solution
According to special theory of relativity when a frame S in which a point P(x, y, z, t) and another frame S' is which constant velocity v then coordintes of point in this frame according to lorenz transformation can be expressed as
x′=γ(x−vt)x'=\gamma(x-vt)x′=γ(x−vt)
y′=yy'=yy′=y
z′=zz'=zz′=z
t′=γ(t−vxc2)t'=\gamma(t-\frac{vx}{c^2})t′=γ(t−c2vx)
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