The role of pseudo-hypersurfaces in non-holonomic motion
The geometry of hypersurfaces is generalized to pseudo-hypersurfaces, which are defined by Pfaff equations. The general methods are then applied to modeling the kinematics of motion constrained by a single linear, non-holonomic constraint. They are then applied to the example of a charge moving in a...
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Format: | Article |
Language: | English |
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AIMS Press
2020-06-01
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Series: | AIMS Mathematics |
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Online Access: | https://www.aimspress.com/article/10.3934/math.2020307/fulltext.html |
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author | David Delphenich |
author_facet | David Delphenich |
author_sort | David Delphenich |
collection | DOAJ |
description | The geometry of hypersurfaces is generalized to pseudo-hypersurfaces, which are defined by Pfaff equations. The general methods are then applied to modeling the kinematics of motion constrained by a single linear, non-holonomic constraint. They are then applied to the example of a charge moving in an electromagnetic field, and the Lorentz equation of motion is shown to represent a geodesic that is constrained to lie in a pseudo-hypersurface that is defined by the potential 1-form. |
first_indexed | 2024-12-12T18:15:16Z |
format | Article |
id | doaj.art-c685d4c6a8314e6b911bb09c31eb4fcb |
institution | Directory Open Access Journal |
issn | 2473-6988 |
language | English |
last_indexed | 2024-12-12T18:15:16Z |
publishDate | 2020-06-01 |
publisher | AIMS Press |
record_format | Article |
series | AIMS Mathematics |
spelling | doaj.art-c685d4c6a8314e6b911bb09c31eb4fcb2022-12-22T00:16:18ZengAIMS PressAIMS Mathematics2473-69882020-06-01554793482910.3934/math.2020307The role of pseudo-hypersurfaces in non-holonomic motionDavid Delphenich0Independent researcher, 1830 SR 725, Spring Valley, OH USA 45370The geometry of hypersurfaces is generalized to pseudo-hypersurfaces, which are defined by Pfaff equations. The general methods are then applied to modeling the kinematics of motion constrained by a single linear, non-holonomic constraint. They are then applied to the example of a charge moving in an electromagnetic field, and the Lorentz equation of motion is shown to represent a geodesic that is constrained to lie in a pseudo-hypersurface that is defined by the potential 1-form.https://www.aimspress.com/article/10.3934/math.2020307/fulltext.htmlnon-holonomic constraintspfaff equationgeometry of hypersurfacesintegrability of differential systemslorentz equationmechanics and differential forms |
spellingShingle | David Delphenich The role of pseudo-hypersurfaces in non-holonomic motion AIMS Mathematics non-holonomic constraints pfaff equation geometry of hypersurfaces integrability of differential systems lorentz equation mechanics and differential forms |
title | The role of pseudo-hypersurfaces in non-holonomic motion |
title_full | The role of pseudo-hypersurfaces in non-holonomic motion |
title_fullStr | The role of pseudo-hypersurfaces in non-holonomic motion |
title_full_unstemmed | The role of pseudo-hypersurfaces in non-holonomic motion |
title_short | The role of pseudo-hypersurfaces in non-holonomic motion |
title_sort | role of pseudo hypersurfaces in non holonomic motion |
topic | non-holonomic constraints pfaff equation geometry of hypersurfaces integrability of differential systems lorentz equation mechanics and differential forms |
url | https://www.aimspress.com/article/10.3934/math.2020307/fulltext.html |
work_keys_str_mv | AT daviddelphenich theroleofpseudohypersurfacesinnonholonomicmotion AT daviddelphenich roleofpseudohypersurfacesinnonholonomicmotion |