schroder said:
Now right here you are doing something that is unscientific. You may consider it to be “fun” and I agree there is an element of that, but there is also a serious side of this. This ridiculous claim needs to be rebuked by the physics community. You are dismissing what I wrote as illogical without showing where the logic fails. That is like saying “You are wrong because my name is Vanesch, and I say so.” I would expect better from you.
I never used any argument of authority as far as I remember. I do make "authoritative statements" concerning certain properties of Newtonian mechanics, because I think that I know the theory well enough to make them. Like I could make the authoritative statement that Newton's equation is F = m.a without arguing it, because I think that the "physics community" won't dispute it.
If I tell you (or if I say in general) some statements like "you can do the calculations in any frame you like", then this is not on my authority, but simply because I know it is an entirely accepted fact, and that I don't think that there is any physics professor out there who will dispute it.
However, I have taught university level courses, and I can tell you that any student of mine who would display such ignorance of basic material together with such a refusal to reconsider, would have been in serious trouble. I consider this discussion on my side as an exercise in the Art of Zen
And of course it matters what is working against what! The velocity of the wind working against the sail is not used as a reference to measure the velocity of the boat because the boat is not working against the wind, it is working against the water.
You see, that phrase, by itself, doesn't have any meaning when you use standard terminology. The only meaning one could give to it is that no physically meaningful quantity can ever be calculated using the velocity of the wind. That's of course glaring nonsense. After all, the totally valid question "what is the velocity of the boat wrt to the wind" would need to use the velocity of the wind AND the velocity of the boat, in *any randomly chosen frame*, to be able to calculate the answer to the question.
So if you want to know where your logic fails, it is already right here.
How can you honestly say it does not matter what is working against what when you measure velocities?
Because it is true. The kinematical description of a situation (that is, the positions and velocities and so on) are independent of the dynamical description of the situation (the interactions, the forces...). That is what is explained in about the first chapter of every book on classical mechanics.
For instance, in my engineering education, I started out with 45 hours of kinematics, without even mentioning the word "force". It was only in the next course, 90 hours of "dynamics" that force was introduced. I'm not saying that this is the only or best way to teach mechanics, but at least it demonstrates that the kinematical description has nothing to do with what thing is exercising what force on what other thing.
So I am going to walk you through the logic one more time, and this time You need to show me where the logic fails.
Well, it failed already, but let us continue (in my practice of the Art of Zen...: I want at least black belt 6th dan in it...)
If you cannot do so, you must accept the conclusion that the logic leads you to. I am going to be very fair to you and give you advance notice that I am now placing you in checkmate.
Whoo...
You cannot simply knock over the chess board and say this is nonsense. You need to show how and why you are not in checkmate and then show me that you can get out of it.
Just follow the logic:
1) A machine that can do more work than the work that is done on it is by definition an over unity machine.
Yes. At least in steady state. Granted. However, be very careful what is "doing work on" and "work done on it". These are frame-dependent quantities. You can of course have a machine that "does work" on something in one frame, "on which work is done" in another frame, and nevertheless find out that it does more work as per the first quantity than it receives as per the second quantity, without it being an over-unity machine. So, granted on the condition that both amounts of work are calculated in the same frame.
2) There are no over unity machines.
Granted.
3) A machine that can do more work on a tread than the tread does on it, is an over unity machine.
No, not necessarily. You have to find out if there are other contributions. Otherwise, the motor driving the treadmill is an over unity device. But the electric grid does work on the motor, so this is not a problem in this case.
4) There are no over unity machines.
Granted (second time).
5) From 1 - 4 : a machine that has work done on it by a tread cannot do more than that amount of work on the tread.
I don't know exactly what you mean by this. If you mean: *in a specific reference frame, the force exerted by the treadmill on the system, multiplied by the displacement of the treadmill in that frame, is the power provided by the treadmill*, yes, that's the power provided by the treadmill in that reference frame. And this power should not be larger than any work the device is doing on anything else, such as the air, *in that same reference frame*.
6) From 1 - 5 : A machine that has work done on it by a tread, but is clearly seen to be advancing on that tread in the opposite direction to the tread cannot possibly be an over unity machine because there are no over unity machines.
Well, you can simply say: the machine cannot be an over unity device because there aren't any. And the first part of your sentence is not related to this, nor to 1-5.
7) From 1 - 6 : The cart is being powered by the tread. It is also advancing on the tread in the opposite direction to the tread. The cart is not an over unity machine.
