I haven't been here for almost 2 years. I gave up trying to understand relativity because I was stuck on understanding how it differed from the doppler effect. Finally I got the answers I needed on Brian Greene's worldscienceu relativity course. The course really cleared up a lot of things for me but has lead me to a new impasse which I'll discuss below. I'm hoping someone here could get me past this latest problem I'm having. I'm not going to phrase it as a question but more like a bunch of statements that need counter arguments.
This is a physical explanation of how the relative speed of light remains constant for all frames and all observers.
In 1851, the Fizeau experiment showed that the speed of light through moving water, was not a simple sum of c'+v or c'-v (v being the velocity of the medium and c' the speed of light in water). In fact, it was found that whether the water flowed with or against the light, the result was always the same: c'+v=c'-v which always reduces to the nonsensical result of v=0. It was this experiment, and not the completely misunderstood Michelson-Morley experiment, that inspired Einstein's theory of relativity.
The Fizeau experiment was important for two reasons. First it showed that the speed of light, an electromagnetic wave, is dependent on the electromagnetic properties of the medium it propagates in just like a mechanical wave is dependent on the elasticity and inertia of the mechanical medium it propagates in. The electromagnetic equivalent of elasticity and inertia is inductance and capacitance or basically the permitivity and permeability of the medium. If light has no medium then how is its speed of propagation dependent on the permittivity and permeability of each medium? Light would be able to plough thru anything at one speed just like neutrinos do if it was not dependent on a medium for propagation. If space itself was a void, it would not have properties and to say it's not a medium because it can't support mechanical waves makes no sense because light is not a mechanical wave and space is not a mechanical medium. So the "vacuum" of space is indeed a medium and "aether" does exist except not the same as the one Michelson-Morley didn't find. The Fizeau experiment would have been difficult to do in a moving vacuum but moving water (or air or glass) shows the velocity of the medium does affect the velocity of light but not in a simple additive way.
The second reason the Fizeau experiment was important was because it hinted that the relationship between the velocity of the medium and the speed of light could be Pythagorean because the sign of the velocity was irrelevant. So, to jump ahead, c2=v2+c'2 (c squared = v squared + c' squared) where c' is the speed of light in the moving medium as seen from a reference (relatively stationary) frame. The moving frame is the one where time dilates and this difference means it's not correct to state it's physically equivalent to assign either frame as moving or stationary. Solving for c', c'= sqrt(1/(c2-v2). As you'll see later, the time dilation Y gamma factor = c/sqrt(c2-v2) so c'=c/Y. This means the speed of light in the moving frame as seen by the stationary frame is the speed of light slowed by a factor of gamma time dilation. This means that if you were on a spaceship traveling near the speed of light and you turned on a flashlight, the beam you would see would be traveling at the speed of light away from you but the beam the stationary platform would see would be leaving the flashlight very slowly. However, the relativistic combination of the spaceship's velocity and the slowed light beam would equal the same speed of light as on the stationary frame . The velocity of the moving frame dilates time by a factor of gamma slowing the speed of the light beam on the moving frame when seen from the stationary frame such that the combination of the velocity and the slowed light will equal the speed of light where c=sqrt(v2+c2/Y2).
This is difficult to understand because the speed of light on the moving frame is c when seen on the moving frame but is c/Y when seen from the stationary frame. But when that slow light speed is combined with the velocity of the moving frame, using the formula c=sqrt(v2+c2/Y2), then the constancy of the speed of light over all moving frames is preserved (this is not how Einstein interpreted the constant velocity of light for all inertial frames).
I know I keep repeating myself but let's try to look at it from another angle. Take a graph where the dilated time frame t' of the moving frame as seen from the stationary frame is the y-axis and velocity of the moving frame v is the x-axis. At v=0 of the moving frame, the speed of light seen from the stationary frame and the moving frame will be c. Y will equal 1 so c/Y will equal c; no time dilation slowing down c. At the other extreme where v=c, c/Y will be zero and time will stand still for any forward light beam which can't move forward at all. This graph shows time and the light beam is slowed as the velocity of the moving frame increases. Remember, light is not a moving frame of reference, it has a frequency and is therefore a clock and it propagates on a frame but is not itself a frame (also probably not in agreement with Einstein.)
