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'=\\gamma(x-vt)"
"y'=y"
"z'=z"
"t'=\\gamma(t-\\frac{vx}{c^2})"
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