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...Interesting. It only seems that way of course because the dot isn't an actual object, just a point where a stream of photons are hitting and being reflected, and those photons already emitted keep going after the source of them is turned away.
But it still makes some neat turns on perceptions. Like you said, the dot being in two places at once. Or the beam of light; how fast would it be moving as it swept through space if you measured it from, say, a lightyear out? |
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I would like to get ahold of that laser. |
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The moon's shadow travels at the speed of light, but when the earth enters the moon's shadow, it feels it instantaneously.
This is applicable to the speed of gravity. Van Flandern says that gravity is faster than c, but I think he's thinking of this phenomena. See the book "Pushing Gravity". |
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you sure the laser is hitting the moon and not just bouncing off the ozone layer or something? cos i dont think you would see the reflection of the laser on the moon (unless it was a very big lazer)
you could see it if it was the death star lazer through _________________ the guy that has come from mars, for no reason (no reason, or you think for no reason......) <font size=-1>[ This Message was edited by: Martian Jim on 2002-05-03 05:48 ]</font> |
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Moon, definitely moon.
Hey, this is my gedanken. Like I said, I'd like to get ahold of a laser like that. OTOH, we do "see" reflections on the moon from lasers on the Earth. But our seeing is done with instruments. Us pitiful humans have always tended to need a little help seeing, especially after forty. |
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Yeah? I did try to make a little scents
out of the Lunar Range data from http://almagest.as.utexas.edu/~rlr/mlrs.html but gave up on that. Made no centss to me whatever NOW about Gravities "SPEED" I think Gravity "WAVES" travel at whatever speed they feel like {kind of like cars on a freeway} Slow, Fast, and in different sizes & shapes so theres a broad spectrum of the on many paramaters. THEY are not one Size, one Shape, or one speed. So they are not easily detected. BUT IT IS POSSIBLE !!!!. |
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I understand that your contention is that gravity is a result of mass shadows, but what do you mean by the shadow travels at c, in terms of mainstream physics.
Do you mean that when an object moves into position, the light that has already passed it is not obstructed, and the shadow won't appear until the last particles have arrived, which will be at a rate c over the distance to the shadow? |
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Yep. The shadow is just a "hole" in a field of light. So it travels at c. Another way to look at it (no pun in 10, dead)is to consider the edge of the shadow. It is light. As the body moves the edge of the shadow moves at c.
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Just to fill in the details of the original post, per request, and to check my work, I'll walk through the algebra.
The "paper" is 3 meters away, and 400,000,000 meters long, and we'll use a speed of light of 300,000,000 meters per second. I turn one quarter turn in one second, but the photons creating the spot on the moon don't start their motion until 4 x 10^8 m / 3 x 10^8 m/s = 4/3 second later. I said it would be 1.3 seconds. I am assuming that there is a 3 meter "wall" on the moon also, but that's nearly inconsequential. Still, for time t from 0 to 1 second, the "dot" appears on the paper at time T = t + 3 meters / sine(t x pi/2) / c In that formula, t represents the time taken to turn the beam, and t times pi/2 is the angle which has been turned. 3 meters divided by the cosine of the complement of the angle (the cosine of the angle) is the distance that the photons will have to travel. Divide that distance by c the speed of light to get the time when they hit the paper. When do the photons first hit the paper? We want to minimize T = t + 3 meters/c / sine(t x pi/2). The derivative of T with respect to t is 1 + 3/c x (-pi/2) cosine(t x pi/2) / sine^2(t x pi/2) Setting that equal to zero, to find a minimum, and substituting (1 - cosine^2) for sine^2, and solving the quadratic, we get t = 2/pi x arccos((sqrt(4 + (3pi/2c)^2)-3pi/2c)/2), or about 80 msec. Did you guys get that too? |
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That's what I got, after muddling around for a long time. I didn't do anything as elegant as using derivatives, minmax and the quadratic equation...I just set up a loooong spreadsheet and found the point where d went to 3. It surprised me. I had expected to see the first 'touch' materializing much higher. Allowing for travel time back down to the observer, the differences become quite substantial. As to the spreadsheet, I haven't used one for trig before and was irked at first to see that it wanted the angles in radians, and then relieved that all I had to do was use "radians(90*t)". Thanks for the diversion!
