W.D.Clinger
Philosopher
Quoting a freshman-level textbook on special relativity, with italicized English words as in the original:
A.P.French said:[size=+2]7 More about relativistic dynamics[/size]
In this chapter we shall be discussing two main topics. The first of these is a more extended discussion of momentum and energy, with particular emphasis on the transformation of these quantities between two inertial frames. The second topic is the concept of force in relativistic dynamics—the way in which it is defined, its transformations, and the limitations on its usefulness. We begin with an important invariant that can be constructed from the measured values of momentum and energy in a given frame.
Now a simple way of restating [ E2 = (cp)2 + E02 ] is that, if a particle has rest energy E0 (i.e., total energy E0 as measured in the frame in which its momentum is zero), then its energy and momentum as measured in any other frame can be combined to form an invariant quantity as follows:
E2 - (cp)2 = E02....Since this holds for E and p as measured in any frame, the measures of energy and momentum for a particle in any two frames are related according to the equation
E2 - (cp)2 = (E')2 - (cp')2 = E02....It turns out that [the equation above] applies not merely to a single particle, but to any arbitrary collection of particles, in the following way. If, as measured in any given frame of reference, the sum of the energies of the particles is E and the vector sum of all their momenta is of magnitude p, then the value of E2 - (cp)2 has the same value as the corresponding combination (E')2 - (cp')2 as measured in any other frame. This invariant value is equal to the square of the total energy E0 of all the particles as measured in a frame in which the vector sum of the momenta is zero.
Note especially that, in this extended form..., the energy E0 is not, in general, merely a sum of rest energies. The collection of particles considered may have all kinds of motions relative to one another; there need not exist any frame in which they are all at rest.
....Consider, for example, an argon atom containing numerous electrons in states of rapid motion, and having at its center a nucleus, itself a composite of neutrons and protons with large kinetic energies. We have no hesitation in describing this atom, from the standpoint of the kinetic theory of gases, as a single particle endowed with a certain velocity. And the theorem of the inertia of energy makes it all the easier to think of this complicated structure as being describable in terms of a single mass possessed of a certain momentum, despite our awareness of its internal structure.
In Newtonian mechanics we are accustomed to thinking of measures of space as being definable without reference to time, and vice versa. Likewise, we are accustomed to thinking of momentum and energy as representing essentially different (although to some extent related) properties of a body. We have now seen how these distinctions, both kinematic and dynamic, are blurred in special relativity. The specification of time in one system involves both position and time in another system; the specification of energy involves both energy and momentum in another system.
In the above results one can discern...that in general force and acceleration are not parallel vectors....Only in the instantaneous rest frame of a body...can one guarantee that F, as defined by the time derivative of momentum, is in the same direction as the acceleration.