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1 bative enhancement arising from a long-range attractive force.
2 pacing set by the length of the range of the attractive force.
3 lose proximity, which enhances van der Waals attractive forces.
4 ty of the surface and, thus, the short-range attractive forces.
5 n the exhausted adsorbent through interlayer attractive forces.
6 imental observations, from the nature of the attractive force among macroions (counterion-mediated at
8 ynamics is due to the presence of a strongly attractive force and collective conformational fluctuati
9 is determined by a balance between the self-attractive forces and a repulsion that arises from posit
10 Surface roughness, surface area, surface-tip attractive forces, and topographic images of the native,
11 h experimental results, we conclude that the attractive forces are moderate and do not impose a compl
12 the optimal lipid/protein ratio, additional attractive forces are provided by hydrophobic, van der W
13 ar context to the next, suggesting a lack of attractive forces associated with the two stored represe
15 conditions, theoretical calculations show an attractive force between a particle and a flat surface.
18 arlo simulations that there is a short-range attractive force between identical macroions in electrol
20 tions involving counterions can induce a net attractive force between negatively charged strands of D
21 e results indicate that a counterion-induced attractive force between nucleic acid duplexes is not si
23 au-Verwey-Overbeek theory predicted a strong attractive force between PEI-coated MNPs and algae, whic
24 solution, ion correlation induces a possible attractive force between the different parts of the heli
26 /- 0.3 mN/m at pH 6.0, corresponding to 1 pN attractive force between two adjacent MHA molecules.
27 rion concentration range, a rapidly decaying attractive force between two parallel filaments is produ
28 safety and efficacy, we monitor and regulate attractive forces between a magnetic pill and an externa
29 h axons around, as well as various intrinsic attractive forces between axons that cause axon displace
30 s, which takes place not only because of the attractive forces between each of the hosts and the gues
31 g electrostatic repulsive forces to overcome attractive forces between K+ ions and the selectivity fi
34 providing a charged environment in which the attractive forces between the protein molecules is incre
35 Finally, we study the effects that possible attractive forces between the spectrin filaments and the
37 dered bilayers can be much stronger than the attractive forces between this same sterol and an exchan
38 proximately 26-36 A, and the strength of the attractive force can reach -0.37 k(B)T/bp for helix leng
40 ply to conditions where London-van der Waals attractive forces cause particles to be strongly bound i
41 shows that, as a result of relatively strong attractive forces, clusters of two, three, or higher oli
42 assembly of macroions, possibly providing an attractive force contributing to blackberry formation.
43 on dominates at small separations and direct attractive force contribution can-if strong enough-give
44 lsion due to RBC surface charge with osmotic attractive forces due to polymer depletion near the RBC
45 dicted to form stable solitons, in which the attractive forces exactly compensate for wave-packet dis
46 decrease of potential and anisotropy of the attractive force field around the crystallites represent
50 ve model of protein compressibility in which attractive forces from solvent compete with tertiary int
52 rface repulsion uncovers weak and unspecific attractive forces in the bilayer that bring the extracel
58 h titanium is mostly mediated by short-range attractive forces observed at higher surface delays.
59 ctural data and propose a model in which the attractive force of fibrillogenesis comes from a structu
60 pproach curves exhibited jump-in events with attractive forces of 97 +/- 34 pN between E. coli and go
61 elices of MOR induce an effective long-range attractive force on individual protomers, both long-rang
62 In order to test the effects of long-range attractive forces on flipping efficiency, we varied the
64 The interaction provides a slowly varying attractive force over a small but significant region of
65 at rough hydrophobic surfaces can experience attractive forces over distances more than 30 times grea
68 roach of the tunnelling probe, implying that attractive forces that depend on hydrogen bonds also hav
70 er the balanced interaction of repulsive and attractive forces to form one-dimensional chains, each o
72 ium ions are optimized to provide additional attractive forces to stabilize Abeta adsorbed on or inse
73 ic repulsion and the ability of the dominant attractive forces to trap molecules in thermodynamically
75 on the surface of graphene by intermolecular attractive forces while gold nanoparticles are incorpora
79 a result of interplay between repulsive and attractive forces within positively charged histones and
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