Locally mobile bond-vectors
contribute to the conformational entropy
of the protein, given by
S
k
≡
S
/
k
= −∫(
P
eq
ln
P
eq
)dΩ –
ln∫dΩ. The quantity
P
eq
=
exp(−
u
)/
Z
is the orientational
probability density, where
Z
is the partition function
and
u
is the spatially restricting potential exerted
by the immediate internal protein surroundings at the site of the
motion of the bond-vector. It is appropriate to expand the potential,
u
, which restricts local rotational reorientation, in the
basis set of the real combinations of the Wigner rotation matrix elements,
D
0
K
L
. For small molecules
dissolved in
anisotropic media, one typically keeps the
lowest even
L
,
L
= 2,
nonpolar
potential in axial or rhombic form. For bond-vectors
anchored
at
the protein, the lowest odd
L
,
L
= 1,
polar
potential is to be used in
axial or rhombic form.
Here, we investigate the effect of
the symmetry and polarity of these potentials on
S
k
. For
L
= 1 (
L
= 2),
S
k
is the same (differs) for parallel
and perpendicular ordering. The plots of
S
k
as a function of the coefficients of the rhombic
L
= 1 (
L
= 2) potential exhibit high-symmetry (specific
low-symmetry) patterns with parameter-range-dependent sensitivity.
Similar statements apply to analogous plots of the potential minima.
S
k
is also examined as a function of the order
parameters defined in terms of
u
. Graphs displaying
these correlations, and applications illustrating their usage, are
provided. The features delineated above are generally useful for devising
orienting potentials that best suit given physical circumstances.
They are particularly useful for bond-vectors acting as NMR relaxation
probes in proteins, when their restricted local motion is analyzed
with stochastic models featuring Wigner-function-made potentials.
The relaxation probes could also be molecules adsorbed at surfaces,
inserted into membranes, or interlocked within metal–organic
frameworks.