Physics for Scientists and Engineers with Modern Physics
Physics for Scientists and Engineers with Modern Physics
10th Edition
ISBN: 9781337553292
Author: Raymond A. Serway, John W. Jewett
Publisher: Cengage Learning
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Chapter 42, Problem 47CP

As an alternative to Equation 42.1, another useful model for the potential energy of a diatomic molecule is the Morse potential

U ( r ) = B [ e a ( r r 0 ) 1 ] 2

where B, a, and r0 are parameters used to adjust the shape of the potential and its depth. (a) What is the equilibrium separation of the nuclei? (b) What is the depth of the potential well, defined as the difference in energy between the potential’s minimum value and its asymptote as r approaches infinity? (c) If μ is the reduced mass of the system of two nuclei and assuming the potential is nearly parabolic about the well minimum, what is the vibrational frequency of the diatomic molecule in its ground state? (d) What amount of energy needs to be supplied to the ground-state molecule to separate the two nuclei to infinity?

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The Morse potential The harmonic potential, V(x) = ½kx?, is useful start for modelling molecular vibrations, but it has limitations. A realistic potential between to atoms should accurately represent the sharp increase in the potential as two nuclei come in close proximity, and also have the ability for a bond to break: that is, an asymptote V →0 as x →00. One option, as shown in the figure, is the Morse potential: V(r) = D(1 – e-«(r=re))2 15 10 10 15 20 The parameter D is the well depth (or binding energy) of the potential, re is the bond length, and a is the anharmonicity constant.
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