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A solution and solid state study of niobium complexes University of ...

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Chapter 3<br />

electromagnetic spectrum between the visible <strong>and</strong> microwave regions <strong>and</strong> this area<br />

is divided into three regions: near (14 000 – 4 000 cm -1 ), mid (4 000 – 400 cm -1 ) <strong>and</strong><br />

far (400 – 10 cm -1 ) IR. The technique is based on the vibrations <strong>of</strong> atoms <strong>of</strong> a<br />

molecule. Important parameters are the frequency (v), wavelength (λ, length <strong>of</strong> 1<br />

wave) <strong>and</strong> wavenumber (, number <strong>of</strong> waves per unit length) <strong>and</strong> they are related to<br />

one another by the following equation 5 . Here, c is the speed <strong>of</strong> light <strong>and</strong> n the<br />

refractive index <strong>of</strong> the medium it is passing through:<br />

=<br />

<br />

⁄ <br />

= 1<br />

46<br />

λ (3.4)<br />

A spectrum is obtained by passing infrared radiation through a sample <strong>and</strong><br />

determining the fraction <strong>of</strong> incident radiation that is absorbed at a specific energy.<br />

Radiation is considered as two perpendicular electric <strong>and</strong> magnetic fields, oscillating<br />

in a single plane. This radiation can be regarded as a stream <strong>of</strong> particles for which<br />

the energy (E) can be calculated as follows. Where h is the Planck constant (h =<br />

6.626 x 10 -34 J.s).<br />

E = hν (3.5)<br />

Two important characteristics to the process are the radiation frequency <strong>and</strong> the<br />

molecular dipole moment (µ). The interaction <strong>of</strong> radiation with molecules involves a<br />

resonance condition where the specific oscillating radiation frequency matches the<br />

natural frequency <strong>of</strong> a particular normal mode <strong>of</strong> vibration. The molecular vibration<br />

must cause a change in the dipole moment <strong>of</strong> the molecule in order for the energy to<br />

be transferred from the IR photon to the molecule, via absorption 6 .<br />

IR spectroscopy depends on the specific frequencies at which chemical bonds<br />

vibrate or rotate. Chemical bonds can be excited by IR radiation to cause bond<br />

“stretching” (high energy) or bond “bending” (low energy) vibrations. This stretching<br />

or bending <strong>of</strong> bonds can be classified into various vibrational modes. 7 In the case <strong>of</strong><br />

stretching, the modes can either be symmetrical or asymmetrical. The modes <strong>of</strong><br />

bending include rocking, scissoring, wagging <strong>and</strong> twisting. As a rule, the stretching<br />

5<br />

B. H. Stuart, Infrared Spectroscopy: Fundamentals <strong>and</strong> Applications, Wiley <strong>and</strong> Sons, New York, 3, 2004.<br />

6<br />

D. N. Sathyanarayana, Vibrational Spectroscopy: Theory <strong>and</strong> Applications, New Age International, New Delhi,<br />

44, 2004.<br />

7 th<br />

L. D. Field, S. Sternhell, J. R. Kalman, Organic Structures from Spectra, 4 Ed, Wiley <strong>and</strong> Sons, New York, 15,<br />

2007.

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