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Chapter 3: Rate Laws
Transition State Theory
Derivation of the Rotational Partition Function qR
Rigid Rotation 23
To show
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(R1) | |||
where | ||||
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(R2) | |||
Consider a particle of mass m rotating about the z axis a distance r from the origin. | ||||
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(R3) | |||
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This time we convert the wave equation to spherical coordinate to obtain 24 | ||||
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(R4) | |||
Classical Energy of a rigid rotator is | ||||
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(R5) | |||
where w is the angular velocity (rod/s) and I is the moment of inertia 25 | ||||
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(R6) | |||
where mi is the mass located and distance ri from the center of mass. | ||||
Quantum mechanics solutions to the
wave equation gives two quantum numbers, ![]() |
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(R7)26 | |||
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Let J ≡ ![]() |
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For a linear rigid rotator | ||||
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(R8) | |||
Where B is the rotation constant: | ||||
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(R2)27 | |||
with | ||||
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The rotational partition function is | ||||
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(R9)28 | |||
Replacing the ![]() |
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(R10) | |||
where Sy is the symmetry number which is the number of different but equivalent arrangements that can be made by rotating the molecules. | ||||
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where ![]() |
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Sy = symmetry number. 30 For a hetronuclear molecule σ= 1 and for a homonuclear diatomic molecule or a symmetrical linear molecule, e.g., H2, then σ= 2. | ||||
Order of Magnitude and Representative Values | ||||
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23P. W. Atkins, Physical Chemistry, 5th ed. (New York: Freeman, 1994), pp. 409, 413, 557, A24.
24P. W. Atkins, Physical Chemistry, 5th ed. (New York: Freeman, 1994), p. 410.
25P. W. Atkins, Physical Chemistry, 5th ed. (New York: Freeman, 1994), p. 555.
26P. W. Atkins, Physical Chemistry, 5th ed. (New York: Freeman, 1994), pp. 408, 413.
27P. W. Atkins, Physical Chemistry, 5th ed. (New York: Freeman, 1994), p. 557.
28P. W. Atkins, Physical Chemistry, 5th ed. (New York: Freeman, 1994), pp. 414, 563, 671.
29 P. W. Atkins, Physical Chemistry, 5th ed. (New York: Freeman, 1994), p. 694.
30For discussion of s, see K. J. Laidler, Chemical Kinetics, 3rd ed. (New York: Harper Collins, 1987), p.99.
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