Misalignment and Resonance Torques and Their Treatment in the GP-B Data Analysis
Abstract Classical torques acting on the GP-B gyroscopes decrease the accuracy in the measurement of the relativistic drift rate. Based on measurements made during the year-long science data collection, tests done following the science data collection, and a theoretical analysis of potential torques...
Ausführliche Beschreibung
Autor*in: |
Keiser, G. M. [verfasserIn] |
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Format: |
Artikel |
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Sprache: |
Englisch |
Erschienen: |
2009 |
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Schlagwörter: |
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Anmerkung: |
© Springer Science+Business Media B.V. 2009 |
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Übergeordnetes Werk: |
Enthalten in: Space science reviews - Springer Netherlands, 1962, 148(2009), 1-4 vom: 12. Mai, Seite 383-395 |
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Übergeordnetes Werk: |
volume:148 ; year:2009 ; number:1-4 ; day:12 ; month:05 ; pages:383-395 |
Links: |
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DOI / URN: |
10.1007/s11214-009-9516-7 |
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Katalog-ID: |
OLC2033695875 |
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520 | |a Abstract Classical torques acting on the GP-B gyroscopes decrease the accuracy in the measurement of the relativistic drift rate. Based on measurements made during the year-long science data collection, tests done following the science data collection, and a theoretical analysis of potential torques, there are two dominant classical torques acting on the gyroscopes. The first torque, known as the misalignment torque, has a magnitude proportional to the misalignment between the gyroscope spin axis and the satellite roll axis and is aligned perpendicular to the plane containing these two vectors. The second torque, known as the resonance torque, mainly produces a permanent offset in the orientation of the gyroscope spin axis when a harmonic of the gyroscope polhode frequency is in the vicinity of the satellite roll frequency. These two torques have the same physical origin: an electrostatic interaction between the patch effect fields on the surfaces of the rotor and the housing. In the post-mission data analysis, the change in the gyroscope orientation due to both of these torques can be clearly separated from the relativistic drift rate. | ||
650 | 4 | |a Gravity probe B | |
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700 | 1 | |a Silbergleit, A. S. |4 aut | |
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10.1007/s11214-009-9516-7 doi (DE-627)OLC2033695875 (DE-He213)s11214-009-9516-7-p DE-627 ger DE-627 rakwb eng 600 VZ 16,12 ssgn Keiser, G. M. verfasserin aut Misalignment and Resonance Torques and Their Treatment in the GP-B Data Analysis 2009 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media B.V. 2009 Abstract Classical torques acting on the GP-B gyroscopes decrease the accuracy in the measurement of the relativistic drift rate. Based on measurements made during the year-long science data collection, tests done following the science data collection, and a theoretical analysis of potential torques, there are two dominant classical torques acting on the gyroscopes. The first torque, known as the misalignment torque, has a magnitude proportional to the misalignment between the gyroscope spin axis and the satellite roll axis and is aligned perpendicular to the plane containing these two vectors. The second torque, known as the resonance torque, mainly produces a permanent offset in the orientation of the gyroscope spin axis when a harmonic of the gyroscope polhode frequency is in the vicinity of the satellite roll frequency. These two torques have the same physical origin: an electrostatic interaction between the patch effect fields on the surfaces of the rotor and the housing. In the post-mission data analysis, the change in the gyroscope orientation due to both of these torques can be clearly separated from the relativistic drift rate. Gravity probe B Experimental tests of gravitational theories Patch effect Gyroscope torques Kolodziejczak, J. aut Silbergleit, A. S. aut Enthalten in Space science reviews Springer Netherlands, 1962 148(2009), 1-4 vom: 12. Mai, Seite 383-395 (DE-627)129086606 (DE-600)4860-4 (DE-576)014420724 0038-6308 nnns volume:148 year:2009 number:1-4 day:12 month:05 pages:383-395 https://doi.org/10.1007/s11214-009-9516-7 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-AST SSG-OPC-AST GBV_ILN_22 GBV_ILN_40 GBV_ILN_47 GBV_ILN_70 GBV_ILN_2279 GBV_ILN_4046 GBV_ILN_4306 GBV_ILN_4700 AR 148 2009 1-4 12 05 383-395 |
