New views of the spherical Bouguer gravity anomaly

This paper presents a number of new concepts concerning the gravity anomaly. First, it identifies a distinct difference between a surface (2-D) gravity anomaly (the difference between actual gravity on one surface and normal gravity on another surface) and a solid (3-D) gravity anomaly defined in th...

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Main Authors: Vanicek, P., Tenzer, R., Sjoberg, L., Martinec, Z., Featherstone, Will
Format: Journal Article
Published: Blackwell 2004
Subjects:
Online Access:http://hdl.handle.net/20.500.11937/21625
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author Vanicek, P.
Tenzer, R.
Sjoberg, L.
Martinec, Z.
Featherstone, Will
author_facet Vanicek, P.
Tenzer, R.
Sjoberg, L.
Martinec, Z.
Featherstone, Will
author_sort Vanicek, P.
building Curtin Institutional Repository
collection Online Access
description This paper presents a number of new concepts concerning the gravity anomaly. First, it identifies a distinct difference between a surface (2-D) gravity anomaly (the difference between actual gravity on one surface and normal gravity on another surface) and a solid (3-D) gravity anomaly defined in the fundamental gravimetric equation. Second, it introduces the 'no topography' gravity anomaly (which turns out to be the complete spherical Bouguer anomaly) as a means to generate a quantity that is smooth, thus suitable for gridding, and harmonic, thus suitable for downward continuation. It is understood that the possibility of downward continuing a smooth gravity anomaly would simplify the task of computing an accurate geoid. It is also shown that the planar Bouguer anomaly is not harmonic, and thus cannot be downward continued.
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institution Curtin University Malaysia
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publishDate 2004
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spelling curtin-20.500.11937-216252017-09-13T16:00:44Z New views of the spherical Bouguer gravity anomaly Vanicek, P. Tenzer, R. Sjoberg, L. Martinec, Z. Featherstone, Will topography Bouguer correction gravity anomaly geoid This paper presents a number of new concepts concerning the gravity anomaly. First, it identifies a distinct difference between a surface (2-D) gravity anomaly (the difference between actual gravity on one surface and normal gravity on another surface) and a solid (3-D) gravity anomaly defined in the fundamental gravimetric equation. Second, it introduces the 'no topography' gravity anomaly (which turns out to be the complete spherical Bouguer anomaly) as a means to generate a quantity that is smooth, thus suitable for gridding, and harmonic, thus suitable for downward continuation. It is understood that the possibility of downward continuing a smooth gravity anomaly would simplify the task of computing an accurate geoid. It is also shown that the planar Bouguer anomaly is not harmonic, and thus cannot be downward continued. 2004 Journal Article http://hdl.handle.net/20.500.11937/21625 10.1111/j.1365-246X.2004.02435.x Blackwell fulltext
spellingShingle topography
Bouguer correction
gravity anomaly
geoid
Vanicek, P.
Tenzer, R.
Sjoberg, L.
Martinec, Z.
Featherstone, Will
New views of the spherical Bouguer gravity anomaly
title New views of the spherical Bouguer gravity anomaly
title_full New views of the spherical Bouguer gravity anomaly
title_fullStr New views of the spherical Bouguer gravity anomaly
title_full_unstemmed New views of the spherical Bouguer gravity anomaly
title_short New views of the spherical Bouguer gravity anomaly
title_sort new views of the spherical bouguer gravity anomaly
topic topography
Bouguer correction
gravity anomaly
geoid
url http://hdl.handle.net/20.500.11937/21625