Steady Induction Effects in Geomagnetism. Part 1B: Geomagnetic Estimation of Steady Surficial Core Motions: A Non-linear Inverse Problem

Steady Induction Effects in Geomagnetism. Part 1B: Geomagnetic Estimation of Steady Surficial Core Motions: A Non-linear Inverse Problem PDF Author:
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Languages : en
Pages : 32

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Steady Induction Effects in Geomagnetism. Part 1C: Geomagnetic Estimation of Steady Surficial Core Motions: Application to the Definitive Geomagnetic Reference Field Models

Steady Induction Effects in Geomagnetism. Part 1C: Geomagnetic Estimation of Steady Surficial Core Motions: Application to the Definitive Geomagnetic Reference Field Models PDF Author:
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Category :
Languages : en
Pages : 36

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Scientific and Technical Aerospace Reports

Scientific and Technical Aerospace Reports PDF Author:
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Category : Aeronautics
Languages : en
Pages : 1038

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Steady Induction Effects in Geomagnetism. Part 1A: Steady Motional Induction of Geomagnetic Chaos

Steady Induction Effects in Geomagnetism. Part 1A: Steady Motional Induction of Geomagnetic Chaos PDF Author:
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Category :
Languages : en
Pages : 36

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Steady Induction Effects in Geomagnetism. Part 1b

Steady Induction Effects in Geomagnetism. Part 1b PDF Author: National Aeronautics and Space Administration (NASA)
Publisher: Createspace Independent Publishing Platform
ISBN: 9781722802325
Category :
Languages : en
Pages : 30

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The problem of estimating a steady fluid velocity field near the top of Earth's core which induces the secular variation (SV) indicated by models of the observed geomagnetic field is examined in the source-free mantle/frozen-flux core (SFI/VFFC) approximation. This inverse problem is non-linear because solutions of the forward problem are deterministically chaotic. The SFM/FFC approximation is inexact, and neither the models nor the observations they represent are either complete or perfect. A method is developed for solving the non-linear inverse motional induction problem posed by the hypothesis of (piecewise, statistically) steady core surface flow and the supposition of a complete initial geomagnetic condition. The method features iterative solution of the weighted, linearized least-squares problem and admits optional biases favoring surficially geostrophic flow and/or spatially simple flow. Two types of weights are advanced radial field weights for fitting the evolution of the broad-scale portion of the radial field component near Earth's surface implied by the models, and generalized weights for fitting the evolution of the broad-scale portion of the scalar potential specified by the models. Voorhies, Coerte V. Goddard Space Flight Center RTOP 676-40-02; RTOP 579-31-07...

Monthly Catalog of United States Government Publications

Monthly Catalog of United States Government Publications PDF Author:
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Category : Government publications
Languages : en
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Monthly Catalogue, United States Public Documents

Monthly Catalogue, United States Public Documents PDF Author:
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Category : Government publications
Languages : en
Pages : 808

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Government Reports Annual Index

Government Reports Annual Index PDF Author:
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Category : Government reports announcements & index
Languages : en
Pages : 1832

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Government Reports Announcements & Index

Government Reports Announcements & Index PDF Author:
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Category : Science
Languages : en
Pages : 744

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Steady Induction Effects in Geomagnetism. Part 1c

Steady Induction Effects in Geomagnetism. Part 1c PDF Author: National Aeronautics and Space Administration (NASA)
Publisher: Createspace Independent Publishing Platform
ISBN: 9781722802479
Category :
Languages : en
Pages : 30

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In the source-free mantle/frozen-flux core magnetic earth model, the non-linear inverse steady motional induction problem was solved using the method presented in Part 1B. How that method was applied to estimate steady, broad-scale fluid velocity fields near the top of Earth's core that induce the secular change indicated by the Definitive Geomagnetic Reference Field (DGRF) models from 1945 to 1980 are described. Special attention is given to the derivation of weight matrices for the DGRF models because the weights determine the apparent significance of the residual secular change. The derived weight matrices also enable estimation of the secular change signal-to-noise ratio characterizing the DGRF models. Two types of weights were derived in 1987-88: radial field weights for fitting the evolution of the broad-scale portion of the radial geomagnetic field component at Earth's surface implied by the DGRF's, and general weights for fitting the evolution of the broad-scale portion of the scalar potential specified by these models. The difference is non-trivial because not all the geomagnetic data represented by the DGRF's constrain the radial field component. For radial field weights (or general weights), a quantitatively acceptable explication of broad-scale secular change relative to the 1980 Magsat epoch must account for 99.94271 percent (or 99.98784 percent) of the total weighted variance accumulated therein. Tolerable normalized root-mean-square weighted residuals of 2.394 percent (or 1.103 percent) are less than the 7 percent errors expected in the source-free mantle/frozen-flux core approximation. Voorhies, Coerte V. Goddard Space Flight Center ...