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10.1007/s11214-009-9516-7 doi (DE-627)OLC2033695875 (DE-He213)s11214-009-9516-7-p DE-627 ger DE-627 rakwb eng 600 VZ 16,12 ssgn Keiser, G. M. verfasserin aut Misalignment and Resonance Torques and Their Treatment in the GP-B Data Analysis 2009 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media B.V. 2009 Abstract Classical torques acting on the GP-B gyroscopes decrease the accuracy in the measurement of the relativistic drift rate. Based on measurements made during the year-long science data collection, tests done following the science data collection, and a theoretical analysis of potential torques, there are two dominant classical torques acting on the gyroscopes. The first torque, known as the misalignment torque, has a magnitude proportional to the misalignment between the gyroscope spin axis and the satellite roll axis and is aligned perpendicular to the plane containing these two vectors. The second torque, known as the resonance torque, mainly produces a permanent offset in the orientation of the gyroscope spin axis when a harmonic of the gyroscope polhode frequency is in the vicinity of the satellite roll frequency. These two torques have the same physical origin: an electrostatic interaction between the patch effect fields on the surfaces of the rotor and the housing. In the post-mission data analysis, the change in the gyroscope orientation due to both of these torques can be clearly separated from the relativistic drift rate. Gravity probe B Experimental tests of gravitational theories Patch effect Gyroscope torques Kolodziejczak, J. aut Silbergleit, A. S. aut Enthalten in Space science reviews Springer Netherlands, 1962 148(2009), 1-4 vom: 12. Mai, Seite 383-395 (DE-627)129086606 (DE-600)4860-4 (DE-576)014420724 0038-6308 nnns volume:148 year:2009 number:1-4 day:12 month:05 pages:383-395 https://doi.org/10.1007/s11214-009-9516-7 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-AST SSG-OPC-AST GBV_ILN_22 GBV_ILN_40 GBV_ILN_47 GBV_ILN_70 GBV_ILN_2279 GBV_ILN_4046 GBV_ILN_4306 GBV_ILN_4700 AR 148 2009 1-4 12 05 383-395 |
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10.1007/s11214-009-9516-7 doi (DE-627)OLC2033695875 (DE-He213)s11214-009-9516-7-p DE-627 ger DE-627 rakwb eng 600 VZ 16,12 ssgn Keiser, G. M. verfasserin aut Misalignment and Resonance Torques and Their Treatment in the GP-B Data Analysis 2009 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media B.V. 2009 Abstract Classical torques acting on the GP-B gyroscopes decrease the accuracy in the measurement of the relativistic drift rate. Based on measurements made during the year-long science data collection, tests done following the science data collection, and a theoretical analysis of potential torques, there are two dominant classical torques acting on the gyroscopes. The first torque, known as the misalignment torque, has a magnitude proportional to the misalignment between the gyroscope spin axis and the satellite roll axis and is aligned perpendicular to the plane containing these two vectors. The second torque, known as the resonance torque, mainly produces a permanent offset in the orientation of the gyroscope spin axis when a harmonic of the gyroscope polhode frequency is in the vicinity of the satellite roll frequency. These two torques have the same physical origin: an electrostatic interaction between the patch effect fields on the surfaces of the rotor and the housing. In the post-mission data analysis, the change in the gyroscope orientation due to both of these torques can be clearly separated from the relativistic drift rate. Gravity probe B Experimental tests of gravitational theories Patch effect Gyroscope torques Kolodziejczak, J. aut Silbergleit, A. S. aut Enthalten in Space science reviews Springer Netherlands, 1962 148(2009), 1-4 vom: 12. Mai, Seite 383-395 (DE-627)129086606 (DE-600)4860-4 (DE-576)014420724 0038-6308 nnns volume:148 year:2009 number:1-4 day:12 month:05 pages:383-395 https://doi.org/10.1007/s11214-009-9516-7 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-AST SSG-OPC-AST GBV_ILN_22 GBV_ILN_40 GBV_ILN_47 GBV_ILN_70 GBV_ILN_2279 GBV_ILN_4046 GBV_ILN_4306 GBV_ILN_4700 AR 148 2009 1-4 12 05 383-395 |
