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There are two cars facing the opposite directions on a road. One car takes off and travels at a steady speed of 60 MPH. After 1 minute he is 1 mile away from the other car, 2 minutes he is 2 miles away etc. At the 3 minute mark the other car starts up and travels the opposite direction at 60 MPH. At the 4 minute mark the cars are 5 miles apart and the distance between the cars is increasing at the rate of 2 miles per minute. Can I consider that either car is traveling 120 MPH ( 2 miles per minute) since the distance between the cars is increasing at the rate of 2 miles per minute?
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You can consider one of the cars to be traveling at almost 120 MPH in the frame of reference of the other car.
Almost, rather than exactly 120 MPH because of relativity, of course. The slight difference is of no practical importance in this particular case, but it would become significant at (much) higher speeds. Alternatively, you can simply make up a frame of reference in which the car is traveling at exactly 120MPH. This has nothing to do with the other car. You can choose any of an infinite number of possible frames of reference. Depending on what frame of reference you use, you can choose the speed of the car to be any value less than the speed of light. |
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MDT-1,
This had better not be yet another thread on relativity. You have now been warned twice about this. If you want to learn the mainstream answer to relativity questions, you had two threads to do that in, one of which is still open. If you are trying to promote a non-mainstream view, it needs to be in ATM. If you try to push an ATM view in this thread, you will be given infraction points.
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At night the stars put on a show for free (Carole King) One Earth, One Sky - IYA 2009 All moderation in purple |
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The RPM that the tires are turning may appear slower due to relativistic time dilation. The torque on the axle will not be affected by your choice of frame of reference. |
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Each car will be travelling at 60 mph relative to the road and 120mph relative to each other, or as near as significant. But as Isaackuo stated you can propose the car to be travelling at any speed you like less than C depending on your frame of reference. As Ken stated, you may as well change the scenario to suit, so you get the answers you are looking for regarding relativity.
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ooops..... wrong forum!!! |
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I'm going to interpret this as a thread about how relativity works at Newtonian velocity scales, which might be a useful thing because it saves us from the extra complications of time dilation and whatnot. So the questions are about Galilean relativity. Note that even in Galilean relativity, inertial motion is entirely interpretable as purely relative, there is no need for a universal frame of rest to do Galilean relativity. That is also how cosmocrazy answered it.
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You mean the question of, if I turn around and travel at 60 MPH in the same direction of travel as the other car, can I consider myself to be going 0 MPH? If he then turns around, how fast am I going?
When he brakes, my velocity goes down, or up (depending on the direction of travel)? That means if he applies a force to his car, my car accelerates? |
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You can always construct a frame in which you are going 0 MPH. It doesn't matter what other objects are doing, you'll just describe their motions relative to your position. This is actually standard classical mechanics. Isaac Newton proved that one could do this as long as any acceleration on the objects being considered was effectively parallel.
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My velocity is not dependent on any other object. It depends on the distance and time I travel relative to the light I emit. |
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A real world example (which exactly happened to me a few days ago) - have you ever been on a train in a station, looked out the window at a train on the next track, and notice that you are moving? And then realize that (relative to the track and the earth) you are perfectly stationary, and it is the other train that has begun to move? If you consider each car to be traveling at 0 MPH before he turns around, then in this inertial reference frame, you continue to travel at 0 MPH, and the other car is then moving at some speed other than 0 MPH. Even if the other car has a perfectly smooth ride, a passenger in that car who is blindfolded will still be able to tell that the speed of the car has changed. The acceleration requires a force acting on the passenger, which can be felt. If the passenger were holding a glass of water, the water in the glass would slosh around as the car changed speed. In both the physics of Newton and the more accurate physics of special relativity, there is no such thing as absolute motion. You may take the perspective of an observer for whom the earth is stationary, and the cars are moving. Or you may take the perspective of the passenger of one of the cars, and consider the earth to be moving. Or you may take the perspective of the sun, and consider the earth and the cars both to be moving. All perspectives, or inertial reference frames, are equally valid, and the laws of physics work equally well in all of them. But an absolutely critical point is that the perspective of the observer must be inertial, or not accelerating. When the second car turns around, it leaves one inertial reference frame, and enters another one. From the perspective of the reference frame the other car was in before it turns around, the first car was stationary, and it remains stationary after the other car turns around. From the perspective of the reference frame the other car enters after it turns around, the first car is moving, and was moving before the other car turns around. This is a very important point. There is no such thing as absolute velocity. There is such a thing as absolute acceleration (note to anyone reading - I think it is best to avoid general relativity in this discussion at this point). So you are free to define the velocities of all objects relative to the earth, relative to one of the cars, relative to some other car/vehicle, relative to a distant galaxy, and the laws of physics will work perfectly well from this perspective, provided the reference frame you choose is not accelerating. Once it accelerates (changes velocity), as in the case of the car that turns around, all bets are off. If he applies a force to his car, his velocity changes. Your velocity remains the same in the reference frame his car was in before, and your velocity remains the same in the reference frame his car was in after he applies braking or some other force. So it may seem that there is action at a distance, in that the acceleration of the other car also accelerates your car, but to come to this conclusion, you have to take the perspective of a reference frame that is accelerating. And that's a big no-no.
