Moments of inertia of octahedral prolate symmetric rotor with \(D_{4h}\) symmetry

The moments of inertia of an octahedral prolate rotor with symmetry (e.g. Pt(NH3) 2Cl4) are characterised by a unique moment of inertia around the principal axis and two equal moments of inertia perpendicular to the principal axis, where . They are derived using simple geometric considerations.

The diagram above shows an octahedral molecule of the type BA4C2, where B is the central atom. The moment of inertia along the -axis is . Since the four B-A bonds have equal lengths of , we have

 

Question

Why do and  not contribute to ?

Answer

In general, . Since atoms B and C lie along the rotational axis, the moment of inertia about this axis is effectively zero due to the absence of perpendicular mass displacement ().

 

Similarly, the moment of inertia of the molecule about the -axis, which is equal to that about the -axis, is . Since the two B-C bonds have equal lengths of , we have

You’ll find that the expression for the moment of inertia about the -axis is the same as eq36.

 

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