<font size=-1>[ This Message was edited by: roidspop on 2002-05-08 14:03 ]</font> |
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Here is a related topic. If the stick was infinitely rigid, then it would work, but we know of no such material(unless nutronium-the stuff of which neutron stars are made of- would fit the bill)
A notch in a pair of scissors could go faster than light if the scissors were long enough. As the notch(the point at which the two blades meet) gets farther away, it accelerates, so it could potentially go extremely, extremely fast even if the actual molecules of the scissors did not go faster than light. I have heard it argued that matter goes faster than light where black hole accretion occurs. It is argued that the jets that come out of the "poles" of the accretion disk accelerate to a speed greater than c. A wheel of an infinitely rigid material could go above speed c, but relativistic effects in that case would be *REALLY WIERD*. The circumference of the circle would end up being imagionary, and it's area would be complex! The edge would somehow curl into another dimention in order to be imagionary!
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-----BEGIN GEEK CODE----- Version: 3.1 GCS/GM/GS/MU d- s+:+ a--- C++ U--->+++ P--->+++++ L+>+++++ E? W++ N? o? K? w+>--- O? !M V? PS !PE Y+ PGP t+(t++)>+++ 5 X+>++++ R tv+ b+>++ DI++ D+ G++>++++ e>+++ h! !r y? ------END GEEK CODE------ |
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Let's say, hypothetically speaking, that we had a pair of scissors 1 AU long. And in the "notch" where the blades intersect, there is a post. The post sticks down into the notch. Then we close the scissors. If we do it fast enough, can we accelerate the point where the blades intersect--and thus the post--faster than c?
Get NASA on this, stat!
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PC load letter? What the @%$# does that mean? |
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It's okay for mathematical points and quantities to move faster than light speed. For example, the phase velocity of the components of quantum wavefunctions usually travel faster than light speed. This isn't any big deal though, because it's the velocity of the wave packet that really matters. Hmm.. matters.. I just made an unintentional pun.
By the way, I really liked that earth-moon paper strip idea. If it weren't pointed out to me I probably would have said that the dot moves towards Earth. (Something else like that): If you had a bunch of targets placed at one-lightsecond intervals, you could shine your laser at the back one, then after a second, switch to the next closest one, then after another second, the next ... You could be "simultaneously" shining your laser dot on as many things as you liked. [img]/phpBB/images/smiles/icon_smile.gif[/img] Alternately, put reflectors up instead of targets, again one lightsecond apart, but switch to the closer one every two seconds. Then you would be blasted by many laser beams all at once. |
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[edited for spelling error: it hurts my eyes] <font size=-1>[ This Message was edited by: Fruh-Batz on 2002-10-24 07:47 ]</font> |
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This has been discussed herebefore. |
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Just imagine a pair of closed scissors that are finely machined so that the point at which the blades rotate is very close to the line where they meet. When you open them, the "notch" travels from the far end of the scissors to the close end. A better way of looking at the problem, so we don't get bogged down in whether the material is rigid enough, is to use a pair of blades that are rotating already. At some time, they are perfectly parallel, and in the next instance the "notch" travels from the ends to the axis. Nothing physical moves from end to axis, but the conceptual object does. |
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OK, ok. Right. I was thinking of somebody pressing together the handles and the scissors moving in response to it. When they are already in motion, that's something else. It seems that you cannot move any information faster than light from A to B. In the case of the entangled particle pair you can infer something about another system, but you cannot use that information. Is this right so far?
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However, shadows easily travel faster than the speed of light. Say you have an extended light source that starts at a source of 10 meters and ends up projected across a screen that's a lightyear across. Now use a well shielded blocker (that won't be upset by the brilliance of the source radiation necessary for the signal to show up on the screen) and move across the source at a leisurely pace of 1 m/sec. The projected image will have the shadow travelling across the screen at one tenth of a lightyear per second. Note that you could not do this experiment with any sort of physical object, like a rod, that stretched to the screen. If you tried to move your end of the object at 1 m/sec you'd have to overcome tremendous torque that would end up rupturing any system with an arbitrarily large binding-energy at the point where the tangential velocity equalled the speed of light. |
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<font size=-1>[ This Message was edited by: Chip on 2002-11-12 16:49 ]</font> |
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