The Jarzynski Equality is a fundamental result in nonequilibrium statistical mechanics that relates the work done on a system during a non-equilibrium process to the change in free energy of the system. It establishes a powerful connection between thermodynamics and statistical mechanics, revealing that even in far-from-equilibrium situations, the average of the exponential of the work done is equal to the exponential of the negative change in free energy. This equality emphasizes the role of fluctuations and provides insights into how systems can transition between different states.