ライフサイエンスコーパス: attractive force

1 bative enhancement arising from a long-range attractive force.

2 pacing set by the length of the range of the attractive force.

3 n the exhausted adsorbent through interlayer attractive forces.

4 in interactions in the absence of long-range attractive forces.

5 lose proximity, which enhances van der Waals attractive forces.

6 ty of the surface and, thus, the short-range attractive forces.

7 ependence of contact deformation and surface attractive forces (adhesion) on surface interference, an

8 imental observations, from the nature of the attractive force among macroions (counterion-mediated at

9 e change in gel porosity and distribution of attractive forces among gel particles, while below the c

10 A striking observation was that the attractive force amplitudes for all samples collapse to

11 ynamics is due to the presence of a strongly attractive force and collective conformational fluctuati

12 is determined by a balance between the self-attractive forces and a repulsion that arises from posit

13 ed mechanical interaction framework enabling attractive forces and non-spherical agent morphologies a

14 These mosaic charges lead to attractive forces and thereby extreme clustering and col

15 Surface roughness, surface area, surface-tip attractive forces, and topographic images of the native,

16 h experimental results, we conclude that the attractive forces are moderate and do not impose a compl

17 the optimal lipid/protein ratio, additional attractive forces are provided by hydrophobic, van der W

18 ar context to the next, suggesting a lack of attractive forces associated with the two stored represe

19 Attractive forces at short-range stabilize such crossove

20 ormation, the pinnings will be subject to an attractive force because of changes in membrane fluctuat

21 conditions, theoretical calculations show an attractive force between a particle and a flat surface.

22 One subject of significance is the attractive force between dsDNA mediated by polycations o

23 It was shown that the attractive force between homologous protein molecules is

24 arlo simulations that there is a short-range attractive force between identical macroions in electrol

25 In agreement with QCM results, an attractive force between MS2 and the pristine membrane w

26 tions involving counterions can induce a net attractive force between negatively charged strands of D

27 e results indicate that a counterion-induced attractive force between nucleic acid duplexes is not si

28 significantly different from the well-known attractive force between parallel plates.

29 au-Verwey-Overbeek theory predicted a strong attractive force between PEI-coated MNPs and algae, whic

30 solution, ion correlation induces a possible attractive force between the different parts of the heli

31 Higher NaCl concentrations decrease the attractive force between the histone proteins and the DN

32 /- 0.3 mN/m at pH 6.0, corresponding to 1 pN attractive force between two adjacent MHA molecules.

33 The attractive force between two oppositely charged ions can

34 rion concentration range, a rapidly decaying attractive force between two parallel filaments is produ

35 safety and efficacy, we monitor and regulate attractive forces between a magnetic pill and an externa

36 h axons around, as well as various intrinsic attractive forces between axons that cause axon displace

37 lational modifications moderately affect the attractive forces between bacteria but have severe effec

38 s, which takes place not only because of the attractive forces between each of the hosts and the gues

39 it has been recently revealed that specific attractive forces between ions with the same sign are re

40 g electrostatic repulsive forces to overcome attractive forces between K+ ions and the selectivity fi

41 t, globular "ball-of-yarn," implying strong, attractive forces between monomers.

42 dence for the formation of relatively strong attractive forces between PEG and protein.

43 n-n interactions arise as a result of strong attractive forces between positively charged entities an

44 sigma-Hole and pai-hole bonds are the attractive forces between regions of excess electron den

45 ation interface and need to compete with the attractive forces between subunits to be effective.

46 providing a charged environment in which the attractive forces between the protein molecules is incre

47 Finally, we study the effects that possible attractive forces between the spectrin filaments and the

48 alization of the isolated radical as well as attractive forces between the stacked radicals, govern t

49 Meanwhile, a combination of repulsive and attractive forces between the tRNA and the protein's con

50 ea between the particles and, therefore, the attractive forces between them.

51 dered bilayers can be much stronger than the attractive forces between this same sterol and an exchan

52 proximately 26-36 A, and the strength of the attractive force can reach -0.37 k(B)T/bp for helix leng

53 We discover that the attractive forces cause an increase in the pressure as t

54 ply to conditions where London-van der Waals attractive forces cause particles to be strongly bound i

55 shows that, as a result of relatively strong attractive forces, clusters of two, three, or higher oli

56 assembly of macroions, possibly providing an attractive force contributing to blackberry formation.

