An Invariant Ratio in Magnetic Acceleration: Difference between revisions
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This paper presents a simple new rule that is followed by every free charged particle in acceleration caused by a spatially-uniform magnetic field. Every particle in such magnetic acceleration has, ''not only'' an acceleration with respect to a stationary reference frame, ''but also'' an acceleration with respect to a ''rotating'' reference frame, which rotates about the direction of the magnetic field with a quasi Larmor frequency; ''these two accelerations are in constant ratio''. This simple new rule is followed perfectly, regardless of how the other concerned laws of physics operate. This simple new rule brings us a brand new picture of magnetic acceleration, and a brand new analytic tool as well. | This paper presents a simple new rule that is followed by every free charged particle in acceleration caused by a spatially-uniform magnetic field. Every particle in such magnetic acceleration has, ''not only'' an acceleration with respect to a stationary reference frame, ''but also'' an acceleration with respect to a ''rotating'' reference frame, which rotates about the direction of the magnetic field with a quasi Larmor frequency; ''these two accelerations are in constant ratio''. This simple new rule is followed perfectly, regardless of how the other concerned laws of physics operate. This simple new rule brings us a brand new picture of magnetic acceleration, and a brand new analytic tool as well. | ||
[[Category:Scientific Paper]] | [[Category:Scientific Paper|invariant ratio magnetic acceleration]] | ||
Latest revision as of 12:00, 1 January 2017
| Scientific Paper | |
|---|---|
| Title | An Invariant Ratio in Magnetic Acceleration |
| Author(s) | Jia-Qiang Cheng |
| Keywords | {{{keywords}}} |
| Published | 2010 |
| Journal | Galilean Electrodynamics |
| Volume | 21 |
| Number | S1 |
| Pages | 17-18 |
Abstract
This paper presents a simple new rule that is followed by every free charged particle in acceleration caused by a spatially-uniform magnetic field. Every particle in such magnetic acceleration has, not only an acceleration with respect to a stationary reference frame, but also an acceleration with respect to a rotating reference frame, which rotates about the direction of the magnetic field with a quasi Larmor frequency; these two accelerations are in constant ratio. This simple new rule is followed perfectly, regardless of how the other concerned laws of physics operate. This simple new rule brings us a brand new picture of magnetic acceleration, and a brand new analytic tool as well.