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Scenario in an attempt to understand relativity 
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#1
Mar1911, 09:38 PM

P: 158

Greetings,
I am trying to figure out how that can be that everyone can measure all light from any source to be the same speed no matter the speed of the measurer or the source. It seems that the photons would have to be in different places depending on where the person doing the measuring is and at what speed they are traveling. What would happen in this scenario: If a year after a photon is emitted, there is an object, which is stationary relative to the source, a light year away in the path of the photon, then the photon will be there and be absorbed. And the light will seem to have taken one year to travel one light year. Correct? Now, if instead, a year after the photon is emitted (according to clocks at the source and first object), there is an object which is moving (relative to the source and first object) and therfore experiencing time dilation (relative to the source and first object), in the same place as the first object, will the photon be there and be absorbed? Since clocks would be running slower for that object, it would measure the light to have taken less time to travel the light year. So it seems that it would *not* detect the photon. It seems that the second object would have to be in a different location to detect the same photon that the first object would. It seems that whether the photon is at a location depends on the relative speed of an object that would be there to detect it. Thanks 


#2
Mar1911, 09:51 PM

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#3
Mar1911, 10:00 PM

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When we talk about everyone measuring the speed of the same light burst (I'd rather talk about a bunch of photons because, as you pointed out, if you're talking about a single photon, as soon as it gets absorbed by one observer, it ceases to exist and cannot therefore be observered by anyone else), we are always talking about a round trip (another thing a single photon cannot do) involving reflection from a mirror a measured distance away. Each observer will have their own mirror and so there are two different reflections. The time it takes to go from an observer to his mirror and back to the observer is what is used for that observer to calculate the round trip speed of light. A second observer moving with respect to the first will do the same thing with a different portion of the light and because his ruler is contracted and his clock is running slower will calculate the same speed for the round trip of the light.



#4
Mar1911, 10:46 PM

P: 158

Scenario in an attempt to understand relativity
I mean for the second object to be moving perpendicular to the path of the photon from the source, and to cross the path at the location of the first object when the first object's clock would indicate one year had elapsed. So the second object would be at the same location as the first at the same time (according to the first's clock) and without Lorentzcontraction in the direction of the photon source. 


#5
Mar1911, 10:49 PM

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#6
Mar1911, 11:04 PM

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#7
Mar2011, 03:14 AM

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You're conflating many different concepts here which makes it very difficult to address your concerns. I think what you want to know is how time dilation and length contraction work to cause a moving observer to get the same answer for the speed of light when the light is traveling either perpendicular or parallel to his direction of motion since there's no length contraction in the first case but there is length contraction in the latter case. Is that correct? But I'm not sure you understand either of these two cases, is that correct?
You're also talking about the light starting at one source where there is no observer, and traveling for one light year before it arrives in the vicinity of an observer who is stationary to the light source and another observer who is moving with respect to the light source. And you want to use the time that it takes for the entire trip in your measurement. And you want to use a single photon. And you want the second moving observer to travel perpendicular to the path of the photon. All this makes for a very difficult, if not impossible scenario to discuss. I'm not even sure how to configure what you have in mind. I already mentioned the problems of using a single photon: 1) A single photon cannot be observed by two different observers. 2) A single photon can only go in one direction. So can we please not talk about a single photon and instead talk about a flash of light? I already mentioned the fact that a measurement of the speed of light must involve a round trip and the observer has to be located at the start of the trip and at the end of the trip. So your idea of light starting a lightyear away where there is no observer and using that distance and the time it takes for light to travel that distance is not a measurement. To make a measurement of speed, you have to have a ruler and a stop watch and you calculate the speed by dividing the total distance by the total time. These are ideas the Einstein discussed in his 1905 paper where he introduced Special Relativity to the world. We would be wise to follow his example. So can we please change your scenario into something more conventional? I suggest that you consider a very popular Special Relativity issue, which is sometimes called a paradox. It goes like this: We have two observers, I, George, will be the first one and we'll assume that I'm stationary and I have a flash bulb that I have arranged to be energized when you, the CosmicVoyager traveling toward me in a straight line at half the speed of light arrive at my location. You carry a stop watch, as do I, which we both start at the moment of the flash. You continue on without stopping or slowing down. The very bright flash of light will expand outward from its starting point in a perfect sphere getting bigger at the speed of light. According to Special Relativity, I will measure myself to be in the exact center of the expanding sphere of light. That makes sense, doesn't it, since I set off the light and I'm not moving? But according to Special Relativity, you will also measure yourself to be in the exact center of the expanding sphere of light and that doesn't seem right, does it, because you are moving with respect to the source of the light? But would it make sense if you were the one carrying the light source and to have set it off when you arrived at my location? Maybe, but in this case, I, too, would measure myself to be in the center just like you would. And that doesn't seem right but it really doesn't matter what the speed of the source of the light is or the speed of the observers, they all will think they are in the center of the expanding sphere of light. This can only work if the speed of light is the same for all observers, do you agree with that? So how do we observe or measure this expanding sphere of light? Well, once it has traveled away from us, we can have no awareness of its existence or its progression through space unless we place some detectors out in space to tell us when the light arrives at a given location. We could, in principle, wire up some light detectors with long wires to let us know when the light hits them but this has the disadvantage that we would have to take into account the propagation of the signal along the wire back to us. A better idea, in fact, the best idea is to place a bunch of mirrors out in space, all a constant distance away that will simply reflect the light back to us and then if we see the light arriving from all mirrors simultaneously we will know that we are in the center of the expanding sphere of light and we will stop our stopwatch when that happens and calculate the speed of light by taking twice the distance and dividing by the time. Now it's important to realize that we each must have our own set of mirrors because you are traveling with respect to me and your mirrors must be traveling at the same speed as you are. So I take my ruler and carefully place them some constant distance from me and aimed back toward me. My mirrors will form a perfect sphere. You do the same thing with your ruler except that since you are moving, your ruler is length contracted whenever it is parallel to the direction of your motion. But your ruler is the same length as mine when it is perpendicular to your direction of motion and somewhere in between for other angles. So your mirrors will not form a perfect sphere like mine will but rather a somewhat flattened sphere. However, to you it looks like a perfect sphere because you, too, are flattened in the same way. Now what happens when we carry out out test? Well it's a little difficult to describe in words so I have created a little animation that depicts what happens: http://www.youtube.com/watch?v=dEhvU31YaCw In this video, I, the stationary observer, am depicted in green and you, the moving observer, are depicted in red. Our mirrors are in yellow. The outgoing expanding sphere of light is depicted in blue and the collapsing sphere of light reflecting off my mirrors is shown in green while the collapsing sphere of light reflecting off your mirrors is shown in red. Now you will note the shape of my mirrors form a section through a perfect sphere whereas the shape of your mirrors is compressed along the direction of your motion. Now if you follow the progression of the light as it is expanding, it forms a perfect circle and hits all my mirrors at the same time which forms a perfect shrinking circle that collapses on me from all directions simultaneously, taking a particular amount of time which when divided into the total distance yields the correct measure of the speed of light. Now what happens with your mirrors? It turns out that the light does not hit all your mirrors at the same time but what does happen is they create a perfect shrinking sphere of light but repositioned to collapse on you at just the right time as required by Special Relativity according to time dilation (a lengthening of time). It's important to realize that what we see of the progression of light in the animation is not available to us as observers in the animation. We, as observers in the video only know about the beginning of the flash and the separate returns of the reflected flashes off our individual set of mirrors. Let me know if this helps you with your question or if you have any more questions. 


