For a thermodynamic process to be reversible, the system must be in near-equilibrium at each stage, requiring infinitesimally small differences in pressure/temperature, and hence the process proceeds very slowly without dissipative losses.
Ultraviolet light of wavelength 350 nm and intensity \(1.00Wm^{−2 }\) falls on a potassium surface. The maximum kinetic energy of the photoelectron is