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10.1007/s11214-009-9516-7 doi (DE-627)OLC2033695875 (DE-He213)s11214-009-9516-7-p DE-627 ger DE-627 rakwb eng 600 VZ 16,12 ssgn Keiser, G. M. verfasserin aut Misalignment and Resonance Torques and Their Treatment in the GP-B Data Analysis 2009 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media B.V. 2009 Abstract Classical torques acting on the GP-B gyroscopes decrease the accuracy in the measurement of the relativistic drift rate. Based on measurements made during the year-long science data collection, tests done following the science data collection, and a theoretical analysis of potential torques, there are two dominant classical torques acting on the gyroscopes. The first torque, known as the misalignment torque, has a magnitude proportional to the misalignment between the gyroscope spin axis and the satellite roll axis and is aligned perpendicular to the plane containing these two vectors. The second torque, known as the resonance torque, mainly produces a permanent offset in the orientation of the gyroscope spin axis when a harmonic of the gyroscope polhode frequency is in the vicinity of the satellite roll frequency. These two torques have the same physical origin: an electrostatic interaction between the patch effect fields on the surfaces of the rotor and the housing. In the post-mission data analysis, the change in the gyroscope orientation due to both of these torques can be clearly separated from the relativistic drift rate. Gravity probe B Experimental tests of gravitational theories Patch effect Gyroscope torques Kolodziejczak, J. aut Silbergleit, A. S. aut Enthalten in Space science reviews Springer Netherlands, 1962 148(2009), 1-4 vom: 12. Mai, Seite 383-395 (DE-627)129086606 (DE-600)4860-4 (DE-576)014420724 0038-6308 nnns volume:148 year:2009 number:1-4 day:12 month:05 pages:383-395 https://doi.org/10.1007/s11214-009-9516-7 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-AST SSG-OPC-AST GBV_ILN_22 GBV_ILN_40 GBV_ILN_47 GBV_ILN_70 GBV_ILN_2279 GBV_ILN_4046 GBV_ILN_4306 GBV_ILN_4700 AR 148 2009 1-4 12 05 383-395 |
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10.1007/s11214-009-9516-7 doi (DE-627)OLC2033695875 (DE-He213)s11214-009-9516-7-p DE-627 ger DE-627 rakwb eng 600 VZ 16,12 ssgn Keiser, G. M. verfasserin aut Misalignment and Resonance Torques and Their Treatment in the GP-B Data Analysis 2009 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media B.V. 2009 Abstract Classical torques acting on the GP-B gyroscopes decrease the accuracy in the measurement of the relativistic drift rate. Based on measurements made during the year-long science data collection, tests done following the science data collection, and a theoretical analysis of potential torques, there are two dominant classical torques acting on the gyroscopes. The first torque, known as the misalignment torque, has a magnitude proportional to the misalignment between the gyroscope spin axis and the satellite roll axis and is aligned perpendicular to the plane containing these two vectors. The second torque, known as the resonance torque, mainly produces a permanent offset in the orientation of the gyroscope spin axis when a harmonic of the gyroscope polhode frequency is in the vicinity of the satellite roll frequency. These two torques have the same physical origin: an electrostatic interaction between the patch effect fields on the surfaces of the rotor and the housing. In the post-mission data analysis, the change in the gyroscope orientation due to both of these torques can be clearly separated from the relativistic drift rate. Gravity probe B Experimental tests of gravitational theories Patch effect Gyroscope torques Kolodziejczak, J. aut Silbergleit, A. S. aut Enthalten in Space science reviews Springer Netherlands, 1962 148(2009), 1-4 vom: 12. Mai, Seite 383-395 (DE-627)129086606 (DE-600)4860-4 (DE-576)014420724 0038-6308 nnns volume:148 year:2009 number:1-4 day:12 month:05 pages:383-395 https://doi.org/10.1007/s11214-009-9516-7 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-AST SSG-OPC-AST GBV_ILN_22 GBV_ILN_40 GBV_ILN_47 GBV_ILN_70 GBV_ILN_2279 GBV_ILN_4046 GBV_ILN_4306 GBV_ILN_4700 AR 148 2009 1-4 12 05 383-395 |
