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Chemistry · Glossary

What is Normal mode?

Definition 5.12 University Chemistry — Year 3 · Chapter 5 — Group Theory Applied

A normal mode of a molecule is a collective vibration in which all atoms oscillate at the same frequency and in phase, along the eigenvector of the mass-weighted Hessian (Proposition 3.3). Each normal mode transforms as an irreducible representation of the point group.

The three normal modes of water (arrows: displacements, not to scale). Both a_1 modes keep the full symmetry of the molecule; the b_1 mode changes sign under C_2.
The three normal modes of water (arrows: displacements, not to scale). Both a1a_1 modes keep the full symmetry of the molecule; the b1b_1 mode changes sign under C2C_2.

Examples

Example 5.15 (Water)

HX2O\ce{H2O} in C2vC_{2v}, molecule in the xzxz plane. Atoms left in place: 3, 1, 3, 1; χxyz\chi_{xyz}: 3,−1,1,13, -1, 1, 1; so χ3N=9,−1,3,1\chi_{3N} = 9, -1, 3, 1. The reduction gives 3A1+A2+3B1+2B23A_1 + A_2 + 3B_1 + 2B_2. Translations A1+B1+B2A_1 + B_1 + B_2 and rotations A2+B1+B2A_2 + B_1 + B_2 removed: Γvib=2A1+B1\Gamma_{\mathrm{vib}} = 2A_1 + B_1. The two a1a_1 modes are the symmetric stretch (3657 cm−13657\,\mathrm{cm}^{-1}) and the bend (1595 cm−11595\,\mathrm{cm}^{-1}); the b1b_1 mode is the antisymmetric stretch (3756 cm−13756\,\mathrm{cm}^{-1}).

Example 5.16 (Four more molecules)

The same procedure (computed and checked in the figure data of this chapter) gives:

moleculegroupΓvib\Gamma_{\mathrm{vib}}modes
NHX3\ce{NH3}C3vC_{3v}2A1+2E2A_1 + 2E6
CHX4\ce{CH4}TdT_dA1+E+2T2A_1 + E + 2T_29
COX2\ce{CO2}D∞hD_{\infty h} (via D2hD_{2h})Σg++Σu++Πu\Sigma_g^+ + \Sigma_u^+ + \Pi_u (Ag+B1u+B2u+B3uA_g + B_{1u} + B_{2u} + B_{3u})4
BFX3\ce{BF3}D3hD_{3h}A1′+2E′+A2′′A_1' + 2E' + A_2''6
XeFX4\ce{XeF4}D4hD_{4h}A1g+B1g+B2g+A2u+B2u+2EuA_{1g} + B_{1g} + B_{2g} + A_{2u} + B_{2u} + 2E_u9
SFX6\ce{SF6}OhO_hA1g+Eg+T2g+2T1u+T2uA_{1g} + E_g + T_{2g} + 2T_{1u} + T_{2u}15

For a linear molecule the infinite group is replaced by its subgroup D2hD_{2h}, in which the degenerate Πu\Pi_u bend splits into B2u+B3uB_{2u} + B_{3u}.

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