The Galilean transformation that we presented in Section 25-2 is not consistent with the postulates of special relativity. A set of transformation equations that is consistent with relativity is the Lorentz transformation. As in Figure 25-3, we take frame \(S'\) to be moving at speed \(V\) in the positive \(x\) direction relative to frame \(S\). The origins of the two frames coincide at \(t = 0\) in frame \(S\) and \(t' = 0\) in frame \(S'\). If an event takes place at coordinates \(x, y, z, t\) in frame \(S\), the coordinates of that same event in frame \(S'\) are