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The International Geomagnetic Reference Field (IGRF) is a standard mathematical description of the large-scale structure of the Earth's main magnetic field and its secular variation. It was created by fitting parameters of a mathematical model of the magnetic field to measured magnetic field data from surveys, observatories and satellites across the globe. The IGRF has been produced and updated under the direction of the International Association of Geomagnetism and Aeronomy (IAGA) since 1965. The IGRF model covers a significant time span, and so is useful for interpreting historical data. (This is unlike the World Magnetic Model, which is intended for navigation in the next few years.) It is updated at 5-year intervals, reflecting the most accurate measurements available at that time. The current 13th edition of the IGRF model (IGRF-13) was released in December 2019 and is valid from 1900 until 2025. For the interval from 1945 to 2015, it is "definitive" (a "DGRF"), meaning that future updates are unlikely to improve the model in any significant way.


Spherical Harmonics

The IGRF models the geomagnetic field \vec(r,\phi,\theta, t) as a gradient of a
magnetic scalar potential Magnetic scalar potential, ''ψ'', is a quantity in classical electromagnetism analogous to electric potential. It is used to specify the magnetic H-field in cases when there are no free currents, in a manner analogous to using the electric ...
V(r,\phi,\theta, t) : \vec(r,\phi,\theta, t) = -\nabla V(r,\phi,\theta, t) = -\left(\dfrac, \dfrac 1r\dfrac, \dfrac 1\dfrac\right) The magnetic scalar potential model consists of the Gauss coefficients which define a
spherical harmonic In mathematics and physical science, spherical harmonics are special functions defined on the surface of a sphere. They are often employed in solving partial differential equations in many scientific fields. Since the spherical harmonics for ...
expansion of V : V(r,\phi,\theta, t) = a \sum_^L\sum_^\ell \left(\frac\right)^ \left(g_\ell^m(t)\cos m\phi + h_\ell^m(t)\sin m\phi\right) P_\ell^m\left(\cos\theta\right) where r is radial distance from the Earth's center, L is the maximum degree of the expansion, \phi is East longitude, \theta is colatitude (the polar angle), a is the Earth's radius, g_\ell^m and h_\ell^m are Gauss coefficients, and P_\ell^m\left(\cos\theta\right) are the Schmidt normalized
associated Legendre function In mathematics, the associated Legendre polynomials are the canonical solutions of the general Legendre equation \left(1 - x^2\right) \frac P_\ell^m(x) - 2 x \frac P_\ell^m(x) + \left \ell (\ell + 1) - \frac \rightP_\ell^m(x) = 0, or equivalently ...
s of degree l and order m : P_n^(\cos\theta) = (-1)^m (\sin \theta)^\ \fracP_n(\cos\theta) where : P_n(\cos\theta) = \frac\left frac\left((\cos\theta)^2-1\right)^n\right The Gauss coefficients are modeled as a piecewise-linear function of time with a 5 year step size.


See also

* World Magnetic Model * Geomagnetic latitude *
Magsat Magsat (Magnetic field Satellite, Applications Explorer Mission-C or AEM-C or Explorer 61) was a NASA/USGS (United States Geological Survey) spacecraft, launched on 30 October 1979. The mission was to map the Earth's magnetic field, the satelli ...
* Ørsted (satellite) * CHAMP (satellite)


References


External links


IGRF Model Description by IAGA


{{Geophysics-stub Geomagnetism Magnetic field of the Earth