ライフサイエンスコーパス: hydration force

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 as water-filled porous solids, subjected to hydration forces.

8 latively simple electrostatic and solvation (hydration) forces.

9 rs, finding that these are controlled by the hydration force(16-18).

10 ion and a combination of ion-correlation and hydration forces affect the Sr(2+) distribution around D

11 , steric repulsion of coating molecules, and hydration forces against van der Waals attractions.

12 onventional surfactants: the balance between hydration force and entropy.

13 mics of proteins, such as self-organization, hydration forces and ionic interactions received less at

14 he properties of both primary and structural hydration forces and reveal new insights into the interp

15 This is a fundamental study of DLVO and hydration forces, and of their connection, on atomically

16 ctrostatic forces; b), short-range repulsive hydration forces; and c), novel polymer-induced depletio

17 gests an alternative interpretation in which hydration forces are either attractive or oscillatory, a

18 Hydration forces are thought to result from the energeti

19 The weakly oscillating hydration force arises from coalescence and depletion of

20 rands experience repulsive electrostatic and hydration forces as well as bending stress associated wi

21 sults reveal new insights into the nature of hydration forces at interfaces due to our ability to mea

22 In this study, we have investigated hydration forces at the mica-electrolyte interface as a

23 nd numerical calculations, the effect of the hydration force between a conical tip and a flat surface

24 Hydration forces between hydrated, polar, and nonpolar i

25 ral capsid, enabling steric interactions, or hydration forces between the two hydrophilic interfaces

26 the tip will determine the magnitude of the hydration force, but that the averaged hydration pressur

27 his model by testing the prediction that DNA hydration forces can be dramatically decreased by additi

28 atter with fluidity but also can-through the hydration force-control macroscopic properties and give

29 ghlight the difficulty in directly comparing hydration force data from different measurement techniqu

30 ake into account ion-ion correlation and ion hydration forces, DNA topology, and the discrete distrib

31 e argue that the reason for such behavior is hydration force due to the formation of a water shell ar

32 tributed to the presence of strong repulsive hydration forces due to the highly hydrophilic headgroup

33 Our theory based on the hydration force explains an extreme slowdown of water tr

34 The hydration force field accounts for the entropic and enth

35 water and suggesting a greater interlamellar hydration force in DOPS.

36 In general, the contribution of the hydration force is relatively small, but, given the smal

37 be no penalty for the use of sharper tips if hydration force is the dominant interaction between the

38 asured by osmotic stress, follow the form of hydration forces observed with condensed dsDNA.

39 at they experience a monotonically repulsive hydration force owing to structuring of water molecules

40 The numerical results show that the hydration force remains oscillatory, even down to a tip

41 The hydration forces that operate on the microscopic scale o

42 sis of the oscillatory component of a strong hydration force, the subnanometer interfacial structure

43 elasticity and a simple model of charge and hydration forces to derive the force required to pack DN