In an intermediate case, when v=c/2, the c/Y component will be c/1.155 or .866c. Just to check that total c is preserved in the moving frame when viewed from the stationary frame, c=sqrt(.25c2 + .75c2) = c but the relative speed of the light beam itself, not helped by the moving frame and slowed by time dilation, is only .866c. But since it's relative to the moving frame, it will be seen at velocity c from the stationary frame and by those moving with the moving frame.
It's important to note that the orthogonal velocity on a moving frame is zero to the stationary frame just as if the stationary frame was riding along attached to the side of the moving frame (as it was in the Michelson Morley experiment). This means light is seen to spread out sideways at full speed even though its frontal speed is slowed on the moving frame when seen from the relatively stationary frame. It also means that any sideways motion within the spaceship would look like normal speed to the stationary observers while any forward motion would greatly slow. So the forward parts of the passengers would also age slower than the side parts and just turning one's head would change one from moving at high relative speed to zero speed relative to a stationary observer. In a moving 3D frame, only 1 dimension is moving and the other two are stationary with respect to it even though they are moving alongside with it.
Remember, all of these acrobatics is to preserve the speed of light in all frames in any direction regardless of the frame of reference. To me this indicates that linear velocity is the 4th dimension and not time. All components of a 3 dimensional space that move at the same velocity share the same time. In fact, all low speed 3 dimensional spaces share pretty much the same time. When we will work out how simultaneity works, we'll see that even when two frames are at vastly different speeds, a universal present is shared at different spacial coordinates and shared universal spatial coordinates have different time coordinates. This means a ship traveling near light speed will see a supernova flash at the same time as earth sees it even though the ship is far closer to the supernova. Any other planet that the ship may be passing over will have already seen that same flash in the past even though they're at the same location as the ship.
This is not at all how Einstein saw it; no universal simultaneity or shared present time between moving frames. I'm saying the shared present time is shifted to different spatial coordinates and shared spatial coordinates will not see the same events happening simultaneously between the moving frames. The difference in the interpretation stems from Einstein's statement that a forward moving frame will see light before a stationary frame sees it and I'm saying that a forward moving velocity cannot add to the relative speed of light and hence it cannot get to the moving observer faster than the stationary one.
When anything such as a spaceship moves, it may also move an entire 3d coordinate universe where all objects within that universe share the same velocity. We know space is a medium for light because it has permitivity and permeability and light changes its propagation velocity based on different permittivity and permeability values for different mediums. The light wave moves through that medium like any other wave would move through its medium. So let's see what that would look like if we considered a flatbead train hauling a whistle (sound wave comparison).
Air is the medium. The train has a relative velocity to the still air and if you were riding on the train you would feel a breeze as if the train was stationary on a windy day. The whistle would not see it this way. The train velocity would not be able to push the sound velocity, only compress its frequency producing a doppler effect. The sound velocity is constant through still air because that's what its velocity is relative to; not the train speed. The sound velocity would be affected by a true breeze where the air actually moves and not by a wind caused by train movement.
Now suppose the train is encased in glass and an observer could see the sound wavefront inside. At that point, the sound would move with the still air inside the train and hence its relative velocity to the outside world WOULD be affected by the train velocity. Replace the sound with a light beam and relativity would kick in to prevent the train velocity from forcing the light velocity through air to surpass the light velocity through space.
Although relativity guarantees light speed is maintained whether in a open bed train moving through still air, moving air, or an enclosed train with still air inside it or even if the entire platform was attached to a moving train (i.e. the Michelson-Morley experiment), it's important to understand the subtleties of relative motion in all these examples.
