Early Quantum Theory & Models of the Atom (Ch 27) Discovery of electron. Blackbody Radiation. Blackbody Radiation. J. J. Thomson ( )

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Early Quantum Theory & Models of the Atom (Ch 27) Discovery of electron Modern physics special relativity quantum theory J. J. Thomson (1856-1940) measured e/m directly set-up was similar to mass spectrometer believed the electron was part of an atom Millikan (1868-1953) oil-drop experiment measured charge of electron, e Physics 120 1 Physics 120 2 Blackbody Radiation Blackbody Radiation Blackbody perfect absorber & emitter of light Wien s Law ultraviolet catastrophe models predicted too much flux at ultraviolet wavelengths Max Planck (1858-1947) developed equation to predict spectra The blackbody spectrum of light emitted by hot objects was unexplained at end of 1800 s Planck Physics 120 3 Physics 120 4 1

Planck s Quantum Hypothesis The Photoelectric Effect Energy is quantized E = h f h = 6.626 x 10-34 J s Energy of molecular vibrations can only be multiples of hf E = n h f, n=1,2,3 n = quantum number E 0.2 hf, 0.33 hf, 0.5 hf,... Planck considered this a mathematical device did not realize he started a revolution! Einstein provided interpretation for Planck s work (1905) Photon theory of light E = h f energy per photon (particle) of light Photoelectric Effect provides a test for photon theory of light Einstein won Nobel Prize for his work on the Photoelectric Effect Physics 120 5 Physics 120 6 The Photoelectric Effect Wave theory as intensity of light increases, max KE of e- increases b/c higher intensity -> higher E field -> higher KE frequency of light should not effect KE of e-, only intensity does Particle theory increasing intensity should produce more e- but should not change max KE of e- increasing frequency of light should increase max KE of e- hf = KE + W Einstein proved right by Millikan Physics 120 7 Photon properties Energy mass momentum Physics 120 8 2

Wave-Particle Duality Wave Nature of Matter some experiments indicate that light is a wave (Young s double-slit experiment) some experiments indicate that light is a particle (Photoelectric effect) Principle of Complementarity light is both wave and particle, probably more complex than both light shows different faces to experimenters models drawn from macroscopic world are inadequate true nature of light is not possible to visualize Note E=hf links particle and wave properties Louis de Broglie (1892-1987) extended wave-particle duality to matter in his PhD thesis (12 pages; 1923) won Nobel Prize in 1929 - first award for a thesis! perhaps things we think of as particles (e-, atoms, a ball, you) have wave properties as well wavelength given by: Physics 120 9 Physics 120 10 Problem What is the de Broglie wavelength of a 50 kg person traveling at 15 m/s? (h = 6.6 x 10-34 J s) Electron Diffraction wavelength of e- ~10-10 m comparable to spacing between atoms in a crystalline structure can use crystal as diffraction grating Confirms wave nature of particles also confirmed for neutrons, protons, etc Again, models are inadequate e- diffraction pattern Physics 120 11 Physics 120 12 3

Early Models of Atom Plum Pudding Model Atomic Spectra Models needed to explain why only discreet lines are emitted by atoms Ernest Rutherford: -alpha particles at gold foil -recoiling particles indicate presence of dense nucleus -solar system model for atom Physics 120 13 Physics 120 14 Bohr Model of Atom Bohr Model of Atom Following Planck and Einstein, perhaps e- s in atom have quantized energy proposed angular momentum is quantized, results in: Physics 120 15 Physics 120 16 4

de Broglie s Hypothesis Bohr s theory was ad hoc (designed to explain specific observations) wave nature of e- provided explanation for Bohr s model each e- in an orbit is a standing wave de Broglie s Hypothesis A wave that does not close destructively interferes with itself and rapidly decays Explains Bohr s conservation of angular momentum! quantum condition Physics 120 17 Physics 120 18 Bohr Model Limitations could not predict spectra for more complex atoms could not explain why emission lines, when view at high resolution, consist of 2 or more lines why are some spectral lines brighter than others? could not explain bonding between atoms not satisfactory from a theoretical point of view Needed a more comprehensive theory Quantum Mechanics provided by Erwin Schrodinger Werner Heisenberg Physics 120 19 5