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Organic Chemistry Semester 1 LABORATORY MANUAL - Moravian ...

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Part V. Techniques and Theory Appendix C1 Infrared Spectroscopy<br />

Appendix C. Infrared Spectroscopy:<br />

See also See Padías pp. 64 – 74 and CGWW pp. 65-72<br />

Source of the IR Spectrum<br />

Vibrational Energy Levels<br />

Covalent bonds link atoms together to form molecules. Though these bonds have normal<br />

average lengths, the relative positions of the atoms are constantly changing due to bond<br />

vibrations. A bond can be thought of as a spring with atoms attached to each end.<br />

A<br />

B<br />

bending<br />

stretching<br />

bond<br />

stretching<br />

As with other types of molecular changes, bond vibrations occur only at certain frequencies<br />

(ν) and each of these ν's is associated with a vibrational energy level of energy = hν. Thus, each<br />

bond has a series of vibrational energy levels.<br />

Transitions<br />

When electromagnetic radiation (light) is shone upon a molecule, one of its bonds can absorb a<br />

quantum of the energy and pass from a lower vibrational energy level to a higher one if the<br />

radiation contains light of a proper frequency (ν).<br />

e.g.<br />

light (! 1 )<br />

E 3<br />

!E o -> 2<br />

E = h! 1<br />

E 2<br />

E 1<br />

The Spectrum:<br />

" !E 0 -> 2 = h! 1<br />

E 0<br />

IR absorption bands are measured as a function of the ν of the incident light. The units of ν are<br />

cm -1 .<br />

Note: Since E = hν for light, the energy of absorbed light is proportional to ν, that is, the energy<br />

of the photons of light increase as their ν's increase.

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