Download presentation
Published byThomasina Leonard Modified over 9 years ago
1
Vertical axis is energy Emitter WE Collector
No electrical connection between emitter (cathode) and collector (anode) . The vacuum levels are aligned Notation: EF Fermi energy EFE , EFC Fermi energy of emitter and collector respectively WE , WC Work function of emitter and collector respectively Photon energy hn KEE Vacuum level Vertical axis is energy Emitter WE Collector Kinetic energy of the electron when leaving the emitter Is: WC EFE EFC Emitter and connector are connected (V=0). Note that now the Fermi energies in the two metals are aligned KEE KEC Kinetic energy of the electron when reaching the collector. Is: Collector WC -WE WC Emitter WE
2
Retarding voltage Now: Collector WC Emitter WE eV
Apply a retarding voltage V between collector and emitter. The two Fermi energies are now offset by eV where e is the electron charge (note e is negative) KEC Now: KEE Collector eV+WC -WE WC Emitter WE Potential difference between collector and emitter as seen by the electron: eV Condition of zero current corresponds to Zero Kinetic energy of the electron when reaching the collector: PROVIDED that the photoelectric effect happened ie:
3
Accelerating voltage Emitter WE Collector WC eV
Now consider Forward bias - accelerating voltage KEE KEC Potential difference between collector and emitter as seen by the electron: Emitter WE Collector WC eV Now it looks like the electron velocity and therefore the current increases with V. But the current cannot increase indefinitely it will saturate when the electron flux equals to the incoming photon flux ๐ = ๐ โ๐ where P is the light power impinging on the emitter.
4
Saturation voltage electron is neither accelerated nor retarded
Now consider Forward bias - accelerating voltage KEE KEC Emitter WE Collector WC eV Now it looks like the electron velocity and therefore the current increases with V. But the current cannot increase indefinitely it will saturate when the electron flux equals to the incoming photon flux ๐ = ๐ โ๐ where P is the light power impinging on the emitter.
Similar presentations
© 2024 SlidePlayer.com. Inc.
All rights reserved.