The forward and backward wave fronts of a light flash in an open train moving through still air would not be affected by the movement of the train like those of a light flash in an enclosed train. In that case, the origin of the light flash will move with the enclosed train and the forward and backward wave fronts would be affected by the motion of the train using the relativistic velocity combination formula. Relativity would guarantee the same relativistic behavior even though the two examples look nothing alike.
Unlike light, neutrinos travel at one speed totally medium independent. That speed is so close to c that I don't think scientists have yet determined if the difference is due to measurement uncertainty. If neutrinos were used instead of light, they would behave as light in an open flatbed train and the source would not move with the moving frame. Electrons, on the other hand, have a speed dependent on the energy that frees them from the atom. They are like baseballs independent from a medium but their speed is not independent of the speed of the train platform. Hence, they would track the velocity of the moving frame whether the train was open bed or enclosed. Including little details like these really gives the math a physical perspective.
Relativity of Simultaneity
In our world, a ball thrown at a stationary person would take less time, and hence record a greater relative velocity, if the ball was thrown at a forward moving person. This is not true if the ball was replaced by a beam of light, the time would be equal and also equal for someone moving away from the ball.
Consider an open-bed train of length 2L moving at velocity v past a platform also of length 2L where 2 midpoint lights are turned on when both midpoints are directly opposite each other. One light is on the train and the other is on the platform. (The calculations for an enclosed train would be different from an open-bed train but would still yield the same results.) Even though time dilation would appear to slow the train's light beam when seen from the platform, the combination law with the train's velocity would yield a light speed of c (not c/Y) towards both ends of the train. Hence the time t' for the light on the train to hit both ends of the train when seen from the platform would be L/c. The distance that the train moves (x) in this time = vt'. Substituting in t' and x=vL/c. If the midpoint of the platform is the origin, then the coordinate (a) on the platform that a person on the platform sees the train's light hit the end of the train is -(L-x) = -L(1-v/c) = -L(c-v)/c (at the other end of the train moving from the light, the x coordinate would be L(1+v)/c). According to relativity, the time it takes for the dilated train light to hit the end of the train, is the same time it takes the platform light to hit the end of the platform.
So let's go through this slowly. The x-coordinate on the platform that a platform observer would be closest to seeing the light hit the end of the train is -L(c-v)/c. That observer would be hit by the platform light at c= -L(c-v)/cta. So ta= -L(c-v)/c2. The next event is tb where the platform light hits the end of the platform and the platform observer at point a would see the train light hit the end of the train. tb=L/c.
The observer on the other end of the train, the one receding from the light, would be stationed at point d which is at platform x-coordinate L(1+v)/c. He would also see the train light hit his end of the train at tb but he'd have to wait an additional time of td=vL/c2 for the platform light to hit him. The time the platform light hit point a was vL/c2 sooner. The platform light is what supposedly determines simultaneity on the platform so when there's a difference between when the platform light hits point a and point d of 2* vL/c2, that's the relativity of simultaneity. At point tb, observers of the train ends from the platform ends would see the train light hitting both ends of the train at the exact same time they get hit by the platform light. Hence no relativity of simultaneity from their positions. This is quite different from Einstein's interpretation.
The difference in interpretation is that Einstein believed that since light speed is the same for all reference frames that the train light would track the platform light. It does not because the two have 2 different time frames; the moving one is time dilated relative to the stationary one. The idea then that the platform light determines simultaneity on the platform is wrong even though my derivation produces the same equation for simultaneity as appears in the Lorentz transformation. The 2 observers on the platform ends will see (using telescopes) the platform light hit them simultaneously with the train light hitting both ends of the train simultaneously. How simultaneity should be interpreted is that the light source (not differentiating between the train and platform light source) hits 2 different spots simultaneously on half a platform or hits 1 spot at 2 different times with 2 really separate lights). I don't take this as being particularly significant enough to make all the wild claims that relativity makes. The only thing I feel is right about relativity is that time dilates for the relatively moving frame (which is one way to tell which frame is moving relative to the other).
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