My apologies John. In point of fact I wasn't trying to correct you. As I do often with this thread, I use my dandy new humber fast scroller. I saw some back and forth on the gravity vs. acceleration issue, and I added my 1.2 cents (hard economic times) because I've found it a subtle and fascinating issue for some time. I was not specifically trying to correct anyone, but rather clarify a subtle issue (which I've probably failed at).
Thanks, spork. I don't feel that any apology is necessary. I just wanted to clarify it too, and I wanted in particular to clarify it in relation to the heading of the thread. It began because Michael C made a very clear and "obvious" statement that of course an accelerometer in a falling lift would read zero,
because it is not accelerating. There is no drag, he said, so it's in free fall, hence it's not accelerating. It subsequently appears that it is not accelerating because as it accelerates the acceleration produces a force which opposes gravity or something. Hence, despite the walls of the building going past at a velocity that increases at 9.8 m/s/s, you're not accelerating at all. I will now spend the next three months correcting all previous posts about kites and carts and balloons. When you're not accelerating in a gravitational field, you're accelerating. Fine. It's an accelerating frame of reference, and the walls are accelerating at the same speed. When you freefall, you stop accelerating, and the walls continue to accelerate upwards at 9.8 m/s/s. Everything on the earth's surface is accelerating outward at that rate while it's motionless with respect to everything else except things that are falling, which are {ETA:
stationary not accelerating } because they're falling. Have I got it now?
Ah yes - but only because you view it as a 2-dimensional problem. You don't just ignore gravity and vertical acceleration; you ignore the vertical degree of freedom altogether.
Newton seems to say that there's a force down on you and a force up on you, and they equal out, so you remain at the velocity you were at before. We've been discussing classical mechanics and bashing humber over the head with F = ma long enough. Suddenly we're in Einstein country, where spacetime is curved and mass causes an acceleration field.
Actually, if a massive body suddenly materialized next to our free floating accelerometer, the accelerometer would in fact start to accelerate toward that body, but continue to read zero acceleration.
You must have speed scrolled through the next bit. RossFW (I think) put me right about that. However, as I said, if a mass suddenly materialised next to you with a physical resistance, a normal force, the accelerometer would now measure 1 g. You haven't physically moved in classical terms, you haven't accelerated in classical terms. Your accelerometer is measuring a force of gravity on its moving part. It measures 0g. Then it measures 1g. It didn't move. Great these things arent they?
"suddenly" is trickier still. The "knowledge" that this massive body just appeared travels at the speed of light. The gravitational effect travels at the same speed. So it would not accelerate toward it instantly, but pretty darn soon after it materialized. And in any case the accelerometer would read exactly zero throughout.
Sure. "Suddenly" was just rhetoric. Again, Newton didn't deal with the speed of light as far as I'm aware, at least if he did, I don't think it comes into his laws of motion. Classical mechanics - have we actually defined it in this thread at all? I thought it was pretty much Newton's three laws, and the conservation of energy and conservation of momentum. I didn't think warped spacetime and the speed of light came into it.
Gravity is not a force. Gravity times mass is (or produces?) a force. Gravity is more accurately considered an acceleration field.
Hmmm. I'm not sure about that. Once again, from a Newtonian perspective, I thought gravity was considered a force, F = G m1 m2/d2, which produced an "acceleration
due to gravity", g. if not resisted.
Correct. This is the root of the two gradient effects seen with gravity, and not seen with linear acceleration.
So gravity is not the same as acceleration? How do you explain the way we call something "equivalent" without there being two different things to equate? Doesn't it mean that there are equivalences, rather than that they are the same thing?
Linear acceleration is seen as parallel. In other words, two accelerometers in the accelerating cart would show acceleration in the exact same direction. Two accelerometers in a cart in a gravitational field (if prevented from accelerating) would show an acceleration in slightly different directions - both pointing toward the center of mass of the nearby massive body.
And again, in classical mechanics, a spring with a load on the end would be described as having a force of gravity upon it. An accelerometer isn't much more than a spring measurer.
I think that these are academic points to some extent. If we take F = ma, the classical explanation suggests that there is a real force, acting on a real mass, and acceleration is a sort of measured change of position over time over time, like it is the result and response of a mass to force. I realise that in reality it is not like that, and that these are all interlinked. I realise that there is something very difficult with action at a distance, as Newton worried about, and that Einstein's view is more encompassing. But really we're getting into the realms of cosmological philosophy. If Michael and you are happy to consider a falling elevator as at rest and the ground accelerating up towards it, fine. We should all get out of the way in either case.
We could just answer the implied question of the thread title, "The validity of classical physics: nope, superceded", and move on. Let's describe the cart on the treadmill from GR theory instead, stop lying about kites and planes maintaining level flight due to balanced forces, and not experiencing acceleration vertically. Let's trawl through this classical mechanics thread making it all agree with Einstein.
I realise that you weren't arguing much about this with me. I just feel that Michael's statement about a falling elevator not accelerating didn't take any account of the context of the conversation, presented this as obvious because he knows what an accelerometer would read (implying that zero G = no acceleration), that this was completely counter to everyday or 'classical' understanding, and he failed to - and still has failed to - say why the building is changing its relative velocity over time wrt the elevator. He hasn't clarified that this statement is only true from the perspective of all stationary objects in a grav field accelerating upwards or whatever it is that they're supposed to be doing.
I'd like to potter about in Newtonian space a bit longer, find my land legs, you know, before I take on Relativity. Call me old. Besides, we don't need any of the last 100 years of advanced physics to make sense of a falling lift, just as was chucked at humber repeatedly when he mentioned anything general-relativistic. And furthermore, people keep using my supposedly wrong terminology, talking about accelerating elevators not feeling any acceleration, to refute my argument. We just need to stick to the same terms, or it's going to get mental.