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1 dded adhesion within the local region of low electrostatic energy.
2 ding reductions in the supercoil elastic and electrostatic energies.
3 imated from the intramolecular hydrogen bond electrostatic energies.
4 select complexes with lowest desolvation and electrostatic energies.
5 analyzed in terms of both bond distances and electrostatic energies.
8 defects, adds hydrogen atoms and calculates electrostatic energies and the corresponding electrostat
9 accompanied by a significant lowering of the electrostatic energy and a rise in the surface area of t
10 , allowing us to explore the balance between electrostatic energy and ligand desolvation energy in a
11 is a result of the molecule reaching a lower electrostatic energy and the formation of the highly fol
14 rges, we measure ~200 millielectron volts of electrostatic energy arising from electron-hole separati
15 on potential energy functions that treat the electrostatic energy as a sum of pairwise Coulombic inte
16 g surfactant Survanta by inducing steric and electrostatic energy barriers analogous to those that pr
17 roughly estimated from the van der Waals and electrostatic energies between the glutathionyl moiety a
18 select among final states that have the same electrostatic energy, but differ dramatically in elastic
24 actions, and (3) decreased unfavorable total electrostatic energies (Coulombic plus desolvation).
28 compared with differences in the calculated electrostatic energies for a wide range of Cyt/RC config
29 ration scheme to rationally modulate surface electrostatic energies for crystallographic-selective gr
30 s a reasonable description of the underlying electrostatic energies for monovalent ions, but large de
31 um mechanics region and to ensure consistent electrostatic energies for reactants, transition states,
36 folding, and augmenting them with a focus on electrostatic energies, has led to models that are parti
37 energy (hydrogen bonding, van der Waals, and electrostatic energies), in agreement with previous muta
38 ropy compensates significantly for the large electrostatic energy increase due to closer-packed P bac
39 d is maximum at the surface of each ion, the electrostatic energy is dominated by the Born energy; in
42 ant free energy contributions, including the electrostatic energies of the generated charges, the ene
43 ation of the leaving group, and the relative electrostatic energies of the heterocycles in the transi
45 general relationship between the calculated electrostatic energy of a charged residue and its degree
46 curvature stress, due to alterations in the electrostatic energy of dioleoylphosphatidylserine bilay
49 imple model is described for calculating the electrostatic energy of lipid domains at the air-water i
50 cture in the dataset we calculated the total electrostatic energy of the binding and its two componen
51 ence in ion binding, not a difference in the electrostatic energy of the condensed state as previousl
53 rate of PTR in proteins is determined by the electrostatic energy of the transferred proton as long a
55 favor the complex formation while the total electrostatic energy predominantly opposes the binding.
56 ole in stabilizing the micelles, whereas the electrostatic energies present a stable but minor energe
57 occupancy could be due to a decrease in the electrostatic energy profile for K(+) throughout the por
58 x-rays reveal a highly ordered state with an electrostatic energy significantly exceeding the thermal
61 implementation that allows the inclusion of electrostatic energy terms, important to the interaction
62 n contribution to the binding is usually the electrostatic energy, the geometries are not always dete
64 the corresponding large reduction in overall electrostatic energy (which would otherwise arise from p
65 n of shape complementarity, desolvation, and electrostatic energies, which suggests a dimeric arrange
66 ion enhances dipolar interactions and lowers electrostatic energy, which may provide an energy source
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