ghwellsjr said:
Are you looking at the current English version of the wikipedia.org article on Time Dilation? I cannot see much of what you say you are seeing.
I don't see any mention of the word "photon" in the article and I don't see any mention of the expression cΔt'. Tell me where you are getting this from.
Yes, but a lot of it comes from my own simple proof of relativity that is just similar to the page described. In my own proof I say that the distance traveled by the photon is cΔt. Then the length in a direction that I just used as L not considering direction, so that L=cΔt. This equation suggest that you can take L/Δt and then calculate the speed of light.
ghwellsjr said:
The observer at rest does not see a hypotenuse. Where are you getting this from?.
If a photon is sent from a moving object it does in the light clock example, since the object in motion observers the photon to travel straight out perpendicular to its direction of motion. So then a observer at rest relative to this object sending the photon see's it to travel straight out along with the object in motion.
ghwellsjr said:
The section starts off by saying that the speed of light is constant in all reference frames. It doesn't say anything about calculating the speed of light. Where are you getting this from?
That is a problem I saw with the proof on the page. In making my own proof I found that the distances of the sides of the triangle on the page where not the correct size. Then I realized that it doesn't account for light being a constant speed in each frame of reference, because the variables where not correctly assigined to do so. So what I did was instead of counting the number of times the light clock ticks, I found the relation between two distances that actually measure the value c to come out correctly.
My simple proof.
An observer in motion observers a photon to travel straight out in a line a distance cΔt'. An observer at rest measures the photon to travel out at an angle along with the objects direction of motion cΔt. The observer at rest also measures the object to travel a distance vΔt. This gives three sides of a right triangle and then the relation to how they measure Δt can be found.
(ct')^2+(vΔt)^2=(cΔt)^2 a^2+b^2=c^2
c^2Δt'^2=c^2Δt^2-v^2Δt^2 distribute the square and subtract both sides by (v^2Δt^2)
Δt'^2=(c^2Δt^2-v^2Δt^2)/c^2 divide both sides by c^2
Δt'^2=c^2Δt^2(1-v^2/c^2)/c^2 factor out a (c^2Δt^2) from (c^2Δt^2-v^2t^2)
Δt'=Δt√(1-v^2/c^2) the c^2 cancels and take the square root of both sides
It then follows that the Michealson-Morley experiment also measured the photon to travel out in a straight line even though the experiment was under constant acceleration due to the Earths movement. So then, the distance traveled by the object in constant acceleration can be replaced with Δt(vi+vo)/2.
s=Δtvo+(aΔt^2)/2
s=Δtvo+(Δt^2(vi-vo)/t)/2 substitute from a=(vi-vo)/Δt
s=Δtvo+(Δtvi-Δtvo)/2 cancel a Δt from the substitution and distribute the Δt
s=2Δtvo/2+Δtvi/2-Δtvo/2 multiply Δtvo by 2/2 and separate the factor
s=Δt(vi+vo)/2 add like terms and factor out Δt
(cΔt')^2+(Δt(vi+vo)/2)^2 = (cΔt)^2 Pythagorean Theorem
c^2Δt'^2 = c^2Δt^2 - Δt^2(vi+vo)^2/4 distribute the square
c^2Δt'^2 = c^2Δt^2(1-(vi+vo)^2/4c^2) factor out c^2Δt^2 from the right side
Δt'^2 = Δt^2(1-(vi+vo)^2/4c^2) divide both sides by c^2
Δt'=Δt√(1-(vi+vo)^2/4c^2) take the square root
Then you have an equation for the relation between time dilation and constant acceleration. I noticed that by adding the initial velocity and the final velocity that you can get double that amount of velocity than just the time dilation equation alone. Then when it is squared it comes to be counteracted by the 4 in the denominator. This is because 2 in the acceleration equation is squared to give 4. So you have 4c^2 instead of just c^2, that seems to work out. But my proof seems to imply that as a velocity becomes c then the amount of time that is dialated comes to zero instead of being undefined.