Infrared band intensities: a comparative study of the transition moment matrix elements for the fundamental and overtones: Part II . Application to CO, HCl and OH

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The various expressions considered in Part I for the transition moment matrix elements of fundamental and first two overtones are applied to carbon monoxide. The coefficients a ij in the expressions R io = Σ a ij p j (where R io is the transition moment integral for the O → i vibrational transition and p j is the dipole moment derivative ∂ j P /∂XXX j , XXX = ( r — r e)/ r e, r e is equilibrium bond distance) are reported for i, j = 1, 2, 3. It is found that these coefficients do not vary by more than 5% when compared for the same i, j values in various expressions irrespective of the most exhaustive treatments used in deriving the original expressions. On the basis of the values of the coefficients obtained for CO, generalisations have been suggested on the effects of inclusion of mechanical and electrical anharmonicity to the intensities of fundamental and first two overtones. It is generally observed that the contribution of p' 1, is about 100 fold more than the contribution of p' 2, for R 10. On the other hand the contributions of p' 1, and p, for R 20 and R 30 are of nearly equal magnitude but opposite in sign. The contribution of p' 1 to R 10 is much higher than its contribution to R 20 and R 20. The various observations lead us to conclude that, whereas the effect of inclusion of mechanical anharmonicity on the intensity of the fundamental band is negligible, this effect is almost comparable to the effect of inclusion of electrical anharmonicity for the first two overtones. Simple forms of the a ij expressions are applied to HC1 and OH to demonstrate the effect of variation of molecular constants on the a ij values. On the basis of the observed trend in the values of these coefficients for CO, HCl and OH general remarks on the effects of hydrogen bonding on IR band intensities are given.