#8
Mar2011, 04:34 AM

P: 158

That is awesome! Thanks :)
I will think about it some more and see if it raises any questions. I took a conceptual basic physics class which focused on understanding. I wish there was a conceptual relativity class, and a conceptual quantum physics class. We know that time dilation is more than a technique to make things work out. We have actually measured it with pairs of high precision clocks. Is there a way to measure length contraction to know objects are actually getting thinner? Since density is increasing, it's gravity should be affected. You could pass in front or behind it closer to it's center since it is narrower and experience stronger gravity. 


#9
Mar2011, 09:41 AM

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Also, keep in mind that a clock is accumulating time dilation which is the reason why we can see a difference between the clock that took a trip and the one that remained stationary. Once the two clocks are brought back together, there is no more difference in time dilation for them, as they tick at the same rate. If we took a metronome (which is the ticking portion of the clock without the accumulator) on a trip and left one at home, we would not be able to demonstrate time dilation because whenever we brought them back together for comparison, they would be ticking at the same rate. If we could devise a similar instrument, like an odometer, that would accumulate length contraction of the distance traveled, then we would see that taking two such instruments on the same path at different speeds would measure different length accumulations. Actually, we can build such instruments but they have no where near the precision, stability and accuracy to demostrate length contraction, but maybe some day we will. But to me, the fact that traveling clocks demonstrate time dilation without regard to their orientation is proof enough that length contraction is also being demonstrated, otherwise, it would be possible to devise a clock that would be sensitive to its orientation and we could take two or more of them on the same trip and they would keep accumulate different times. 


#10
Mar2411, 04:41 AM

P: 158

Okay, I have run into a problem with the idea that objects get narrower the faster they move.
If I were to measure out the distances between my mirrors when I am stationary to you, and I and all of the mirrors were to accelerate together, then they should still be arranged in a circle because as the mirrors narrow, the space between them increases since they are not connected. This also got me to thinking more about what is happening when an object narrows. Objects are made up of smaller objects, and it is actually the smaller objects that are narrowing, and when when they do, the space between them increases. The length of the larger object would stay the same if it were not for the forces binding solids together, and the object should be torn apart if accelerated quickly enough. The edges of the object would undergo the most strain since they would move a longer distance toward the center. It seems like we should be able to measure this. 


#11
Mar2411, 10:10 AM

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So in your above examples, the distances between the discreet objects also length contract. 


