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CHEM 515 Spectroscopy. Vibrational Spectroscopy II. Vibrations of Polyatomic Molecules. N particles have 3N degrees of freedom ( x , y and z for each). Three degrees of freedom are translations . T X = X 1 + X 2 +…+ X N T Y = Y 1 + Y 2 +…+ Y N T Z = Z 1 + Z 2 +…+ Z N.
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CHEM 515Spectroscopy Vibrational Spectroscopy II
Vibrations of Polyatomic Molecules • N particles have 3N degrees of freedom (x, y and z for each). • Three degrees of freedom are translations. • TX = X1 + X2 +…+XN • TY = Y1 + Y2 +…+YN • TZ = Z1 + Z2 +…+ZN
Vibrations of Polyatomic Molecules • N particles have 3N degrees of freedom (x, y and z for each). • Three degrees of freedom are rotations about x, y and z axes. RX, RY, and Rz . • For linear molecules, only two rotational axes will represent degrees of freedom.
Vibrations of Polyatomic Molecules • N particles have 3N degrees of freedom (x, y and z for each). • The rest of degrees of freedom are vibrations. Number of vibrations are: • 3N – 6 for nonlinear molecules. • 3N – 5 for linear molecules.
Classical Picture of Vibrational Motions in Molecules • Classically, polyatomic molecules can be considered as a set of coupled harmonic oscillators. • Atoms are shown as balls connected with each other by Hooke’s law springs.
Classical Picture of Vibrational Motions in Molecules • Stronger forces between O and H atoms are represented by strong springs (resistance to stretching the bonds). • Weaker force between H atoms is represented by weaker spring (resistance to increase of decrease of the HOH angle “bending of the angle”)
Normal Modes of Vibrations • The collective motion of the atoms, sometimes called Lissajous motion, in a molecule can be decomposed into normal modes of vibration within the harmonic approximation.
Normal Modes of Vibrations • The normal modes are mutually orthogonal. That is they represent linearly independent motions of the nuclei about the center-of-mass of the molecule. • For CO2 molecule, number of vibrations = 3N – 5 = four vibrations.
Normal Modes in Water Molecule • For H2O molecule, number of vibrations = 3N – 6 = three vibrations. • Liberation motions are the x, y and z rotations.