Locating the Boundary of a Magnetic Field: Difference between revisions
Imported from text file |
infobox: unlink bare volume/issue numbers (removes redlinks to numeric titles) |
||
| (One intermediate revision by one other user not shown) | |||
| Line 4: | Line 4: | ||
| published = 2001 | | published = 2001 | ||
| journal = [[Galilean Electrodynamics]] | | journal = [[Galilean Electrodynamics]] | ||
| volume = | | volume = 12 | ||
| number = | | number = 5 | ||
| pages = 97-99 | | pages = 97-99 | ||
}} | }} | ||
| Line 11: | Line 11: | ||
==Abstract== | ==Abstract== | ||
To ascertain the reach of a magnetic field, equations were found for energy density in the field, a spatial accounting of its internal energy was made, and used to estimate the radius of an outer boundary for the field. If the Biot-Savart law is valid, the test field considered herein, can reach no further than about 70 (cm) from the current section which raised it, regardless of current magnitude.[[Category:Scientific Paper]] | To ascertain the reach of a magnetic field, equations were found for energy density in the field, a spatial accounting of its internal energy was made, and used to estimate the radius of an outer boundary for the field. If the Biot-Savart law is valid, the test field considered herein, can reach no further than about 70 (cm) from the current section which raised it, regardless of current magnitude. | ||
[[Category:Scientific Paper|locating boundary magnetic field]] | |||
Latest revision as of 09:31, 21 July 2026
| Scientific Paper | |
|---|---|
| Title | Locating the Boundary of a Magnetic Field |
| Author(s) | Richard M Collier |
| Published | 2001 |
| Journal | Galilean Electrodynamics |
| Volume | 12 |
| Number | 5 |
| Pages | 97-99 |
Abstract
To ascertain the reach of a magnetic field, equations were found for energy density in the field, a spatial accounting of its internal energy was made, and used to estimate the radius of an outer boundary for the field. If the Biot-Savart law is valid, the test field considered herein, can reach no further than about 70 (cm) from the current section which raised it, regardless of current magnitude.