syano said:
I was explaining to one of my friends about how if you could travel the speed of light then you could get to any destination, no matter how far away, instantaneously. And if you were going a bit slower then the speed of light (lets say 98% C) then you could reach a destination, let's say 100 light years away, in just a few years (or you would just age a couple of years even though you traveled a distance of 100 light years)
Would someone here mind to elaborate on this and give a more technical explanation? My friend is very skeptical on what I am saying.
Thanks,
The only technical correction that comes to mind is to expand on your last remark, and to talk about the limit as one approaches 'c' rather than talking about traveling at c. One can definitely say that in the limit as v->c, the proper time elapsed for an observer moving a finite proper distance 'd' with a velocity v goes to zero.
The proof is simple. For the observer at rest, we can assign coordinates to the events of the start and end of the trip as follows:
start of trip: t=0, x=0
end of trip: t = d/v, x=d
The invariant lorentz interval is
L = c^2 (\Delta time)^2 - (\Delta distance)^2 =
c^2*(d/v)^2 - d^2 =
d^2*(c^2/v^2-1)
For the observer in motion, the coordinates will be:
start of trip: t=0, x=0
end of trip: t=tau, x=0
The invariant lorentz inteval will be
L = c^2*tau^2
Because the Lorentz interval is invaraint for all inertial observers, we write:
c^2*tau^2 = d^2*(c^2/v^2-1)
tau = d *sqrt(1/v^2 - 1/c^2) =
<br />
\frac{d}{v} \sqrt{1-(v/c)^2}<br />
This result can be interpreted from the moving observer's POV as the fact that the distance he travels is shorter than the proper distance 'd' by the factor of sqrt(1-(v/c)^2) due to Lorentz contraction.
From the stationary obsever's POV, the moving observer's clocks run slow by a factor of 1/sqrt(1-(v/c)^2)
In any event, in the limit as v->c, the value of tau approaches the limit zero, because sqrt(1-(v/c)^2) approaches zero while d/v approaches a finite value d/c.
Your friend might also want to look at the sci.physics.faq on the relativistic rocket http://math.ucr.edu/home/baez/physics/Relativity/SR/rocket.html
This handles the case of an observer traveling at a constant acceleration, rather than a constant velocity, however.