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Physics 361 Principles of Modern Physics Lecture 2
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Photoelectric Effect When light strikes a metal, electrons (or “photoelectrons”) can be dislodged from metal. Energetic diagram e-e- e-e- Vacuum Level Weakest-Bound Electrons EFEF work function
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Work Function e-e- Vacuum Level Weakest-Bound Electrons EFEF work function Work functions of common metals
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Photoelectric Effect (Experiment) When light strikes E, photoelectrons are emitted Electrons collected at C and passing through the ammeter create a current in the circuit C is maintained at a positive potential by the power supply
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What Property of Light Determines Its Ability to Dislodge Electrons? Size of wave (“Amplitude”)? e-e-
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What Property of Light Determines Its Ability to Dislodge Electrons? Size of wave (“Amplitude”)? e-e- NO
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It’s the Frequency or Wavelength that matters! When light strikes E, photoelectrons are emitted Electrons collected at C and passing through the ammeter create a current in the circuit C is maintained at a positive potential by the power supply No electrons are emitted if the incident light frequency is below some cutoff frequency that is characteristic of the material being illuminated
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Einstein’s Explanation The photon’s energy would be E = hƒ, with h a universal constant. Each photon can give all its energy to an electron in the metal The maximum kinetic energy of the liberated photoelectron is KE max = hƒ – Φ Φ is the work function of the metal
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Verification of Einstein’s Theory Experimental observations of a linear relationship between KE and frequency confirm Einstein’s theory The x-intercept is the cutoff frequency
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Cutoff Wavelength The cutoff wavelength is related to the work function Wavelengths greater than C incident on a material with a work function don’t result in the emission of photoelectrons Can write cutoff relation in terms of f or through
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