Monday, June 2, 2014

This situation is not in conformity with the principle of causal specific uniqueness

From: Jean de Climont <jeandeclimont@yahoo.ca>
Date: Sat, May 31, 2014 at 3:38 AM
Subject: Electron beams magnetic field

Dear Sir,

There is in the current theoretical approach two potential causes of magnetic fields of electric currents : the translation of electrons of Maxwell's equations and the magnetic moment of electrons used in the explanation of magnetism of materials. This situation is not in conformity with the principle of causal specific uniqueness applicable to elementary phenomena , and no more with the simplicity principle of Occam's. It is possible of course to add a new postulate assuming a random distribution of the magnetic moments .

But there is another solution. This is to eliminate the translation of electrons as a cause of the magnetic field of electron flows .

I am pleased to send you a report presenting an experience that should settle the question.

Electron beams magnetic field is not the result of electron motion
but the result of the intrinsic magnetic moment
 
Yours very sincerely

Jean de Climont





Electron beams magnetic field is not a result of electron motion but of their intrinsic magnetic moment. 

(May 2014) 

Jean de Climont 

 jeandeclimont@yahoo.ca 

Abstract : This paper proposes an experiment intended for showing that the magnetic field of electrons is not the result of their translation, but of their magnetic moment. The magnetic moments of electrons are aligned in the metal cathode until the electrons are ejected towards the anode, and then they pass through the hole provided for this purpose to form a cathodic beam. Electric fields do not change the orientation of the magnetic moments of the electrons. If this beam is deflected up to 90 ° by an electric field, the magnetic moments of electrons are no longer parallel to their direction of translation, thus the magnetic field of the cathodic beam should disappear or at least no longer be measured by coils placed in a plane containing the beam, unlike what can be observed before deflection.