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Diatomic configurational symmetry

In the case of atoms, deriving states from configurations, in the Russell-Saunders approximation (Section 7.1.2.3), simply involved juggling with the available quantum numbers. In diatomic molecules we have seen already that some symmetry properties must be included, in addition to the available quantum numbers, in a discussion of selection rules. [Pg.237]

From the quantum mechanical standpoint the appearance of the factor 1/2 = 1/s for the diatomic case means the configurations generated by a rotation of 180° are identical, so the number of distinguishable states is only one-half the classical total. Thus the classical value of the partition function must be divided by the symmetry number which is 1 for a heteronuclear diatomic and 2 for a homonuclear diatomic molecule. [Pg.110]

Problem 9-3. Predict the electron configurations, and the possible symmetry species of the ground states of the second-row diatomics Li2, BC2, B2, C2, N2, O2, F2, NC2. [Pg.87]


See other pages where Diatomic configurational symmetry is mentioned: [Pg.167]    [Pg.248]    [Pg.259]    [Pg.5]    [Pg.264]    [Pg.50]    [Pg.109]    [Pg.107]    [Pg.195]    [Pg.59]    [Pg.110]    [Pg.284]    [Pg.192]    [Pg.45]    [Pg.113]    [Pg.115]    [Pg.230]    [Pg.25]    [Pg.42]    [Pg.13]    [Pg.245]    [Pg.280]    [Pg.264]    [Pg.246]    [Pg.267]    [Pg.411]    [Pg.665]    [Pg.107]    [Pg.211]    [Pg.182]    [Pg.115]    [Pg.327]    [Pg.239]    [Pg.27]    [Pg.104]    [Pg.6]    [Pg.487]    [Pg.411]    [Pg.168]    [Pg.34]    [Pg.411]    [Pg.2738]    [Pg.355]    [Pg.5]    [Pg.665]    [Pg.452]   
See also in sourсe #XX -- [ Pg.65 , Pg.74 ]




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Configurational symmetry

Symmetry configurations

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