Giveni Lo = 100 cons & Train's proper length i.e, in the Reference frame I of Beth = 100x3x10 m x 10 = 30m = 3c velocity of train with respect to Alan on the ground. @ We know , moving train would appear shorter to Alan. By Length contraction, we have La Lo where r = - - r - 25 : Alan, The length of train acc. to Lubom 4L0 = 80 C-ns 24 m L = 24 m
6 Now, consider firecrackers in the event Alan's events of frame I Train I O (x, t) = (0,0) CL,O) where we make convention (without loss of generality) that assistant's set-off crackers at t=0 de. simultaneously for them.
Let the (0,0) Space - time event Event 1 and that occur at (2,0) event 2, Transformations. Now We have Lorents x = x (x-ut) t=r ( tv) where & x&t xgt are are space-time space-time for for Alan's frame Beth's Shame Event 1 in 0,0) = (xit) x'=r (o-o) =0 ; t'arco-o) = 0. and Event. 2 (Lio) = (xit) as explain in @ x t =r (L-0,0)=rL=Lo; = r Co-LV) (2 02 • For Beth this two events occur at Coo) and CrL , NLV) time Separation - MLY = Ę.24.20 m.my's (m/s)
s Second. = 18 3x108 ot' = 68108 lot = 0.6 nos) © Now we find same but by conservation interval ot' without L-T. of space-time i.e. Dx?_c²at2 = Dne 12 – C² at 2 .. We have according to problem @ Dx=L DX'= Lo st=o ot' =2 . L2-(²,0 = Lo2_c? at 2 i L²= L ² - c² Dt 2 (24)2 = (30)2 - c²ot 2 (² ot2 = 900-576 c²ot 2 = 324 cot = 18 ot'=18 с Second. 107' = 0.6 ms]