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*From*: David Rutherford <drutherford@SOFTCOM.NET>*Date*: Sat, 16 Jun 2001 18:30:37 -0700

On Sat, 16 Jun 2001 18:49:30 -0400, Bob Sciamanda <trebor@VELOCITY.NET>

wrote:

David,

I have not yet found the time to read your provoking writings, but let me

raise one question which I have noticed. You correctly state that the

Maxwellian forces of interaction between two electrons are not, in the

general case, "equal and opposite." You then state that these forces ARE

equal snd opposite in the CM frame, "because of symmetry". I doubt the

truth of this latter statement - please prove.

Hi Bob,

The electrons in the CM frame are always travelling on parallel paths at

the same speed, but opposite directions, or are both at rest, so v = -v'

or v = v' = 0. The Lorentz force on q due to q' is

F = q(E + v x B)

Substituting B = (1/c^2)(v' x E), you get

F = q(E + (1/c^2)(v x (v' x E))) (*)

and since

v x (v' x E) = v'(v . E) - E(v . v')

(*) becomes

F = q(E + (1/c^2)(v'(v . E) - E(v . v')))

The electric fields are equal in magnitude and opposite in direction, so

E = -E', and since q = q', we can say for the case v = -v' in the CM

frame,

F = -q'(E' + (1/c^2)(v(v' . E') - E'(v' . v))) (**)

From the vector identity

v' x (v x E') = v(v' . E') - E'(v' . v)

we can write (**) as

F = -q'(E' + (1/c^2)(v' x (v x E'))) (***)

or, since B' = (1/c^2)(v x E'), we can write (***) as

F = -q'(E' + v' x B')

and, since F' = q'(E' + v' x B'),

F = -F'

Now, for the case v = v' = 0, we have simply

F = qE = -q'E' = -F'

So for all cases in the CM frame, the forces are equal and opposite,

using just the Lorentz force equations.

--

Dave Rutherford

"New Transformation Equations and the Electric Field Four-vector"

http://www.softcom.net/users/der555

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