jay t said:
Thanks guys for all the responses.
I realize that however i phrase the question, you will all find things which i may have missed. Therefore I will explain it one very last time (while trying to plug all the relativity holes I may have missed). If this is still explain by relativity, then i will give up and just study the theory more until i get it. Here goes.
In the image below we have
3 Scenes. I will explain the scenes, then tell me where I am wrong in my logic.
Scene #1
We have a stationary laser gun, 7 miles away from a computer ( computer which measures the time that the laser hits it). Assume, that the laser takes 5 seconds to hit it. (
please these times/scales/distances are not drawn to scale, so no nit-picking please

) .
Scene #2
We have the same scene, only this time, the Computer is mounted on a truck that is traveling away from the laser-gun at 4600MPH. My assumption here is that the laser will take a longer time to hit. Let's say this takes 7 seconds (not drawn to scale please). The laser is first fired at the same 7 miles mark. The truck began moving at 4600mph the very same time the trigger was pulled. (please no talk about the 0-4600mph acceleration.. remember this is a thought experiment..)
All ok with the the first 2 scenes? good...
Scene #3
We have a crazy setup. A mobile truck with an attached laser-cart is speeding toward the start line. When both lasers are aligned with the start line, they are both fired at the same time. Assume that we have the firing of both laser-guns done at the same time. So we have
1) Guns fired at same point (7miles), and at the same time
2) Lasers traveling through the air (light is constant speed) uninterrupted by speed of truck or air resistance.
3) There is only one observer -> The computer whose sole purpose is to determine while laser hit first.
View attachment 212332So from the computer's perspective, will both the yellow and the orange laser take the same time to hit? or, will the yellow laser have 5 seconds while the orange have 7 seconds (even though they are fired from the
same distance and their end point is moving away from them)?
Let's see if I can shed some light on this(pun intended).
I'm going to take this scenario, with just a couple of modifications. 7 miles and 4600 mph are really too small of figures to work with when dealing with relativity. ( light would only take 0.000037634... sec to travel 7 miles and 4600 mph is such a small fraction of c,that the effect we are looking for would just be too small.
So let's make the distance 10 light seconds or ~3,000,000 km, and the relative velocity 0.6c (this particular value gives a bit nicer looking numbers in the example)
So to start off, we can use this diagram for Scene 1 and scene 2, with the difference being that for scene 2 the sensor/computer is moving to the right at 0.6c. The lined box is a ruler resting on the ground marked off by 1 ls segments.
Scene 1 is easy to analyze since both the laser gun and sensor are at rest with respect to each other. Thus we can say that the laser light takes 10 sec to reach the sensor, whether it is according to the ground or the computer.
Scene 2 is a bit different. First we have to establish from what frame this image is taken in. Since we are basically using the same image as we did for scene 1, we will assume that this image also taken from being at rest with respect to the ground and ruler. Thus when the moving computer is 10 ls away from the laser cannon(at the end of the ruler) the laser fires. If we ask how long it takes for the laser to reach the computer, we have to take into account the distance between cannon increases after the cannon is fired and the light has to catch up to the receding computer. It works out that, with a relative velocity of 0.6c, it would take the light 25 seconds to hit the computer. That is how long it will take according to someone on the ground.
You are interested in how long it will take according to the computer. The thing to keep in mind, it that as far as the computer is concerned, it is the cannon that is receding from it. Thus what happens to the cannon after it fires has no effect on how fast the light reaches the computer. All that counts is how far apart they were when the cannon fired. At first, you might think that since they are 10 ls apart when the cannon fires, 10 seconds should pass for the computer between firing and reception of the light. However, the distance between the two is only 10 ls according to someone measuring the distance while at rest with respect to the ruler on the ground. Relativity says that frame with relative motion to each other measure distances differently. This is commonly known as Length contraction. what this means is that the computer and ruler on the ground each measure the length of each other as being contracted. At 0.6c this contraction factor is 0.8. So while the laser cannon and the ground ruler itself measure the ground ruler as being 10 ls long, the computer would measure it as being only 8 ls long.
So according to the computer, when it is even with the end of the ruler, things look like this:
and it is only 8 ls from the cannon (Note that the computer box itself is not a square in this image. This is because the square you see it as above for scene 2, is because it is length contracted according to the ground frame. This also means that technically I shouldn't have used the same image for scene 1 and 2, as for in scene one the computer was at rest and would not have been shown length contracted to a square. I just didn't want to confuse you with drawing it that way before I brought up length contraction.)
From this image it might appear that we can now say that it takes 8 sec for the light from the cannon to reach the computer as measured by the computer. Alas, we can't do this either. The problem is that while this shows the moment that the computer reaches the end of the ruler according to the computer, it is not the moment the laser fires according to the computer. (This is where the Relativity of Simultaneity brought up by other rears its head.)
To figure out when the laser fires according to the computer, we need to ask how does the laser know when to fire? We know that it is when the computer reaches the end of the ruler, but how does the laser know when this happens. A signal can't be sent back from the end of the ruler, because it would get to the laser until after the computer is well past the end of the ruler. You might send a signal from carefully chosen point along the ruler so that the signal it reaches the laser cannon at the same moment as the computer reaches the end of the ruler, or you might use this method:
Assume the computer starts to the left of the cannon. At the moment it passes the cannon a clock at the cannon starts counting from zero. You know how long the ruler is and how fast the computer is moving relative to it, so you know it will take to reach the end of the ruler after passing the cannon. The laser clock waits until its ticked off this much time, and then fires the cannon. With the values we are using, this works out to 16 2/3 seconds. So when the clock at the laser cannon reads 16 2/3 sec, it fires the cannon.
But what does this mean as far as the computer is concerned? Now we have to consider time-dilation. Clocks in motion with respect to you tick slow compared to your own clock. At 0.6 c, this factor is again 0.8 (for every 1 sec ticked of by your clock, a clock moving at 0.6c relative to you only ticks off 0.8 sec.)
So if we give the computer its own clock that starts at zero when it passes the laser cannon, for every 1 sec that ticks off on the laser cannon clock, 1.25 sec tick off for the computer clock. (It is important to note that this is not what the computer would visually see happening to the laser clock if it were watching it in a telescope as they separated, As that would be due to a combination of the increasing distance the light has to travel and time dilation. Here we are only interested in the time dilation part.)
If the laser fires when its local clock reads 16 2/3 sec, and 1.25 sec pass for the computer clock according to the computer for every sec on the laser clock, then 20 5/6 sec have passed on the computer clock when the laser fires, and at .6 c it will be 12.5 ls from the laser when it fires and it will take 12.5 sec for the light to reach the computer.
This is how things will appear for the computer when the laser fires:
Notice that it is far past the end of the ruler.
Now let's consider scene 3. As before, in the ground frame, things look like this when the laser is fired:
If both laser fire as they pass each other, both laser will catch the computer in 25 sec just like in the ground frame of scene 3.
But as mentioned before, this view of the computer and its attached laser cannon are length contracted due to the relative motion between ground frame and computer.
So when we transition to computer frame, the distance between the computer and its attached laser cannon is the non-length contracted distance of 12.5 ls. And at the moment that the two laser cannons pass and they both fire, things look like this:
Note that the only difference between this and the computer frame image for scene 2 is the arm extension and extra laser cannon.
Again, since both cannon are equal distance from the computer when they fire, both lights reach the computer at the same time, 12.5 sec later.
One last point. Earlier, I gave an alternative method for how the laser cannon decides when to fire. Using that alternative method would not have resulted in any difference in the final answers.