Conventionalism and general relativity
Abstract We argue that the geometry of spacetime is a convention that can be freely chosen by the scientist; no experiment can ever determine this geometry of spacetime, only the behavior of matter in space and time. General relativity is then rewritten in terms of an arbitrary conventional geometry...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Roxburgh, I. W. [verfasserIn] |
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| Format: |
Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
1978 |
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| Schlagwörter: |
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| Anmerkung: |
© Plenum Publishing Corporation 1978 |
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| Übergeordnetes Werk: |
Enthalten in: Foundations of physics - Kluwer Academic Publishers-Plenum Publishers, 1970, 8(1978), 3-4 vom: Apr., Seite 229-237 |
|---|---|
| Übergeordnetes Werk: |
volume:8 ; year:1978 ; number:3-4 ; month:04 ; pages:229-237 |
| Links: |
|---|
| DOI / URN: |
10.1007/BF00715209 |
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OLC2039076352 |
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| 520 | |a Abstract We argue that the geometry of spacetime is a convention that can be freely chosen by the scientist; no experiment can ever determine this geometry of spacetime, only the behavior of matter in space and time. General relativity is then rewritten in terms of an arbitrary conventional geometry of spacetime in which particle trajectories are determined by forces in that geometry, and the forces determined by fields produced by sources in that geometry. As an example, we consider radial trajectories in the field of a single particle expressed in the spacetime of special relativity. | ||
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10.1007/BF00715209 doi (DE-627)OLC2039076352 (DE-He213)BF00715209-p DE-627 ger DE-627 rakwb eng 570 530 VZ 11 12 5,21 ssgn Roxburgh, I. W. verfasserin aut Conventionalism and general relativity 1978 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1978 Abstract We argue that the geometry of spacetime is a convention that can be freely chosen by the scientist; no experiment can ever determine this geometry of spacetime, only the behavior of matter in space and time. General relativity is then rewritten in terms of an arbitrary conventional geometry of spacetime in which particle trajectories are determined by forces in that geometry, and the forces determined by fields produced by sources in that geometry. As an example, we consider radial trajectories in the field of a single particle expressed in the spacetime of special relativity. General Relativity Single Particle Special Relativity Particle Trajectory Radial Trajectory Tavakol, R. K. aut Enthalten in Foundations of physics Kluwer Academic Publishers-Plenum Publishers, 1970 8(1978), 3-4 vom: Apr., Seite 229-237 (DE-627)130020907 (DE-600)421748-2 (DE-576)015562387 0015-9018 nnns volume:8 year:1978 number:3-4 month:04 pages:229-237 https://doi.org/10.1007/BF00715209 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY SSG-OLC-AST SSG-OPC-AST GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_24 GBV_ILN_30 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_70 GBV_ILN_130 GBV_ILN_2006 GBV_ILN_2279 GBV_ILN_4012 GBV_ILN_4046 GBV_ILN_4305 GBV_ILN_4318 AR 8 1978 3-4 04 229-237 |
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10.1007/BF00715209 doi (DE-627)OLC2039076352 (DE-He213)BF00715209-p DE-627 ger DE-627 rakwb eng 570 530 VZ 11 12 5,21 ssgn Roxburgh, I. W. verfasserin aut Conventionalism and general relativity 1978 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1978 Abstract We argue that the geometry of spacetime is a convention that can be freely chosen by the scientist; no experiment can ever determine this geometry of spacetime, only the behavior of matter in space and time. General relativity is then rewritten in terms of an arbitrary conventional geometry of spacetime in which particle trajectories are determined by forces in that geometry, and the forces determined by fields produced by sources in that geometry. As an example, we consider radial trajectories in the field of a single particle expressed in the spacetime of special relativity. General Relativity Single Particle Special Relativity Particle Trajectory Radial Trajectory Tavakol, R. K. aut Enthalten in Foundations of physics Kluwer Academic Publishers-Plenum Publishers, 1970 8(1978), 3-4 vom: Apr., Seite 229-237 (DE-627)130020907 (DE-600)421748-2 (DE-576)015562387 0015-9018 nnns volume:8 year:1978 number:3-4 month:04 pages:229-237 https://doi.org/10.1007/BF00715209 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY SSG-OLC-AST SSG-OPC-AST GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_24 GBV_ILN_30 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_70 GBV_ILN_130 GBV_ILN_2006 GBV_ILN_2279 GBV_ILN_4012 GBV_ILN_4046 GBV_ILN_4305 GBV_ILN_4318 AR 8 1978 3-4 04 229-237 |
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10.1007/BF00715209 doi (DE-627)OLC2039076352 (DE-He213)BF00715209-p DE-627 ger DE-627 rakwb eng 570 530 VZ 11 12 5,21 ssgn Roxburgh, I. W. verfasserin aut Conventionalism and general relativity 1978 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1978 Abstract We argue that the geometry of spacetime is a convention that can be freely chosen by the scientist; no experiment can ever determine this geometry of spacetime, only the behavior of matter in space and time. General relativity is then rewritten in terms of an arbitrary conventional geometry of spacetime in which particle trajectories are determined by forces in that geometry, and the forces determined by fields produced by sources in that geometry. As an example, we consider radial trajectories in the field of a single particle expressed in the spacetime of special relativity. General Relativity Single Particle Special Relativity Particle Trajectory Radial Trajectory Tavakol, R. K. aut Enthalten in Foundations of physics Kluwer Academic Publishers-Plenum Publishers, 1970 8(1978), 3-4 vom: Apr., Seite 229-237 (DE-627)130020907 (DE-600)421748-2 (DE-576)015562387 0015-9018 nnns volume:8 year:1978 number:3-4 month:04 pages:229-237 https://doi.org/10.1007/BF00715209 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY SSG-OLC-AST SSG-OPC-AST GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_24 GBV_ILN_30 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_70 GBV_ILN_130 GBV_ILN_2006 GBV_ILN_2279 GBV_ILN_4012 GBV_ILN_4046 GBV_ILN_4305 GBV_ILN_4318 AR 8 1978 3-4 04 229-237 |