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Misalignment and Resonance Torques and Their Treatment in the GP-B Data Analysis |
abstract |
Abstract Classical torques acting on the GP-B gyroscopes decrease the accuracy in the measurement of the relativistic drift rate. Based on measurements made during the year-long science data collection, tests done following the science data collection, and a theoretical analysis of potential torques, there are two dominant classical torques acting on the gyroscopes. The first torque, known as the misalignment torque, has a magnitude proportional to the misalignment between the gyroscope spin axis and the satellite roll axis and is aligned perpendicular to the plane containing these two vectors. The second torque, known as the resonance torque, mainly produces a permanent offset in the orientation of the gyroscope spin axis when a harmonic of the gyroscope polhode frequency is in the vicinity of the satellite roll frequency. These two torques have the same physical origin: an electrostatic interaction between the patch effect fields on the surfaces of the rotor and the housing. In the post-mission data analysis, the change in the gyroscope orientation due to both of these torques can be clearly separated from the relativistic drift rate. © Springer Science+Business Media B.V. 2009 |
abstractGer |
Abstract Classical torques acting on the GP-B gyroscopes decrease the accuracy in the measurement of the relativistic drift rate. Based on measurements made during the year-long science data collection, tests done following the science data collection, and a theoretical analysis of potential torques, there are two dominant classical torques acting on the gyroscopes. The first torque, known as the misalignment torque, has a magnitude proportional to the misalignment between the gyroscope spin axis and the satellite roll axis and is aligned perpendicular to the plane containing these two vectors. The second torque, known as the resonance torque, mainly produces a permanent offset in the orientation of the gyroscope spin axis when a harmonic of the gyroscope polhode frequency is in the vicinity of the satellite roll frequency. These two torques have the same physical origin: an electrostatic interaction between the patch effect fields on the surfaces of the rotor and the housing. In the post-mission data analysis, the change in the gyroscope orientation due to both of these torques can be clearly separated from the relativistic drift rate. © Springer Science+Business Media B.V. 2009 |
abstract_unstemmed |
Abstract Classical torques acting on the GP-B gyroscopes decrease the accuracy in the measurement of the relativistic drift rate. Based on measurements made during the year-long science data collection, tests done following the science data collection, and a theoretical analysis of potential torques, there are two dominant classical torques acting on the gyroscopes. The first torque, known as the misalignment torque, has a magnitude proportional to the misalignment between the gyroscope spin axis and the satellite roll axis and is aligned perpendicular to the plane containing these two vectors. The second torque, known as the resonance torque, mainly produces a permanent offset in the orientation of the gyroscope spin axis when a harmonic of the gyroscope polhode frequency is in the vicinity of the satellite roll frequency. These two torques have the same physical origin: an electrostatic interaction between the patch effect fields on the surfaces of the rotor and the housing. In the post-mission data analysis, the change in the gyroscope orientation due to both of these torques can be clearly separated from the relativistic drift rate. © Springer Science+Business Media B.V. 2009 |
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container_issue |
1-4 |
title_short |
Misalignment and Resonance Torques and Their Treatment in the GP-B Data Analysis |
url |
https://doi.org/10.1007/s11214-009-9516-7 |
remote_bool |
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author2 |
Kolodziejczak, J. Silbergleit, A. S. |
author2Str |
Kolodziejczak, J. Silbergleit, A. S. |
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doi_str |
10.1007/s11214-009-9516-7 |
up_date |
2024-07-03T18:03:34.681Z |
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