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 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

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

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

14 Attractive forces at short-range stabilize such crossove

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

48 This attractive force follows from the internal-energy contri

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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