Semon said:
The response by Anders is correct. F=dp/dt by definition. If the mass of the system is constant, then F=ma follows.
Neddy Bate said:
Acceleration approaches infinity as mass approaches zero. Where does an infinite acceleration take a zero-mass particle? To an infinite velocity, instantaneously.
Not necessarily. Acceleration is the
rate of change of velocity with respect to time. An infinite rate of change of a function does not imply that the value of the function is infinite. Look at the unit step function U(t). On the interval (-infinity,0<sup>-</sup>) the function is zero, and on (0<sup>+</sup>, +infinity) the function is 1. The derivative of U(t) blows up to infinity at t=0, but the function itself does not blow up to infinity.
Neddy Bate said:
Does this accurately reflect what light does, for example?
Of course not. Newton's second law was never meant to apply to light.
Neddy Bate said:
One can see why the formula might need some tweaking with respect to c in vacuo.
It doesn't need tweaking at all. One does not describe light with Newton, one describes light with Maxwell.
PhysMachine said:
True, F=ma requires that we are not accounting for relativistic effects.
Not if the 4-vectors F and a are used. And if the mass of the system is not constant, then we can still use F=dp/dT in relativity provided that F and p are 4-vectors and T is the proper time.
PhysMachine said:
If we were, we would have to deploy General Relativity on our accelerating reference frame, and that's a whole new can of worms.
That is not true. Special Relativity is perfectly capable of dealing with forces and accelerations. It's just that in SR accelerated frames are treated on a different footing than inertial frames, whereas in GR all frames are treated on equal footing.
martillo said:
It's inevitable! The only theory that neglects the formula F=ma is Relativity!
That's wrong on 2 counts.
First, it's wrong because F=ma
does appear in relativistic dynamics. And second, it's wrong because there are
other theories that
do not acknowledge F=ma, such as QM and QFT.
martillo said:
The question is wether the mass m really varies with velocity or not.
No, that's not the question. The question is whether the quantities that are really conserved in nature are the 3-momentum and energy or the 4-momentum. Variation of mass with velocity is a matter of interpretation only. Whether one accepts it or rejects it has no bearing on relativistic dynamics.
martillo said:
I propose to take a deep look in Davisson-Germer experiment. Remember? The experiment that relates the De Broglie wave-lenght to the velocity of electrons. It's amazing to note that in this experiment the classic formula for the kinetic energy is used: K=mv2/2 (this is only true if we assume the formula of this thread: F=ma), not the relativistic one: K=(m-m0)c2.
It's not amazing at all, and you cite the reason why yourself. The electrons are decidedly nonrelativistic. Using the nonrelativistic expression for kinetic energy is no more "amazing" than an atomic theorist who uses nonrelativistic quantum mechanics.
martillo said:
Of course it can be argued that the velocities are too small for relativistic effects appear but the electrons were accelerated only by 50 volts! It would be very easy to accelerate them more and verify what happens with the mass! It's an excellent experiment for both the relativity defenders and who are against.
Ask anyone who works at any medium or high energy facility and they will tell you: You have to use relativistic formulae to match observations at relativistic velocities. It's a matter of daily routine for such people.