h8ter said:
How can it have two lengths at the same time?
Because it happens to be a feature of the universe we live in that the length of an object is a function of its speed.
No, it isn't. In fact, it's quite impossible for it
not to be that way!
I know this is in regards to different inertial reference frames, but reference frames doesn't make something heavier or lighter depending on the speed of one related to another. That would make something have two different masses at the same time.
The concept of relativistic mass can be accepted or abandoned at will, but we are stuck with length contraction and time dilation. So, I'll be confining my remarks to the latter two phenomena.
A good explanation would help me understand.
It all starts with Maxwell's equations of electrodynamics. This is how Einstein derived Special Relativity from two postulates:
1. The laws of physics must be the same in every inertial frame.
2. The speed of light must be the same in every inertial frame.
The first postulate means that you should not be able to tell whether you are moving or at rest merely by performing an experiment in a closed laboratory. What it really amounts to is that there is no such thing as a state of absolute rest. Equivalently, it means that there is no preferred inertial frame of reference.
The second postulate means that, for any light pulse, its speed will be measured to be 'c', no matter what the relative motion between the source and the observer. So if a source is stationary in your frame and you measure the speed of a pulse, it is 'c'. And if that same source comes at you at 0.5c and you measure the speed of another pulse, you
still measure the speed to be 'c' (
not 1.5c!).
That second postulate gives an inkling of length contraction and time dilation: Space and time cannot possibly be reckoned the same for all observers, if the speed of light
is reckoned the same for all observers.
Now back to Maxwell. What Einstein did was pose the question, "What sort of coordinate transformation would leave Maxwell's equations in the same form for all inertial observers?" This question is relevant because of the first postulate. If the laws of physics have to be the same for everybody, then the
equations have to be the same for everybody. Einstein didn't just pose the question, he also answered it: The coordinate transformation is the
Lorentz transformation.
And derivable from the LT are the formulas for length contraction and time dilation. So the best way I can think of the "explain" these phenomena is to say that they are deduced from the postulates of SR, which in light of all the experimental data are eminently reasonable, and the covariance of Maxwell's equations, which are well-confirmed experimentally.