Rotational relaxation

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Rotational relaxation refers to the decay of certain autocorrelation magnitudes related to the orientation of molecules.

If a molecule has an orientation along a unit vector n, its autocorrelation will be given by

c1(t)=⟨n(0)⋅n(t)⟩.

From the time decay, or relaxation, of this function, one may extract a characteristic relaxation time (either from the long-time exponential decay, or from its total integral, see autocorrelation). This magnitude, which is readily computed in a simulation is not directly accessible experimentally, however. Rather, relaxation times of the second spherical harmonic are obtained:

c1(t)=⟨P2(n(0)⋅n(t))⟩,

where P2(x) is the second Legendre polynomial.

According to simple rotational diffusion theory, the relaxation time for c1(t) would be given by τ1=1/2Drot, and the relaxation time for c2(t) would be τ2=1/6Drot. Therefore, τ1=3τ2. This ratio is actually lower in simulations, and closer to 2; the departure from a value of 3 signals rotation processes "rougher" than what is assumed in simple rotational diffusion (Ref 1).


Water

Often, molecules are more complex geometrically and can not be described by a single orientation. In this case, several vectors should be considered, each with its own autocorrelation. E.g., typical choices for water molecules would be:

symbol explanation experimental value, and method
HH H-H axis τ2=2.0ps (H-H dipolar relaxation NMR)
OH O-H axis τ2=1.95ps ( 17O-H dipolar relaxation NMR)
μ dipolar axis not measurable, but related to bulk dielectric relaxation
⊥ normal to the molecule plane not measurable


References

See also