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Spectroscopy 29 Atoms and Molecules Spectroscopy Atoms Bohr Hydrogen Excited States Lasers Slide 29-2 © 2010 Pearson Education, Inc. Continuous Spectra and Blackbody Radiation Slide 29-11 © 2010 Pearson Education, Inc. The Hydrogen Spectrum © 2010 Pearson Education, Inc. Slide 29-10 Discrete Spectra of the Elements © 2010 Pearson Education, Inc. Slide 29-12 Rutherford’s Experiment Wavelengths of visible lines in the hydrogen spectrum Balmer’s formula l = © 2010 Pearson Education, Inc. 91.1 nm 1 1 2− 2 m n Slide 29-13 © 2010 Pearson Education, Inc. Slide 29-14 1 Using the Nuclear Model Bohr’s Model of Atomic Quantization Ionization The nucleus Isotopes © 2010 Pearson Education, Inc. Slide 29-15 Bohr’s Model of Atomic Quantization (cont’d) Slide 29-16 © 2010 Pearson Education, Inc. Frequencies of Photons Emitted in Electron Transitions fphoton = © 2010 Pearson Education, Inc. Slide 29-17 Representing Atomic States ∆Eatom h © 2010 Pearson Education, Inc. Slide 29-18 The Bohr Hydrogen Atom Energy-level diagram © 2010 Pearson Education, Inc. Slide 29-19 © 2010 Pearson Education, Inc. Slide 29-20 2 Energy-Level Diagram of the Hydrogen Atom The Quantum-Mechanical Hydrogen Atom 1. Schrödinger found that the energy of the hydrogen atom is given by the same expression found by Bohr, or En = − 13.60 eV n2 n = 1, 2,3,... The integer n is called the principal quantum number. 2. The angular momentum L of the electron’s orbit must be one of the values L = l (l + 1) U l = 0,1, 2,3,..., n − 1 The integer l is called the orbital quantum number. Slide 29-21 © 2010 Pearson Education, Inc. The Quantum-Mechanical Hydrogen Atom (cont’d) 3. The plane of the electron’s orbit can be tilted, but only at certain discrete angles. Each allowed angle is characterized by a quantum number m, which must be one of the values Slide 29-22 © 2010 Pearson Education, Inc. Energy and Angular Momentum of the Hydrogen Atom m = −l , −l + 1,..., 0,..., l − 1, l The integer m is called the magnetic quantum number because it becomes important when the atom is placed in a magnetic field. 4. The electron’s spin can point only up or down. These two orientations are described by the spin quantum number ms, which must be one of the values ms = − 1 1 or + 2 2 Slide 29-23 © 2010 Pearson Education, Inc. Excited States and the Pauli Exclusion Principle Energy Levels in Multielectron Atoms Hydrogen atom © 2010 Pearson Education, Inc. Slide 29-24 © 2010 Pearson Education, Inc. Multielectron atom Helium atom Slide 29-25 © 2010 Pearson Education, Inc. Lithium atom Slide 29-26 3 The Periodic Table © 2010 Pearson Education, Inc. Building Up the Periodic Table Slide 29-27 Slide 29-29 Molecules © 2010 Pearson Education, Inc. Slide 29-28 Emission Spectra Excitation by Absorption and Collision © 2010 Pearson Education, Inc. © 2010 Pearson Education, Inc. © 2010 Pearson Education, Inc. Slide 29-30 Fluorescence Slide 29-33 © 2010 Pearson Education, Inc. Slide 29-34 4 Photon Amplification Stimulated Emission and Lasers © 2010 Pearson Education, Inc. Slide 29-37 © 2010 Pearson Education, Inc. Slide 29-38 A Helium-Neon Laser © 2010 Pearson Education, Inc. Slide 29-39 5