{3} _{3 (\sin\theta)} \cos 3 \varphi = (1)/(r ^{4}) 15 \cos ^{3} \theta \cos 3 \varphi
	(1)/(r ^{4}) P ^{3} _{3 (\sin\theta)} \sin 3 \varphi = (1)/(r ^{4}) 15 \cos ^{3} \theta \sin 3 \varphi

Formulation

The model for Earth's gravitational potential is a sum

where

\mu = GM and the coordinates are relative to the standard geodetic reference system extended into space with origin in the center of the reference ellipsoid and with z-axis in the direction of the polar axis.

The zonal terms refer to terms of the form:

(P ^{0} _{n(\sin\theta)})/(r ^{n+1}) n =0 , 1 , 2 , ...

and the tesseral terms terms refer to terms of the form:

(P ^{m} _{n(\sin\theta)} \cos m\varphi)/(r ^{n+1}) , 1 \le m \le n n =1 , 2 , ... (P ^{m} _{n(\sin\theta)} \sin m\varphi)/(r ^{n+1})

The zonal and tesseral terms for n = 1 are left out in . The coefficients for the n=1 with both m=0 and m=1 term correspond to an arbitrarily oriented dipole term in the multi-pole expansion. Gravity does not physically exhibit any dipole character and so the integral characterizing n = 1 must be zero.

The different coefficients J_n, C_n^m, S_n^m, are then given the values for which the best possible agreement between the computed and the observed spacecraft orbits is obtained.

As P⁰_n(x) = −P⁰_n(−x) non-zero coefficients J_n for odd n correspond to a lack of symmetry "north–south" relative the equatorial plane for the mass distribution of Earth. Non-zero coefficients C_n^m, S_n^m correspond to a lack of rotational symmetry around the polar axis for the mass distribution of Earth, i.e. to a "tri-axiality" of Earth.

For large values of n the coefficients above (that are divided by r^{(n + 1)} in) take very large values when for example kilometers and seconds are used as units. In the literature it is common to introduce some arbitrary "reference radius" R close to Earth's radius and to work with the dimensionless coefficients

\begin{align} \tilde{J _{n}} & =- (J _{n})/(\mu R ^{n}) , & \tilde{C ^{m}} _{n} & =- (C ^{m} _{n})/(\mu R ^{n}) , & \tilde{S ^{m}} _{n} & =- (S ^{m} _{n})/(\mu R ^{n}) \end{align}

and to write the potential as

Derivation

The spherical harmonics are derived from the approach of looking for harmonic functions of the form

where (r, θ, φ) are the spherical coordinates defined by the equations . By straightforward calculations one gets that for any function f

Introducing the expression in one gets that

As the term

(1)/(R) (d)/(dr) \left(r ^{2 (dR)/(dr)} \right) only depends on the variable r and the sum(1)/(\Theta\cos\theta) (d)/(d\theta) \left(\cos\theta (d\Theta)/(d\theta) \right) + (1)/(\Phi\cos ^{2\theta}) (d ^{2\Phi})/(d\varphi ^{2})

only depends on the variables θ and φ. One gets that φ is harmonic if and only if

and

for some constant

λ .

From then follows that

(1)/(\cos\theta \Theta) (d)/(d\theta) \left(\cos\theta (d\Theta)/(d\theta) \right) + λ \cos ^{2 \theta + (1)/(\Phi)} (d ^{2\Phi})/(d\varphi ^{2}) = 0

The first two terms only depend on the variable

\theta and the third only on the variable \varphi .

From the definition of φ as a spherical coordinate it is clear that Φ(φ) must be periodic with the period 2π and one must therefore have that

and

for some integer m as the family of solutions to then are

With the variable substitution

x = \sin \theta

equation takes the form

From follows that in order to have a solution

\phi withR(r) = (1)/(r ^{n+1})

one must have that

λ = n (n + 1 )

If P_n(x) is a solution to the differential equation

one therefore has that the potential corresponding to m = 0

\phi = (1)/(r ^{n+1}) P _{n(\sin\theta)}

which is rotationally symmetric around the z-axis is a harmonic function

If

P ^{m} _{n} (x) is a solution to the differential equation

with m ≥ 1 one has the potential

where a and b are arbitrary constants is a harmonic function that depends on φ and therefore is not rotationally symmetric around the z-axis

The differential equation is the Legendre differential equation for which the Legendre polynomials defined

are the solutions.