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10.1007/BF00715209 doi (DE-627)OLC2039076352 (DE-He213)BF00715209-p DE-627 ger DE-627 rakwb eng 570 530 VZ 11 12 5,21 ssgn Roxburgh, I. W. verfasserin aut Conventionalism and general relativity 1978 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1978 Abstract We argue that the geometry of spacetime is a convention that can be freely chosen by the scientist; no experiment can ever determine this geometry of spacetime, only the behavior of matter in space and time. General relativity is then rewritten in terms of an arbitrary conventional geometry of spacetime in which particle trajectories are determined by forces in that geometry, and the forces determined by fields produced by sources in that geometry. As an example, we consider radial trajectories in the field of a single particle expressed in the spacetime of special relativity. General Relativity Single Particle Special Relativity Particle Trajectory Radial Trajectory Tavakol, R. K. aut Enthalten in Foundations of physics Kluwer Academic Publishers-Plenum Publishers, 1970 8(1978), 3-4 vom: Apr., Seite 229-237 (DE-627)130020907 (DE-600)421748-2 (DE-576)015562387 0015-9018 nnns volume:8 year:1978 number:3-4 month:04 pages:229-237 https://doi.org/10.1007/BF00715209 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY SSG-OLC-AST SSG-OPC-AST GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_24 GBV_ILN_30 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_70 GBV_ILN_130 GBV_ILN_2006 GBV_ILN_2279 GBV_ILN_4012 GBV_ILN_4046 GBV_ILN_4305 GBV_ILN_4318 AR 8 1978 3-4 04 229-237 |
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10.1007/BF00715209 doi (DE-627)OLC2039076352 (DE-He213)BF00715209-p DE-627 ger DE-627 rakwb eng 570 530 VZ 11 12 5,21 ssgn Roxburgh, I. W. verfasserin aut Conventionalism and general relativity 1978 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1978 Abstract We argue that the geometry of spacetime is a convention that can be freely chosen by the scientist; no experiment can ever determine this geometry of spacetime, only the behavior of matter in space and time. General relativity is then rewritten in terms of an arbitrary conventional geometry of spacetime in which particle trajectories are determined by forces in that geometry, and the forces determined by fields produced by sources in that geometry. As an example, we consider radial trajectories in the field of a single particle expressed in the spacetime of special relativity. General Relativity Single Particle Special Relativity Particle Trajectory Radial Trajectory Tavakol, R. K. aut Enthalten in Foundations of physics Kluwer Academic Publishers-Plenum Publishers, 1970 8(1978), 3-4 vom: Apr., Seite 229-237 (DE-627)130020907 (DE-600)421748-2 (DE-576)015562387 0015-9018 nnns volume:8 year:1978 number:3-4 month:04 pages:229-237 https://doi.org/10.1007/BF00715209 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY SSG-OLC-AST SSG-OPC-AST GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_24 GBV_ILN_30 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_70 GBV_ILN_130 GBV_ILN_2006 GBV_ILN_2279 GBV_ILN_4012 GBV_ILN_4046 GBV_ILN_4305 GBV_ILN_4318 AR 8 1978 3-4 04 229-237 |
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Abstract We argue that the geometry of spacetime is a convention that can be freely chosen by the scientist; no experiment can ever determine this geometry of spacetime, only the behavior of matter in space and time. General relativity is then rewritten in terms of an arbitrary conventional geometry of spacetime in which particle trajectories are determined by forces in that geometry, and the forces determined by fields produced by sources in that geometry. As an example, we consider radial trajectories in the field of a single particle expressed in the spacetime of special relativity. © Plenum Publishing Corporation 1978 |
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Abstract We argue that the geometry of spacetime is a convention that can be freely chosen by the scientist; no experiment can ever determine this geometry of spacetime, only the behavior of matter in space and time. General relativity is then rewritten in terms of an arbitrary conventional geometry of spacetime in which particle trajectories are determined by forces in that geometry, and the forces determined by fields produced by sources in that geometry. As an example, we consider radial trajectories in the field of a single particle expressed in the spacetime of special relativity. © Plenum Publishing Corporation 1978 |
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Abstract We argue that the geometry of spacetime is a convention that can be freely chosen by the scientist; no experiment can ever determine this geometry of spacetime, only the behavior of matter in space and time. General relativity is then rewritten in terms of an arbitrary conventional geometry of spacetime in which particle trajectories are determined by forces in that geometry, and the forces determined by fields produced by sources in that geometry. As an example, we consider radial trajectories in the field of a single particle expressed in the spacetime of special relativity. © Plenum Publishing Corporation 1978 |
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Conventionalism and general relativity |
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