Tiran said:
Is this a claim that has anything to do with relativistic speeds, or are you just pointing out how vectors work?
It is a claim about relativistic speeds and it is one of the bigger differences between relativistic and classical kinematics. In classical mechanics the direction of acceleration is always in the same direction as the force (if it weren't, we wouldn't be able to write ##F=ma##, which only makes sense for scalars and vectors pointing in the same direction). In relativistic mechanics it is not.
As an aside, if we use the modern four-vector formulation (which was not known when relativity was first discovered, or no one would have bothered with the idea of mass increasing with speed) we can write the analogous vector equation ##\vec{F}=m\vec{a}## and it does work properly. But it's very different beast:
- The four-vectors are vectors in four-dimensional spacetime instead of three-dimensional space
- The acceleration four-vector ##\vec{a}## is defined as the time derivative of the velocity four-vector ##\vec{v}## as you'd expect, but ##\vec{v}## has a constant magnitude in all coordinate systems, and only its direction changes.
- The time derivative is with respect to a clock moving at the same speed and in the same direction as the object, at the moment that the force is applied. (That would be "proper time along the object's wordline" in the jargon).
- The ##m## that appears in ##\vec{F}=m\vec{a}## is the mass of the object as observed by an observer at rest relative to it, no adjustments for speed or time dilation needed to make everything come out right.