Michael C
Graduate Poster
Now comes the question: in which reference frame are the laws of motion simpler?
a) the surface of the earth
b) the elevator in free fall
The laws of motion that we can use are equally simple in both cases. Both of your examples are reasonably close approximations to inertial frames of reference for suitably "small scale" scenarios, and so Newton's Laws should be adequate. After all, one of the main points of using inertial reference frames is that the same (and also simplest) set of laws apply in all such frames.
If we call both frames inertial things can get confusing, since one frame is clearly accelerating with respect to the other. There's a good presentation of the conflict in terminology here: the author suggests that we should avoid the term "inertial frame" altogether and use the terms "freely-falling frame" and "Newtonian frame".
The laws of physics really are simpler in the freely-falling frame, since it gets rid of the pesky problem of the weird force of gravity acting at a distance. This doesn't mean that it's always simpler to analyse a problem using a freely-falling frame, though! In particular, we're better off using the Newtonian frame (well, the almost Newtonian frame...) of the surface of the earth to analyse the antics of the DDWFTTW cart: no need to complicate matters by looking at it from a freely falling elevator.
There are definitely some very ambiguous and potentially confusing terms "floating around" this whole area. Taken being "weightless" for example. In terms of pure physics, we aren't actually without weight when we say we are experiencing "weightlessness" (because we're in free-fall, etc.). Our "apparent weight" is zero, simply because we are experiencing the state where there are essentially no internal stresses on body organs, etc. In other words our brains think we are without weight because the usual stresses are suddenly removed. But our "real weight" is still given by mass times "acceleration due to gravity". In other words, our "real weight" is the force exerted on our body by gravity, and that force doesn't disappear when we start to free-fall, or start orbiting the Earth.
"Weight" only has meaning relative to a particular frame of reference. With respect to the freely-falling frame of reference, our weight is zero. With respect to the frame of reference of the Earth, our weight is our mass multiplied by g. If we want to be pedantic, instead of talking about "real weight" and "apparent weight", we should talk about "weight as measured in such-and-such frame of reference". I can happily decide that I weigh nothing at all, even though I'm not in free fall, by considering my position from the point of view of a freely-falling reference frame. In this case, the upward force I'm feeling from my chair comes from the fact that it is accelerating my mass upwards through this reference frame at a rate of 9.8 m/s2.