Well, whether the cart is powered by the tread or not is dependent on from which frame you look upon it. In the frame of the tread, it isn't, of course. Because "powered by" means: has a positive value of "the product of force exerted by and displacement by". But as in the frame of the tread, the tread is not moving, the displacement is 0, and hence it is not doing any work. In the frame of the ground, this might be the case, if the force exerted by the treadmill on the cart is in the same direction as the movement of the treadmill.
8). From 1 – 7 : Since the cart is not an over unity machine, but it is advancing on the tread in the opposite direction to the tread and it is being powered by the tread it cannot possibly be working against the tread.
Not at all. This is wrong. The treadmill can exert a force on the cart in the same direction as it moves, and that is then the power given by the treadmill to the cart *in this frame*. And this number depends on what frame one uses.
The state of motion (position and velocity) of the cart wrt the treadmill is independent, a priori, of the direction and magnitude of the force that one can exert on the other. Moreover, the statement "moves in the opposite direction as the treadmill" is also a frame dependent quantity. In the airplane that flies by, both move in the same direction.
Because if it were working against the tread , due to being being worked on by the tread , it would be doing more work on the tread than the tread is doing on it which means it is an over unity machine and they do not exist!
No, that's wrong, for several reasons, but the main reason is this: the exchange of power is not only with the treadmill, and, as I said before what exchanges power with what is frame dependent. You can do the balance in any frame, and as long as you stick to it, things will come out all right. But when you switch frames during the calculation, you will make errors.
In the frame of the tread, the tread is NOT doing any work on the cart, and the air is doing all the work. That means: you calculate the total force exerted on a certain mass of air, and the displacement that goes with it, you multiply and that gives you the amount of energy (in the given time lapse) that the air has given to the system. As the treadmill didn't move in this frame, it can't give any energy.
In the frame of the air (= frame of outside ground), the air is not moving and not doing any work, and the treadmill is doing all the work. Now, in this frame, the treadmill is exerting a certain force on the cart, and undergoes a certain displacement in doing so, hence delivers an amount of work to the system. That's the power that is available. It doesn't matter at what velocity the cart is moving, the power that is extracted from the treadmill is the velocity of the treadmill here (in the ground/air frame) times the force it exerts on the system. It is this amount of power that the motor of the treadmill will have to deliver.
In the frame of the cart, the treadmill is moving (faster than in the previous frame btw). So in this frame, the cart receives energy from the treadmill (a larger number than the number calculated in the previous case), but has to spend also energy with the propeller on the air.
Now, the erroneous objection might be that in *this frame* (the cart frame) the cart receives more energy from the treadmill than the treadmill delivered *in the ground frame*. So did there go *more energy* in the cart than the treadmill actually delivered ?
No, the error here is that we are using energies calculated in two different frames, and we shouldn't use them in the same balance. It is an error that is easy to make. It is the one I pointed out already several times.
It is even more confusing. Let us place ourselves in the ground/air frame. Now, there's something weird. The treadmill is going at velocity v1 and is undergoing a force - F by the wheel (v1 and F positive numbers). So it is "receiving" power from the cart v1 x (-F), or in other words, the treadmill is DELIVERING the power v1 x F.
The air is still and is exerting a force F on the cart (as the cart is in steady state, there's no net force on it). However, the air being steady, there is no power delivered by the air to the cart.
The cart is going at a velocity v2 in the opposite direction as the mill (v2 positive number).
So the cart is delivering a power F x (v2) to the treadmill and is receiving power F x v2 from the air.
Now, note that it is extremely confusing that what the treadmill is giving to the cart, is not what the cart is receiving from the treadmill, and that what the air is giving to the treadmill (nothing) is not what the cart is receiving from the air.
That is because we used an abuse of language. It is not because we have a force, and its reaction, that the displacements along them are equal, in a random reference frame. So a force F and its reaction -F do not correspond to individual power balances because the v1 of the point where F acts, and the v2 of the point on which -F acts, doesn't have to move at equal velocities ; hence F x v1 will in general not be equal and opposite to - F x v2.
So the abuse of language has been to take couples of "action / reaction" and to call the associated powers "the power given to ... " and the "power received from".
Newtonian mechanics doesn't require a detailed power balance for every interaction individually, but it does require a power balance overall.
And that's ok here: power balance of the treadmill: lost v1 x F.
power balance of air: 0
power balance of cart: delivered F x (v2), received v2 x F.
The power balance of the cart is actually trivial in the steady state, as the total force on it is 0, so it is normal that the total amount of mechanical power received by it is 0. If the system were not steady yet, there would be an effect: the acceleration of the cart would make for a positive power balance which is going into the kinetic energy of the cart.
