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1 s mainly responsible for the large repulsive hydration force.
2 ieve that this is a new manifestation of the hydration force.
3 lculate and compare local hydration maps and hydration forces.
4 drophobic interactions, and repulsive steric-hydration forces.
5 s and with the order-parameter formalism for hydration forces.
6 that anion selectivity by YFP is related to hydration forces.
7 latively simple electrostatic and solvation (hydration) forces.
8 ion and a combination of ion-correlation and hydration forces affect the Sr(2+) distribution around D
11 mics of proteins, such as self-organization, hydration forces and ionic interactions received less at
12 he properties of both primary and structural hydration forces and reveal new insights into the interp
14 ctrostatic forces; b), short-range repulsive hydration forces; and c), novel polymer-induced depletio
15 gests an alternative interpretation in which hydration forces are either attractive or oscillatory, a
18 rands experience repulsive electrostatic and hydration forces as well as bending stress associated wi
19 sults reveal new insights into the nature of hydration forces at interfaces due to our ability to mea
21 nd numerical calculations, the effect of the hydration force between a conical tip and a flat surface
23 ral capsid, enabling steric interactions, or hydration forces between the two hydrophilic interfaces
24 the tip will determine the magnitude of the hydration force, but that the averaged hydration pressur
25 his model by testing the prediction that DNA hydration forces can be dramatically decreased by additi
26 ghlight the difficulty in directly comparing hydration force data from different measurement techniqu
27 ake into account ion-ion correlation and ion hydration forces, DNA topology, and the discrete distrib
28 e argue that the reason for such behavior is hydration force due to the formation of a water shell ar
29 tributed to the presence of strong repulsive hydration forces due to the highly hydrophilic headgroup
33 be no penalty for the use of sharper tips if hydration force is the dominant interaction between the
35 at they experience a monotonically repulsive hydration force owing to structuring of water molecules
38 sis of the oscillatory component of a strong hydration force, the subnanometer interfacial structure
39 elasticity and a simple model of charge and hydration forces to derive the force required to pack DN
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