#12
Mar2411, 10:28 AM

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And you are correct when you talk about an "object should be torn apart if accelerated quickly enough". Yes, yes, yes, but when we discuss these thought problems in relativity, we ignore all these issues that would bring us down to reality because there are so many of them and we can't do anything about them anyway. So we pretend. The only things we can actually accelerate to these speeds are atomic particles and all experiments that can and have been done support the conclusions of special and general relativity. 


#13
Mar2411, 11:09 AM

P: 158

Okay, this is what I was afraid of. It seems to me this "length contraction" idea is just a convenient mathematical correction to compensate for something we have no explanation for, made up so that things will work out in calculations so that it can be predicted how things will *appear* in different circumstances. It is not really happening. Rulers are not contracting. And space is certainly not expanding and contracting based on how fast an object is moving. So it is extremely misleading to say objects flatten the faster they go. The correct answer for how it is that the speed of light can be measured to be the same regardless of one's speed is "No one knows. We only know how to calculate what the results of measurements will be." 


#14
Mar2411, 12:08 PM

P: 789

The square and hexagon are only 2dimensional shadows of the real thing  the cube. What is the true shape of a cube? Is it square or hexagonal? Neither, its a 3dimensional object. In the theory of relativity, when you talk about the length of an object, you are talking about a shadow of a 4dimensional object that exists in space and time. Different inertial frames view this 4 dimensional object in different ways. They measure different lengths of the object, different shadows. When you are at rest with respect to the object, you see a shadow which is longer than any other shadow, its called the "rest length". Just like when you look at the shadow of a cube, the square shadow is special  no other shadow has a smaller area. But so what? Basically, Einstein realized that its all about the cube, not about its shadows. He developed the geometry and physics of 4dimensional spacetime, and explained how different inertial frames saw the shadows that resulted. This is more than saying that he just came up with a bunch of equations that worked and had no idea what they meant. 


#15
Mar2411, 12:25 PM

P: 158

*edit I thought about this some more and realize that everything including the observer would be 4dimensional objects. If that were true, why do we only see and move in three? Why are we confined to 3 axes? 


#16
Mar2411, 12:48 PM

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#17
Mar2411, 01:09 PM

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Draw two dots on the graph. These are events, like firecrackers going off, they have a fixed point in spacetime. You drop a perpendicular from those points to your space axis  that's the distance you see between the events. You draw a perpendicular to your time axis  that's the time you see between these events. Draw a perpendicular to the other person's space and time axes, that's the space and time intervals that they see between these events  totally different. Now comes the hard part  spacetime is not a Euclidean space. The distance between two points in Euclidean space is the square root of x^2+y^2+z^2 no matter what your axes are, but in spacetime, the spacetime distance between two points is the square root of x^2+y^2+z^2t^2 (x,y,z in light years, t in years) no matter what your axes are. That minus sign in front of t^2 changes things. It means that what you draw as perpendicular on your Euclidean graph paper does not represent a perpendicular in nonEuclidean spacetime. For your space and time, the perpendiculars you draw on your graph are ok, but a perpendicular to the other person's time axis does not drop below your space axis at the same angle, it goes above it by the same angle, and when you draw perpendiculars to the other persons space and time axes, they won't look perpendicular on your Euclidean piece of paper. As the other person goes faster and faster, their time axis will get closer and closer to the 45 degree line, the speed of light, and their space axis will get closer and closer to that 45 degree line as well. If you tell the other person to draw a graph of things, like you have done, they will say that the speed of light is 45 degrees on their graph too! This gives you a feel for why the speed of light is special. 


#18
Mar2411, 08:37 PM

P: 158

"If I were to measure out the distances between my mirrors when I am stationary to you, and I and all of the mirrors were to accelerate together, then they should still be arranged in a circle because as the mirrors narrow, the space between them increases since they are not connected." To which you replied, "You are correct when you say if the mirrors accelerate together, you mean that you put individual rockets on each mirror and accelerate each of them with no rigid connectors between them but if you mean they are fastened to some kind of structure and you have only one rocket that accelerates the entire structure together, then the mirrors will move closer together." If I measured them out into a circle, then accelerated and they remained in a circle then they are not in the ellipse needed to make the light appear to travel at the same speed for me as it does for you. Anyway, Janus replied saying, "Length contraction is not something that "physically" acts on objects. It means that reference frames in motion with respect to each other measure the length differently. In other words, if there are two points in space that are 1 meter apart according to you, for someone traveling parallel to the line joining them, these two points will be closer together, regardless of the fact that there is no physical connection between those points or even if there is any physical objects at those point. So in your above examples, the distances between the discreet objects also length contract." To which I replied, "Okay, this is what I was afraid of. It seems to me this "length contraction" idea is just a convenient mathematical correction to compensate for something we have no explanation for, made up so that things will work out in calculations so that it can be predicted how things will *appear* in different circumstances. It is not really happening. Rulers are not contracting. And space is certainly not expanding and contracting based on how fast an object is moving. So it is extremely misleading to say objects flatten the faster they go. The correct answer for how it is that the speed of light can be measured to be the same regardless of one's speed is "No one knows. We only know how to calculate what the results of measurements will be." 


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