Lorentz Transformation is a fundamental idea in the theory of Special Relativity, formulated by the scientist Hendrik Lorentz. It describes how measurements of space and time by two observers are related to each other in scenarios where the observers are moving at constant velocities relative to one another. Specifically, it's used to transform the coordinates of an event as seen in one inertial frame to the coordinates in another inertial frame.
A key aspect of Lorentz Transformation is that it accounts for the fact that the speed of light is the same in all inertial frames, irrespective of the motion of the light source or the observer. This is different from classical mechanics, where speeds can simply be added or subtracted depending on the direction of motion.
In mathematical form, the Lorentz transformations show how a set of coordinates \( (x, y, z, t) \) in one frame of reference can be transformed to another frame \( (x', y', z', t') \) using the equations:\
- \( x' = \gamma (x - vt) \)
- \( t' = \gamma (t - \frac{vx}{c^2}) \)
where \( v \) is the relative velocity between the frames and \( c \) is the speed of light in a vacuum, and \( \gamma \) is the Lorentz factor defined as \( \gamma = \frac{1}{\sqrt{1 - \frac{v^2}{c^2}}} \).
The Lorentz Transformation preserves the spacetime interval \( s^2 = x^2 + y^2 + z^2 - c^2t^2 \), showing that this interval is invariant for all observers, underpinning the consistent value of the speed of light and the relativistic effects it entails.