The Photoelectric Effect
This section focuses on the photoelectric effect, first observed by Heinrich Hertz in 1887, where light is seen to release electrons from metal surfaces. Light strikes the metal and the electrons absorb enough energy to overcome the attractive forces holding them. This process is characterized by a minimum threshold frequency, below which no electrons are emitted regardless of light intensity. Experimental observations by Hallwachs and Lenard further established the dependency of current flow on intensity and frequency of the incident light. The section explains the significant deviation of these observations from classical wave theory and introduces Einstein’s photon theory, which accounts for the observations. Einstein proposed that light consists of energy packets (quanta), with the energy of each quantum given by E = hn. This culminated in Einstein's photoelectric equation, allowing for the calculation of the maximum kinetic energy of emitted electrons, emphasizing the dual nature of light and laying the groundwork for modern quantum physics.