So we have that the overall mechanical power received by the system is - v1 x F + 0 + v2 x F - F x (v2) = -v1 x F < 0 as it should be. Energy balance is ok: in the steady state, the entire energy delivered by the treadmill (the only external source of power) is dissipated.
If the total balance would have been > 0, we would have had an over-unity device.
So far from being an over-unity device, this thing is just dissipating the power of the treadmill, which is obvious, because once steady state is reached, no energy is stored anymore in the system, no power is done by the system on anything, and the treadmill is delivering power to the system (in the frame of the ground). So whatever is pumped into it, is dissipated.
Now, this amount of dissipated energy IS a frame-independent quantity. However, the *source* of it is dependent on the frame. Let's redo the exercise in the frame of the treadmill.
Here, the cart is moving at (v1 + v2), and the air is moving at v1, both in the opposite directions as the treadmill was moving in the ground frame. Let us call "forward direction" this direction of the motion of the air and the cart. (in this frame, they move in the same direction, v1 and v2 are positive numbers).
Now, in *this* frame, the air is exerting a force F on the cart in the positive direction, the air is hence undergoing a force -F, and the work done on the air is v1 x (-F) ; in other words the air is DELIVERING power to the system here, and that amount of power is v1 x F.
The cart undergoes a force +F by the air, and is undergoing a force -F by the treadmill. Hence the cart receives a power (v1 + v2) x F from the air and delivers a power (v1 + v2) x F to the treadmill (but we know again that this "to this" or "to that" is just indicating where the force is coming from, and isn't a power balance). Again, we could also have said that because the total force on the cart is 0 (steady state) that the cart doesn't receive or do any work overall.
The treadmill undergoes a force +F by the cart. As it is not moving in this frame, however, it is not delivering any work.
Overall balance: power received by all components: - v1 x F + (v1+v2) x F - (v1 + v2 ) x F + 0 = - v1 x F.
Total balance negative, this is what is dissipated. It is again equal to v1 x F.
Third way of calculating: the frame of the cart.
Here, the air is moving at velocity v2 and the treadmill is moving at velocity (v1 + v2), both in the sense of the motion of the treadmill in the frame of the ground. Let us call this direction positive.
The air is undergoing a force F in the positive direction. It is hence RECEIVING the power v2 x F.
The cart will again give a 0 balance, this time for two reasons: total force = 0, and on top of that, velocity is 0.
The treadmill is undergoing a force F in the negative direction. So it is DELIVERING the power
(v1 + v2) x F.
Total balance of received power: v2 x F - (v1 + v2) x F = - v1 x F.
Again, this indicates that the total power dissipated is v1 x F.
You see that no matter what frame one uses, we come out all the same. However, we see that the individual contributions of treadmill and air are different according to the frame in which we do the calculation.This comes about because in steady state, if there were no dissipation, the force F would actually be 0 when steady state would be reached. This would be (in the frame of the cart) when the propeller is not delivering any work anymore to the air (that is, when v_out would be equal to the apparent headwind velocity), and if dissipation-less, would hence not require any power from the wheel, which would then be rolling totally freely over the surface.
First definitive conclusion: From 1 – 8 : The cart is being powered by the tread. It is advancing on the tread in the opposite direction to the tread. The cart is not an over unity machine. The cart is not working against the tread.
I think I explained you why it is not correct.
If you accept (and you have no choice) that the cart is not working against the tread, then you need to justify why you insist on measuring the velocity with respect to the tread.
First of all, it is not right that the cart is not "working against the tread" in any frame. But second, I can measure a velocity wrt to anything I like. So your statement hasn't head or tails (let alone follows from any logical deduction).
If you can justify that, you would also be saying that the velocity of a sailboat can be measured with respect to the wind which is pushing it.
Of course it can. That's actually what is most easily done with an anemometer on the boat.
You would get some very low numbers because the boat is moving in the same direction as the wind.
yes.
And the reason you are getting high numbers for the cart velocity is because the tread and the cart are moving in opposite directions and you are measuring the velocity of the cart with respect to the tread.
yes.
In both cases, sailboat and cart, the only CORRECT approach is to measure the velocity of the vehicle with respect to the interface it is moving against.
This is a nonsensical statement.
Since you have displayed a disturbing tendency, when cornered, to simply dismiss even the most logical presentation as mere gibberish, I now openly challenge you to go through the above presentation and show where you feel it is wrong. You like chess?
I do.