The arbitrary factor 1/(2ⁿn!) is selected to make and for odd n and for even n.

The first six Legendre polynomials are:

The solutions to differential equation are the associated Legendre functions

One therefore has that

P ^{m} _{n} (\sin\theta) = \cos ^{m} \theta (d ^{n} P _{n})/(dx ^{n}) (\sin\theta)

Largest terms

The dominating term (after the term −μ/r) in is the J₂ coefficient, the second dynamic form factor representing the oblateness of Earth:

u = (J ^{0} _{2 (\sin\theta)})/(r ^{3}) = J _{2} (1)/(r ^{3}) (1)/(2) ( 3 \sin ^{2\theta} -1 ) = J _{2} (1)/(r ^{5}) (1)/(2) ( 3 z ^{2} - r ^{2)}

Relative the coordinate system

illustrated in figure 1 the components of the force caused by the "J₂ term" are

In the rectangular coordinate system (x, y, z) with unit vectors (x̂ ŷ ẑ) the force components are:

The components of the force corresponding to the "J₃ term"

u = (J _{3} P ^{0} _{3 (\sin\theta)})/(r ^{4}) = J _{3} (1)/(r ^{4}) (1)/(2) \sin\theta \left( 5 \sin ^{2\theta} - 3 \right) = J _{3} (1)/(r ^{7}) (1)/(2) z \left( 5 z ^{2} - 3 r ^{2\right)}

are

and

The exact numerical values for the coefficients deviate (somewhat) between different Earth models but for the lowest coefficients they all agree almost exactly.

For the JGM-3 model (see below) the values are:

μ = 398600.440 km³⋅s⁻²

J₂ = 1.75553 × 10¹⁰ km⁵⋅s⁻²

J₃ = −2.61913 × 10¹¹ km⁶⋅s⁻²

For example, at a radius of 6600 km (about 200 km above Earth's surface) J₃/(J₂r) is about 0.002; i.e., the correction to the "J₂ force" from the "J₃ term" is in the order of 2 permille. The negative value of J₃ implies that for a point mass in Earth's equatorial plane the gravitational force is tilted slightly towards the south due to the lack of symmetry for the mass distribution of Earth's "north–south".

Recursive algorithms used for the numerical propagation of spacecraft orbits

Spacecraft orbits are computed by the numerical integration of the equation of motion. For this the gravitational force, i.e. the gradient of the potential, must be computed. Efficient recursive algorithms have been designed to compute the gravitational force for any

N _{z} and N _{t} (the max degree of zonal and tesseral terms) and such algorithms are used in standard orbit propagation software.

Available models

The earliest Earth models in general use by NASA and ESRO/ESA were the "Goddard Earth Models" developed by Goddard Space Flight Center (GSFC) denoted "GEM-1", "GEM-2", "GEM-3", and so on. Later the "Joint Earth Gravity Models" denoted "JGM-1", "JGM-2", "JGM-3" developed by GSFC in cooperation with universities and private companies became available. The newer models generally provided higher order terms than their precursors. The EGM96 uses N_z = N_t = 360 resulting in 130317 coefficients. An EGM2008 model is available as well.

For a normal Earth satellite requiring an orbit determination/prediction accuracy of a few meters the "JGM-3" truncated to N_z = N_t = 36 (1365 coefficients) is usually sufficient. Inaccuracies from the modeling of the air-drag and to a lesser extent the solar radiation pressure will exceed the inaccuracies caused by the gravitation modeling errors.

The dimensionless coefficients

\tilde{J _{n}} =- (J _{n})/(\mu R ^{n}) , \tilde{C ^{m}} _{n} =- (C ^{m} _{n})/(\mu R ^{n}) , \tilde{S ^{m}} _{n} =- (S ^{m} _{n})/(\mu R ^{n}) for the first zonal and tesseral terms (using R = and \mu =) of the JGM-3 model are

According to JGM-3 one therefore has that J = × 6378.1363 × = andJ = × 6378.1363 × = .

