Jump to content

Kepler's Law of Areal Velocity in Cyclones: Difference between revisions

From Natural Philosophy Wiki
Imported from text file
ClaudeBot (talk | contribs)
Add full-text link (reconnected from abstracts archive; URL verified live)
Line 1: Line 1:
{{Infobox paper
{{Infobox paper
| title = Kepler\'s Law of Areal Velocity in Cyclones
| title = Kepler\'s Law of Areal Velocity in Cyclones
| url = [http://gsjournal.net/Science-Journals/Research%20Papers-Mechanics%20/%20Electrodynamics/Download/239 Link to paper]
| author = [[David Tombe]]
| author = [[David Tombe]]
| published = 2009
| published = 2009
Line 6: Line 7:
| num_pages = 5
| num_pages = 5
}}
}}
'''Read the full paper''' [http://gsjournal.net/Science-Journals/Research%20Papers-Mechanics%20/%20Electrodynamics/Download/239 here]


==Abstract==
==Abstract==

Revision as of 18:50, 18 July 2026

Scientific Paper
TitleKepler\'s Law of Areal Velocity in Cyclones
Read in fullLink to paper
Author(s)David Tombe
Published2009
JournalGeneral Science Journal
No. of pages5

Read the full paper here

Abstract

Faraday?'s law of electromagnetic induction and Kepler'fs law of areal velocity are two manifestations of a single principle which requires two distinct phenomena for its full understanding. The former is an expression for the rate of change of angular momentum, with particular reference to the sea of tiny molecular vortices which acts as the domain of the electromagnetic field. The latter expresses conservation of angular momentum in situations in which there is no net tangential force in that same sea of molecular vortices. The single principle which lies behind these two laws needs to be split into two distinct phenomena for the full understanding of the principle. These two phenomena are Coriolis force vXH and angular force ??A/??t. The Coriolis force that is observed in all vortex phenomena is a constituent part of the general principle that underlies both Faraday?'s law and Kepler'fs second law. It is a hydrodynamical effect.