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But in either of those physics, there is no such thing as "My velocity." There is only your velocity relative to other objects. I don't know what you're doing right now, but are you remaining still, with a velocity of zero? Are you perhaps traveling in a plane, train, or automobile, at speeds somewhere between 10 and 1,000 km per hour? Or are you rushing through space at 100,000 km per hour, because you are attached to the earth which is orbiting the sun at a very high rate of speed. Which of these is "My velocity"?
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"My velocity" is not dependent on the sun , the earth, or the moon, it is dependent on the light I emit. If the light I emit is equal distance away from me at all times, then I am a zero velocity.
Sure, we can refer to roads, moons, suns, etc, and relate our motion to those objects, but that is relative motion, not actual velocity. A zero velocity is that of which the light is equal distance away from me in all directions for any given time interval. |
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Always true. So, without other objects, how do you know?
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Numbers are not case sensitive. (me) |
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No, because after objects emit light, if they have a velocity, they are no longer the center of the light sphere.
If the sun emits a sphere of light, if it were a zero velocity, the sun would stay in the center of that sphere. If it emits a light sphere, and then travels a distance, it is no longer in the center of the original light sphere. |
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So what is your velocity right now?
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Principal Principle Offender |
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This issue was resolved roughly 100 years ago.
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Principal Principle Offender |
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The earth does not stay in the center of its own light, it has a velocity.
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Yes it does. This has been confirmed many times.
Have a look here, for example. By the usual definition of "velocity," it does. By your definition, which bears no resemblance to the normal definition, it doesn't. If you want me (or anyone else) to just throw away the wealth of empirical evidence against what you are claiming, I think you're going to have to offer some evidence.
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Principal Principle Offender |
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MDT-1 As has been pointed out this is a forum for asking questions and getting answers from the Mainstream of science. IF you don't agree with the Mainstream answers and instead want to suggest your own answer which is against the Mainstream then you need to start a thread in the ATM forum.
Check out the rules for posting linked at the bottom of this post. Consider your next post very carefully.
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First of all, that is not what the object sees. Second, even an outside observer will not see the cross hairs outside of any circle because that would imply the object is moving faster than light.
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Numbers are not case sensitive. (me) |
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MDT-1, from your post #18:
”If the sun emits a sphere of light, if it were a zero velocity, the sun would stay in the center of that sphere. If it emits a light sphere, and then travels a distance, it is no longer in the center of the original light sphere.” From your post #20: Quote:
http://imagine.gsfc.nasa.gov/YBA/M31...s/doppler3.gif Notice that the light emitter is not in the center of the earliest expanding light spheres that it emitted. It’s the third illustration down on this NASA webpage: http://imagine.gsfc.nasa.gov/YBA/M31...r-shift-2.html See the caption: ”You will recognize it as the same as the fire truck approaching the stationary observer except now the source is emitting light instead of sound. Notice that the right region where a perceived increase in the frequency is noticed is referred to as "blueshifted", and the region which would appear to be of a lower frequency to an observer on the left is referred to as "redshifted."” In this illustration, the background space would act like a light-speed-regulating “medium” or an “ether”, such as the way the air acted as the sound-speed-regulating medium in the example with the moving fire truck. However, this drawing doesn’t conform to the results of the Michelson-Morley experiment, since they found no evidence of such a “medium” or “ether” at the surface of the earth where their experiment was performed, so there might be some doubt about the validity of this NASA illustration. My opinion is that no one knows yet how to illustrate what really happens. |
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But you may be right, that it is hard/impossible to give a realistic representation. |
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The source changing position after the light sphere was formed has nothing to do with the rate at which the original radius expands. The radius expands at the rate of ~186,000 miles per second from the original point of emission, regardless if the source is at that original point some time later or not.. |
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