See also

• Geoid#Spherical harmonics representation

References

Further reading

• El'Yasberg Theory of flight of artificial earth satellites, Israel program for Scientific Translations (1967)
• Lerch, F.J., Wagner, C.A., Smith, D.E., Sandson, M.L., Brownd, J.E., Richardson, J.A.,"Gravitational Field Models for the Earth (GEM1&2)", Report X55372146, Goddard Space Flight Center, Greenbelt/Maryland, 1972
• Lerch, F.J., Wagner, C.A., Putney, M.L., Sandson, M.L., Brownd, J.E., Richardson, J.A., Taylor, W.A., "Gravitational Field Models GEM3 and 4", Report X59272476, Goddard Space Flight Center, Greenbelt/Maryland, 1972
• Lerch, F.J., Wagner, C.A., Richardson, J.A., Brownd, J.E., "Goddard Earth Models (5 and 6)", Report X92174145, Goddard Space Flight Center, Greenbelt/Maryland, 1974
• Lerch, F.J., Wagner, C.A., Klosko, S.M., Belott, R.P., Laubscher, R.E., Raylor, W.A., "Gravity Model Improvement Using Geos3 Altimetry (GEM10A and 10B)", 1978 Spring Annual Meeting of the American Geophysical Union, Miami, 1978
• Lerch. F.J.. Klosko. S.M.. Laubscher. R.E.. Wagner . C.A.. Gravity Model Improvement Using Geos3 (GEM9 and 10). Journal of Geophysical Research. 84. B8. 3897-3916. 1979. 10.1029/JB084i/B08p03897.
• Lerch. F.J.. Putney. B.H.. Wagner. C.A.. Klosko. S.M.. Goddard earth models for oceanographic applications (GEM 10B and 10C). Marine-Geodesy. 5. 2. 145-187. 1981. 10.1080/15210608109379416.
• Lerch, F.J., Klosko, S.M., Patel, G.B., "A Refined Gravity Model from Lageos (GEML2)", 'NASA Technical Memorandum 84986, Goddard Space Flight Center, Greenbelt/Maryland, 1983
• Lerch, F.J., Nerem, R.S., Putney, B.H., Felsentreger, T.L., Sanchez, B.V., Klosko, S.M., Patel, G.B., Williamson, R.G., Chinn, D.S., Chan, J.C., Rachlin, K.E., Chandler, N.L., McCarthy, J.J., Marshall, J.A., Luthcke, S.B., Pavlis, D.W., Robbins, J.W., Kapoor, S., Pavlis, E.C., " Geopotential Models of the Earth from Satellite Tracking, Altimeter and Surface Gravity Observations: GEMT3 and GEMT3S", NASA Technical Memorandum 104555, Goddard Space Flight Center, Greenbelt/Maryland, 1992
• Lerch. F.J.. Nerem. R.S.. Putney. B.H.. Felsentreger . T.L.. Sanchez. B.V.. Marshall. J.A.. Klosko. S.M.. Patel. G.B.. Williamson. R.G.. A Geopotential Model from Satellite Tracking, Altimeter and Surface Gravity Data: GEMT3. Journal of Geophysical Research. 99. B2. 2815-2839. 1994. 10.1029/93JB02759.
• Nerem. R.S.. Lerch. F.J.. Marshall. J.A.. Pavlis. E.C.. Putney. B.H.. Gravity Model Developments for Topex/Poseidon: Joint Gravity Models 1 and 2. Journal of Geophysical Research. 99. C12. 24421-24447. 1994. 10.1029/94JC01376.
• Tapley. B. D.. M. M.. Watkins. J. C.. Ries. G. W.. Davis. R. J.. Eanes. The Joint Gravity Model 3. J. Geophys. Res.. 101. B12. 1996. 10.1029/96JB01645.

External links

• http://cddis.nasa.gov/lw13/docs/papers/sci_lemoine_1m.pdf
• http://geodesy.geology.ohio-state.edu/course/refpapers/Tapley_JGR_JGM3_96.pdf