The Maxwell-Faraday Equation Extended for Convection: Difference between revisions
The Maxwell-Faraday Equation Extended for Convection |
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{{Infobox paper | |||
| title = The Maxwell-Faraday Equation Extended for Convection | |||
| author = [[David Tombe]] | |||
| published = 2023 | |||
| url = https://www.researchgate.net/publication/372409911_The_Maxwell-Faraday_Equation_Extended_for_Convection | |||
}} | |||
==Abstract== | |||
To show that the curl of E = v×B is an additional convective component to the Maxwell-Faraday equation. | To show that the curl of E = v×B is an additional convective component to the Maxwell-Faraday equation. | ||
[[Category:Scientific Paper|maxwell-faraday equation extended for convection]] | |||
[[Category:Electrodynamics|maxwell-faraday equation extended for convection]] | |||
Latest revision as of 07:07, 22 July 2026
| Scientific Paper | |
|---|---|
| Title | The Maxwell-Faraday Equation Extended for Convection |
| Read in full | https://www.researchgate.net/publication/372409911_The_Maxwell-Faraday_Equation_Extended_for_Convection |
| Author(s) | David Tombe |
| Published | 2023 |
Abstract
To show that the curl of E = v×B is an additional convective component to the Maxwell-Faraday equation.