-
10
-
-
85033304988
-
-
note
-
Properly speaking, the "transition state" should be called the "transition microstate" since only a single conformation is specified. It is important because it usually lies near the center of the extended "transition region" which governs transition rates, particularly at low temperatures.
-
-
-
-
14
-
-
85033285281
-
-
note
-
Y.
-
-
-
-
15
-
-
85033303927
-
-
note
-
If necessary, the labeling of metastable states X and Y can be reversed so that Eq. (11) will hold.
-
-
-
-
16
-
-
85033301337
-
-
note
-
s.
-
-
-
-
17
-
-
85033320360
-
-
note
-
g in lowest order.
-
-
-
-
18
-
-
85033317731
-
-
note
-
s.
-
-
-
-
20
-
-
85033321521
-
-
note
-
i is large will be appropriate.
-
-
-
-
22
-
-
0003525155
-
-
Wiley, New York
-
C. L. Brooks III, M. Karplus, and B. M. Pettitt, Proteins: A Theoretical Perspective of Dynamics, Structure, and Thermodynamics (Wiley, New York, 1988).
-
(1988)
Proteins: A Theoretical Perspective of Dynamics, Structure, and Thermodynamics
-
-
Brooks III, C.L.1
Karplus, M.2
Pettitt, B.M.3
-
27
-
-
85033310531
-
-
note
-
Both these numbers are ∼15% higher than those calculated using MM2 (Ref. 24) and CHARMM (Ref. 2) potentials with explicit hydrogen atoms.
-
-
-
-
28
-
-
85033316934
-
-
note
-
The Monte Carlo sampling was modified to accommodate the degeneracies associated with the rigid-body translational and rotational invariance. The translational degeneracy was eliminated simply by translating the center-of-mass of each sampled conformation back to the origin. The rotational degeneracy was eliminated by rotating each sampled conformation to minimize its mean-square deviation from the reference isomer conformation using the procedure of Ref. 34. The formal justification for this procedure will be described in a subsequent publication.
-
-
-
-
30
-
-
85033292435
-
-
note
-
-5.
-
-
-
-
31
-
-
85033313169
-
-
note
-
i.
-
-
-
-
32
-
-
85033279885
-
-
note
-
BT=0, i.e., when script C sign was determined just using the Hessian. This is probably so only because this problem is relatively simple - we expect that script C sign derived from the Hessian will be much less useful in macromolecular problems. A stable bi-Gaussian approximation was not obtained at temperatures much above ≈2.5 kcal/mol. At higher temperatures the iterative self-consistent quasi-harmonic fitting method (Ref. 29) would not converge to model each metastable state separately - the separate solutions became unstable and only a single Gaussian modeling the combination of both states was stable.
-
-
-
-
33
-
-
85033321284
-
-
note
-
X).
-
-
-
|