5/30/2023 0 Comments Space time itnerval![]() ![]() We have already seen what the inverse Lorentz transformations are, and how we can obtain them, to wit, by replacing by. ![]() This, as we saw, was given by,Įssentially, what we had is nicely illustrated by the following figure:īut what if we want things the other way around (as we had at the beginning when we expressed everything from S’ in terms of S)? To do this, we will need the inverse Lorentz transformation. Last time, we looked at how to write the un-primed basis as observed from the primed basis (i.e. Here is how the Lorentz matrix looks, for our case of motion along the X axis:įor the other cases of motion along the Y, Z and hybrid axes, I suggest taking a look at this wikipedia article on it: Just to jog the memory, and assist in further discussions, take a look at the following figures:Ģ.
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