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-----Original Message-----
From: phys-l-bounces@carnot.physics.buffalo.edu [mailto:phys-l-
bounces@carnot.physics.buffalo.edu] On Behalf Of Tom Sandin
Sent: Wednesday, February 27, 2008 11:41 AM
To: Forum for Physics Educators
Cc: LaMontagne, Bob
Subject: Re: [Phys-l] Invariant mass and relativist mass...
Look at my
Subject: [Phys-l] Non-existence of Transverse and Longitudinal
Relativistic
Mass
post.
If the students are at the |F| = m|a| level, they need to be told
that version of Newton's second law is true only for constant mass.
When the force and velocity are perpendicular, the speed and
therefore the relativistic mass are constant--and F/a equals the
relativistic mass.
When the force and velocity are parallel, the speed and therefore the
relativistic mass are not constant and F is not equal to ma.
(F, p, v, and a are vectors in this paragraph.) For a particle in an
inertial reference frame, the net force equals the time rate of
change of its linear momentum, F = dp/dt = d(mv)/dt. Only if m is
constant does this give F = m dv/dt = ma. If m is not constant, you
have a second (dm/dt)v term.
John Denker's reply is from the perspective of an relativistic mass
opponent.
Tom Sandin
At 7:06 PM -0500 2/26/08, LaMontagne, Bob wrote:
I am still having a problem understanding why the gamma factor would_______________________________________________
be applied to the mass at the introductory level. If students are at
the F=ma level, then the "m" that gives the reistance to
acceleration is really m0/(1-v^2/c^2)^(3/2), as I had noted in
another posting. The gamma factor is actually not the factor that
gives the increased resistance to acceleration - so why use it? If
the studets are at the Impulse=momentum_change level, then the use
of the gamma factor as part of the momentum seems quite natural when
exploring the dynamics of Relativity.
Bob at PC
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