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IR Spectroscopy Wave length ~ 100 mm to 1 mm
Wave number ~ 100 to 10,000 cm-1 Frequency ~ 3 x to 3 x 1014 Hz Energy ~ 1 kJ to 100 KJ /mole
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HCl absorptions 2885.9 cm-1 fundamental band strong
cm first overtone weak cm second overtone cm third overtone cm fourth overtone
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Potential Energy Curve
V(r) r
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Harmonic Approximation
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Vibration of a diatomic molecule
Centre of mass does not move!
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Quantum Mechanics of vibration
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Must have an oscillating dipole moment
Selection Rule Must have an oscillating dipole moment Initial state Final state Transition Moment = Integral Transition Moment Integral
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Morse Potential
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2 1 3 Blue –ALLOWED Red – NOT
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2 1 3
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Morse Potential
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Electric field + vibrating diatomic molecule
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Vibrating Rotating Diatomic
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Variables can be separated!
Change to polar co-ordinates x Y Z Variables can be separated!
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Up to second order in v and J
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Selection Rule Initial state Final state
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J EJ 3 12B 2 6B 1 2B Anti-Stokes J EJ 12B 3 2 6B 1 2B 2B 4B P Q R
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IR Spectrum of CO2
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Polyatomic molecules Normal Modes Center of mass does not move
Motion is in Phase All atoms vibrate with same frequency 3N-6 Normal Modes Bending mode of CO cm-1 We denote normal modes as
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Symmetric Stretch of CO2 1330 cm-1
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Antisymmetric Stretching of CO2, 2349 cm-1
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Vibrational energy of a polyatomic
Each Normal Modes = A Hamonic Oscillator Energy of one hamonic Oscillator is known!
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State of the molecule specified by
Wave function: Selection Rule: Only one of can change
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Benzene
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