2015
DOI: 10.1002/2014ja020565
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Inverse procedure for high‐latitude ionospheric electrodynamics: Analysis of satellite‐borne magnetometer data

Abstract: This paper presents an analysis of data from the magnetometers on board the Defense Meteorological Satellite Program (DMSP) F-15, F-16, F-17, and F-18 satellites and the Iridium satellite constellation, using an inverse procedure for high-latitude ionospheric electrodynamics, during the period of 29-30 May 2010. The Iridium magnetometer data are made available through the Active Magnetosphere and Planetary Electrodynamics Response Experiment (AMPERE) program. The method presented here is built upon the assimil… Show more

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Cited by 23 publications
(45 citation statements)
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“…In the high‐latitude region, we assume FACs are in the radial direction and produce mostly toroidal magnetic perturbation at the altitude of Iridium satellites. The toroidal and poloidal decomposition of the magnetic field can be simplified under this assumption following Matsuo et al () to δtrueBδBtrue→tor=×truekΨ where δtrueB is the magnetic field vector, Ψ is the toroidal magnetic potential, and truek is a unit vector pointing upward. FAC J can then be calculated from magnetic field vectors following Ampere's law assuming an electrostatic condition as J=ktrue→μ0·×δtrueB=1μ0hor2Ψ …”
Section: Methodsmentioning
confidence: 99%
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“…In the high‐latitude region, we assume FACs are in the radial direction and produce mostly toroidal magnetic perturbation at the altitude of Iridium satellites. The toroidal and poloidal decomposition of the magnetic field can be simplified under this assumption following Matsuo et al () to δtrueBδBtrue→tor=×truekΨ where δtrueB is the magnetic field vector, Ψ is the toroidal magnetic potential, and truek is a unit vector pointing upward. FAC J can then be calculated from magnetic field vectors following Ampere's law assuming an electrostatic condition as J=ktrue→μ0·×δtrueB=1μ0hor2Ψ …”
Section: Methodsmentioning
confidence: 99%
“…The magnetic perturbation data y can be related to the coefficient vector x as boldy=boldHx+boldϵ where y is a column vector containing all δtrueB)(,,tjϕiλi at location i and time j ; H is a matrix containing 244 basis functions ×truekboldΨ evaluated at the observation locations, and ϵ accounts for observational and truncation errors (Matsuo et al, ). H represents a linear relationship between x and y in this case and can be computed following Richmond et al (1995) as δBd1tor=truek·][d1×e1RrcosλmΨϕmd2×e1RrsinImΨλm δBd2tor=truek·][d1×e2RrcosλmΨϕmd2×e2RrsinImΨλm where λ m and ϕ m are latitude and longitude; d1 and d…”
Section: Methodsmentioning
confidence: 99%
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“…Using AMPERE data, the Assimilative Mapping of Ionospheric Electrodynamics has been applied to a number of geomagnetic storms [cf. Matsuo et al, 2015]. Wilder et al [2012] obtained dramatic differences in ionospheric Joule heating rates and distributions relative to assimilations using only ground magnetometer, radar, and operational low Earth orbit satellite observations.…”
Section: Introductionmentioning
confidence: 99%
“…Using AMPERE data, the Assimilative Mapping of Ionospheric Electrodynamics has been applied to a number of geomagnetic storms [cf. Matsuo et al ., ]. Wilder et al .…”
Section: Introductionmentioning
confidence: 99%