Derive the transformations x→1−v2x+vt and t→1−v2t+vx in perturbation theory. Start with the Galilean transformation x→x+vt. Add a transformation t→t+δt and solve for δt assuming it is linear in x and t and preserves t2−x2 to O(v2). Repeat for δt and δx to second order in v and show that the result agrees with the second-order expansion of the full transformations.