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| Tags: relativity, work |
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#2
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On 3 Aug 2005 17:01:50 -0700, wrote:
This entire thread seems to be based on an error in calculation by dseppala. It is corrected below. wrote: On Fri, 22 Jul 2005 04:00:03 GMT, The Ghost In The Machine wrote: In sci.physics.relativity, wrote on Thu, 21 Jul 2005 16:30:18 GMT : I don't see how Einstein's length contraction notion works with this simple gedanken experiment. Very simply, I have two identical rods oriented along the x-axis. One rod I'll call rod A and the other rod I'll call rod B. The two rods have a relative velocity V along the x-axis. Well, now they're not identical, as they're in different states. However, that's an extremely minor problem. As measured in their respective frames, each rod has a length L. In Frame A (rod A's rest frame), observers according to Einstein measure rod B to be shorter than rod A. Yes, with varying amounts of shortness depending on precisely how the measurement is done. If one plays "wait for the endpoint" one gets a length-equivalent of L/g, where g = 1/sqrt(1-v^2/c^2). If one plays "pingy ping ping" one gets something else; I'd have to recalculate it. In Frame B, observers measure rod A to be shorter than rod B. Symmetry more or less requires this. Now here's the problem. Let the relative velocity of the two rods be 3 meters / second. So v = 1e-8 * c, and so gamma = 1 + 0.5e-16 to very good approximation. Let the length of the rods be very long say about 10**8 light-seconds. Let's say it is exactly 1e8 light-sec. Erm...you do realize that's a rod stretching about 74% of the way from Earth to Alpha Centauri, I hope. 10^8 seconds = 3.169 years. Yes I realize its a long length. I use the long length because its much easier for me to relate to very low velocities like 3 meters / second, and a time interval of one second because we can easily measure those values in our everyday experience. It much harder for me to relate to velocities approaching c and times that happen in less than a blink of the eye when I'm trying to understand the real physical properties of rods. Now accelerate all points of rod A at the same time (as measured in Frame A) to 3 meters / second such that after the acceleration rod A has zero relative velocity wrt rod B. And you were going to do this precisely how? The rod, in this case, has the usual torsional, flexional, and compressional problems. Also, the endpoints of the rod span a distance that would take 3.169 years for a signal to cross; even if one locates the control in the midpoint the ends won't even receive the signal until 1.584 years have passed. In this gedanken experiment, I would have a conveyer belt moving at 3 meters / second relative to the very long rod. I would have a long line of people (yes, I know its a large number) holding that rod. Then at time t0 according to their synchronized clocks, I would have them each step on to the conveyer belt while holding the rod. These people and the rod will accelerate to 3 meters per second over a very short interval (I've done this experiment with a much shorter rod - a couple of meters in length). Now prior to stepping onto the conveyer belt, I note that there is a second rod that is on the conveyer belt that has zero relative velocity wrt the conveyer belt. I note that it is composed of the same number of atoms, and is the same diameter as the rod my long line of people are holding. At time t0, when each person in the long line of people step on to the conveyer belt, the person at one end point of the rod steps onto the conveyer belt at the same position as one end point of the rod that was already on the conveyer belt happens to be. The person on the other end point must therefore step at a position that is 3 meters beyond the other end point of the rod that is already on the conveyer belt when he steps on to the conveyer belt at time t0 (Einstein's equations). No, the extra distance is about (gamma - 1)*L = .5e-16 * 1e8 = .5e-8 in light-sec, or 1.5m. Now this accelerated rod, does not remain stretched. Over time, the accelerated rod and the non-accelerated rod will have identical lengths since they have zero relative velocity and have the same diameter, and have the same number of atoms, and no permanent deformation of the rod occurs during acceleration (because the acceleration rate is so low). So the rod will eventually contract by three meters. The problem is that I cannot figure out how this process is viewed by observers who are in the conveyer belt frame. They measure the rod held by the long line of people to initally be 3 meters shorter than the rod in their frame. 1.5m When the people step on to the conveyer belt at time t0, the observers in the conveyer frame observe that the people at one end of the rod start stepping on to the conveyer belt one second before the people at the other end. Yes, 1 sec is correct here. But you see, everything works out now if you correct your earlier error. But this would make the end points of each rod coincident when each person steps on to the conveyer belt (a stretching of 3 meters). No, the physical stretch is 1.5m. And since it starts out 1.5m *shorter* (in the belt frame) than its proper length, the end must move 3m to give the required stretch. In other words, exactly 1 sec as we calculated. I think I can snip the rest. Thanks for the reply. I found a high precision calculator which also gives the result 0.5 * 10**-8 light-sec. So the problem I had was due to the calculator I used. Thank you for correcting the arithmetic. David |
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#3
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