Rovibronic Infrared Spectrum of a Rigid Diatomic Rotor

Requires a Wolfram Notebook System

Interact on desktop, mobile and cloud with the free Wolfram CDF Player or other Wolfram Language products.

Requires a Wolfram Notebook System

Edit on desktop, mobile and cloud with any Wolfram Language product.

This Demonstration lets you study rotationally-resolved infrared band spectra of the vibrational transition in diatomic molecules. Due to quantized vibrational and rotational energy levels and the selection rules and , allowed transitions result in a highly ordered spectrum consisting of a P branch ( , smaller wavenumbers) and an R branch ( , larger wavenumbers) separated by a central gap. Adjacent spectral lines are separated by a spacing of , and since line intensities depend on the Boltzmann factor for thermal population and the quantum number , each branch monotonically increases and/or decreases. As temperature increases, more lines are observed and the intensities of the lines decrease due to the population being spread over more rotational levels. Interactivity involves the effects of the fundamental vibrational frequency, rotational constant , temperature, and line width on the observed spectrum.

Contributed by: Whitney R. Hess and Lisa M. Goss (Idaho State University) (March 2011)
Open content licensed under CC BY-NC-SA


Snapshots


Details

The mathematical expressions for the simulated spectra assume that the diatomic molecule is a rigid rotator, with a small anharmonicity constant (, zero electronic angular momentum (), and that the rotational constants of the upper and lower states in any given transition are essentially equal (). It is also assumed that only the vibrational state is thermally populated, in order to eliminate the presence of "hot bands" and simplify the spectra.

Parameter Controls

The first parameter control lets you vary the fundamental vibrational frequency, which will change the spectrum position along the axis. The second control manipulates the rotational constant , which increases or decreases line separation. The third control manipulates temperature, and consequently the number of lines observed and their intensities. The last parameter control manipulates the line width, allowing simulation of spectra at various resolutions.

Spectrum Display Controls

These controls should be used to change how the spectrum is viewed. Line color and background color can be chosen and filling under the line can be turned on. Enabling the peak height control allows for the height of the spectrum to be manually increased or decreased. The axis upper and lower boundary controls function to set the range of the axis.

Snapshot 1: spectra acquired at low temperatures are greatly simplified as a result of few populated rotational energy levels

Snapshot 2: spectra acquired at high temperatures have many populated rotational energy levels, resulting in more observed lines

Snapshot 3: spectra acquired of diatomic molecules with a large rotational constant will have larger line separation

Snapshot 4: an increase in line width causes the lines to overlap and resolution to be lost

Snapshot 5: the lines of the P and R branches are completely unresolved due to low resolution

Snapshot 6: with low resolution characteristic of that used in organic chemistry, the band for the vibrational transition is broad and no longer rotationally resolved

References:

P. Atkins and J. de Paula, Physical Chemistry, New York: Oxford University Press, 2006.

G. Herzberg, Molecular Spectra and Molecular Structure I. Spectra of Diatomic Molecules, New Jersey: D. Van Nostrand Company, Inc., 1967.



Feedback (field required)
Email (field required) Name
Occupation Organization
Note: Your message & contact information may be shared with the author of any specific Demonstration for which you give feedback.
Send