Asking about something that I read on electromagnetic force

In summary, the conversation discusses the concept of Faraday force, which is an accelerating force applied on a charged particle in a magnetic field. This force is derived from the equations for the induced emf and electric field in a changing magnetic field, and can be expressed as F = (1/2B)(dB/dt)mv. The conversation also mentions the importance of references for this force.
  • #1
hagopbul
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TL;DR Summary
read a paper related to electromagnetic force and it mentioned a force i didnt heard before
Hello All:

read a paper related to electromagnetic force and its applications in acceleration of charges particles , some thing came up in it , they drive a force applied on the particle called Faraday force = [1/2B]* [dB/dt]*m*v

B magnetic field , m mass of the particle , v the velocity of the particle

i couldnt find any reference to this force , and didnt help notice the momentum of the particle in the equation
do any one have references about this force

Best
Hagop
 
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  • #2
Here's a scenario where the force equation ##F =\frac 1 {2B} \frac{dB}{dt} mv## arises.
1674015562204.png

Suppose there is a uniform B field in a region of space and there is a particle of mass ##m## and charge ##q## that circles the magnetic field lines with speed ##v##. The figure is drawn for positive ##q##. For nonrelativistic speeds of the particle, the radius of the orbit is determined to be $$r = \frac{mv}{qB}.$$ There is a flux of magnetic field through the circular path equal to $$\Phi = B \pi r^2.$$ If ##B## starts changing at a rate ##\frac{d B}{dt}##, then there will be an induced emf in the path of the particle equal to $$\varepsilon =\frac{d \Phi}{dt} = \frac{dB}{dt} \pi r^2.$$ The emf is due to an induced electric field ##E## and the direction of ##E## at the location of ##q## will be in the direction of ##\vec v## if ##B## is increasing in strength. The relation between ##\varepsilon## and ##E## is $$\varepsilon = E \cdot 2 \pi r.$$ Thus, there will be an accelerating electric force on the charge given by ##F = qE##.

If you put all of these relations together, you find that the accelerating force is ##F = \frac 1 {2B} \frac{dB}{dt} mv##.
 
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