57 on dominates at small separations and direct attractive force contribution can-if strong enough-give

58 lsion due to RBC surface charge with osmotic attractive forces due to polymer depletion near the RBC

59 dicted to form stable solitons, in which the attractive forces exactly compensate for wave-packet dis

60 n length scale (~5 mum), where interparticle attractive forces exceed particle weight.

61 decrease of potential and anisotropy of the attractive force field around the crystallites represent

62 However, long-range attractive forces first bring those surfaces close.

63 This attractive force follows from the internal-energy contri

64 Biomolecular recognition entails attractive forces for the functional native states and d

65 LVO calculations, which revealed the highest attractive forces for the interaction between hydrophobi

66 ve model of protein compressibility in which attractive forces from solvent compete with tertiary int

67 ate these mesoscopic phenotypes to increased attractive forces generated by T4P between cells.

68 The competition between attractive forces (H-bonding and aromatic interactions)

69 The strongest attractive forces (i.e. condensing effect) were identifi

70 s IP results in nonmonotonic curves, even an attractive force in a small gap; (2) for some NdFeB magn

71 rface repulsion uncovers weak and unspecific attractive forces in the bilayer that bring the extracel

72 One type of attractive force involves the recognition by alpha-cryst

73 traction and for the separation at which the attractive force is a maximum are presented.

74 sets a time-dependent range beyond which the attractive force is zero.

75 This attractive force is, however, too weak (approximately 5

76 It can only occur if attractive forces keep the proton at the interface.

77 h titanium is mostly mediated by short-range attractive forces observed at higher surface delays.

78 ctural data and propose a model in which the attractive force of fibrillogenesis comes from a structu

79 e bond can be ruptured either by applying an attractive force of ~150 pN or by a repulsive force of ~

80 pproach curves exhibited jump-in events with attractive forces of 97 +/- 34 pN between E. coli and go

81 elices of MOR induce an effective long-range attractive force on individual protomers, both long-rang

82 In order to test the effects of long-range attractive forces on flipping efficiency, we varied the

83 Every biofilm begins with an attractive force or bond between bacterium and substratu

84 The interaction provides a slowly varying attractive force over a small but significant region of

85 at rough hydrophobic surfaces can experience attractive forces over distances more than 30 times grea

86 ion ionic strength regardless of the type of attractive forces present.

87 we explain that the appearance of effective attractive forces results from the field drop inside the

88 pH or increasing salt concentrations, caused attractive forces such as the hydrophobic and cell-prote

89 aining cell adhesion through long-range cell attractive forces such as the van der Waals forces.

90 rops have long been assumed to experience an attractive force that favours their coalescence.

91 roach of the tunnelling probe, implying that attractive forces that depend on hydrogen bonds also hav

92 We calculate the optical attractive forces that occur between 30-nm Au or Ag nano

93 er the balanced interaction of repulsive and attractive forces to form one-dimensional chains, each o

94 The SNARE complex applies attractive forces to overcome the long-range repulsion b

95 d the selective application of repulsive and attractive forces to send or receive single molecules.

96 ium ions are optimized to provide additional attractive forces to stabilize Abeta adsorbed on or inse

97 ic repulsion and the ability of the dominant attractive forces to trap molecules in thermodynamically

98 th a body length of 25 um) while inducing an attractive force toward the wall.

99 Using perylene pi-pi stacking weak attractive forces, we succeeded in synthesizing perylene

100 on the surface of graphene by intermolecular attractive forces while gold nanoparticles are incorpora

101 t low Mason number (the ratio of shearing to attractive forces) while hydrodynamic stresses tend to c

102 oengineered single crystal probes reveals an attractive force with 60(o) rotational periodicity.

103 The intramolecular attractive force with CoHex is larger than with spermidi

104 arged carboxyl or hydroxyl groups that limit attractive forces with the cellular surface.

105 rogen-bearing DOM, pointing at repulsive and attractive forces with the negatively charged cross-link

106 a result of interplay between repulsive and attractive forces within positively charged histones and