By Hilary D. Brewster
ISBN-10: 9380179030
ISBN-13: 9789380179032
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Additional info for Relativity
Sample text
These are instead due to space time being structured such that the invariant speed c is finite. If we surprisingly discovered that light had some small amount of mass and thus really traveled at speeds just short of c, it would have no ramification on the physics of special relativity whatsoever. It would merely mean that we are using bad terminology, for instance in calling c speed particles "light-like". What actually distinguishes Lorentz transformations and special relativistic physics from Galilean transformations and Newtonian physics is that in the Lorentz transformations the invariant speed c is finite.
Ans that velocity of a particle is obtained from the reciprocal ofthe slope of its path Oil the diagram instead of directly from the slope. Yes, this seems weird to do at first but its also the usual way to do it so you get used to it. So the path of an accelerating particle on a spacetime diagram can look like: ct x 0:ow lets say the path represents the path of an accelerated observer. The events comprised of the ticks on the watch of th is observer all lay along the Relativity Made Simple 36 path and so the observer's world line or the path the observer takes can be labeled as the time axis for this observer.
T 'will be the time it takes the ship to reach the star according to the ship frame and P as a function of proper time is. 130 P = -130 for ct'