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between measured and calculated dipolar couplings. A Q factor of 40%, roughly
corresponding to Pearson's R of 0.9, are commonly found on structures with 2-3 ˚
resolution; and a Q value of 20% or less indicates the structure is at high resolution
(1.5 ˚ ) and accuracy. Clore and Garrett [ 64 ] suggested an alternative form
½
1 = 2 to replace the denominator of ( 8 ) in the case of a limited
RDC sampling over all of the possible orientations. A thorough discussion on Q
factor can be found elsewhere [ 65 ].
2 D a ð
3 R 2
4
þ
Þ=
5
rms
ð
D meas
D calc Þ
Q
¼
;
(8)
rms
ð
D meas Þ
2
E
¼
k
ð
D meas
D calc Þ
:
(9)
For solution structure determination, RDC is normally not included as a poten-
tial term ( 9 ) during the initial structure calculation in a simulated annealing protocol
in a program such as Xplor-NIH [ 66 , 67 ]. Due to directional degeneracy associated
with RDC restraints, as described in the theoretical expression section, multiple
local potential minima will hinder the successful search for the right conformation.
Typically a rough tertiary fold of protein is obtained first with the use of NOE
restraints and such a fold can be used as a starting structure for the next simulated
annealing procedure with the combined NOE and RDC restraints. The procedure to
include RDC restraints in a program such as Xplor-NIH uses four pseudo-atoms
( OXYZ )[ 68 ] to represent the alignment tensor directions [ 69 ]. The RDC force
constant, k in ( 9 ), can be increased gradually as the temperature is being lowered
in the simulated annealing. In the end it is ideal to adjust the force constant k so that
the deviation from the measured RDCs matches the experimental error.
4.3 Ensemble Minimization
As discussed before, RDC reflects the ensemble averaged dipolar coupling and
incorporates a wide range of time scales up to milliseconds. During RDC restrained
structure calculations we made approximations by assuming a single conformer. The
question remains whether it is reasonable to keep this assumption in all cases. Clore
and Schwieters [ 52 ] initially employed a two-member ensemble minimization to test
whether a better agreement between measured and calculated RDC data could be
achieved, and whether it was statistically significant. The ensemble algorithm pro-
posed by Clore and Schwieters [ 52 ] kept a user-defined number of conformers during
the course of a simulated annealing, and any evaluated physical quantity, e.g., D calc ,is
linearly averaged among individual conformers. After refining the ubiquitin structure
with D H-N data sets collected in 11 different alignment media, and a couple of other
heteronuclear RDCs, they found a single conformer in most cases is sufficient to yield
a good quality factor Q less than 20%. The structure was validated against the D H a -C a
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