ash64449 said:
Hello friend,
Can you give me an example that shows simultaneous events in one reference frame not simultaneous in other reference frame with the help of lorentz Transformation?
Sure. I'll use the simplified LT where c=1, and where y and z are zero. First we calculate gamma as a function of the relative speed beta (the ratio of the speed to the speed of light) between the two frames:
γ = 1/√(1-β
2)
Next we have the two equations for the distance, x', and time, t', coordinates in the new frame as a function of the distance, x, and time, t, in the original frame along with gamma and beta:
x' = γ(x-βt)
t' = γ(t-βx)
So let's say our two events are at t1=100, x1=100 and t2=100, x2=200. Note that these two events in our original frame are simultaneous because their time coordinates are the same (t1 = t2 = 100).
And let's say beta = 0.6.
Gamma is calculated as:
γ = 1/√(1-β
2) = 1/√(1-0.6
2) = 1/√(1-0.36) = 1/√(0.64) = 1/0.8 = 1.25
Now we want to calculate the coordinates in the new frame for the first event:
x1' = γ(x1-βt1) = 1.25(100-0.6*100) = 1.25(100-60) = 1.25(40) = 50
t1' = γ(t1-βx1) = 1.25(100-0.6*100) = 1.25(100-60) = 1.25(40) = 50
Finally the coordinates in the new frame for the second event:
x2' = γ(x2-βt2) = 1.25(200-0.6*100) = 1.25(200-60) = 1.25(140) = 175
t2' = γ(t2-βx2) = 1.25(100-0.6*200) = 1.25(100-120) = 1.25(-20) = -25
Actually, I didn't really need to calculate the new distance coordinates because all you wanted was to show that the new time coordinates would not be the same (t1' = 50 ≠ t2' = -25) but it doesn't hurt to see both the new time and distance coordinates.