ライフサイエンスコーパス: viscous drag

1 more lipid molecules and experienced greater viscous drag.

2 ynamics, experiencing both thermal kicks and viscous drag.

3 ting equilibrium before coming to stop under viscous drag.

4 be expected if the dynamics were governed by viscous drag.

5 endent relaxation spectrum, as expected from viscous drag.

6 phases for outer hair cells' force to cancel viscous drag.

7 xternally and when the enzyme is loaded by a viscous drag.

8 These lags may contribute to canceling viscous drag, a requirement for many models of cochlear

9 iments is presented here, which includes the viscous drag acting on the moving fiber and the interact

10 erated by transcription could be retained by viscous drag against the long template, these results ar

11 nt degradation of sensing performance due to viscous drag and relies on the availability of capture m

12 insensitivity of kinetochore velocity to its viscous drag and the large redundancy in its stalling fo

13 aser power because of the anisotropy of both viscous drag and trapping forces.

14 icrotubules, including their charge density, viscous drag, and flexural rigidity.

15 escribes the dependence on the elastic load, viscous drag, and the mass.

16 opagation mechanism while avoiding the large viscous drag associated with a net rotation of the broad

17 With continuing flow into the mantle drip, viscous drag at the base of the remaining approximately

18 n is generally thought to result mainly from viscous drag by the surrounding fluid.

19 higher-flow states, inertial forces overcome viscous drag, causing a flatter profile.

20 considers the angular dependence of both the viscous drag coefficient of the cell and the torque prod

21 ion, the polymer persistence length, and the viscous drag coefficient.

22 In the described method, a viscous drag created by transient rotational flow stretc

23 s radius of elastase moiety, indicating that viscous drag directly affects the protease translocation

24 nsport of mass at low Reynolds numbers where viscous drag dominates inertia.

25 Because the energy dissipated by viscous drag exceeded the work provided by the stimulus

26 By applying viscous drag force to contracting V. convallaria in a mi

27 g protease translocation and a counteracting viscous drag force.

28 ude of an applied force and on the effective viscous drag force.

29 orces due to pH-dependent protein charge and viscous drag forces caused by electro-osmosis.

30 Competing magnetic and viscous drag forces helped to enhance the interaction be

31 Viscous drag forces on deflecting microtubules in electr

32 esumably due to the high shear stress or/and viscous drag forces operating there.

33 This phase lag is largely due to viscous drag forces, which are higher during crawling as

34 This may be due to the effect of viscous drag from surrounding nurse cells together with

35 ow models predict symmetric upwelling due to viscous drag from the diverging tectonic plates, but hav

36 produces negative damping that counters the viscous drag impeding traveling waves; targeted photoina

37 ermined the distance-dependent change of the viscous drag in directions perpendicular and parallel to

38 ved spread in this distribution is caused by viscous-drag-induced velocity fluctuations that are corr

39 It was found that viscous drag is more effective than elastic load in enha

40 alysis of bead motion showed the increase in viscous drag near the surface; we also found that any el

41 tate) that drives actin movement against the viscous drag of myosin heads strongly bound to actin (Hi

42 of the resting tension: to help overcome the viscous drag of the hair bundle during the oscillatory m

43 he self-organizing fast phase is a result of viscous drag on kinesin-driven cargoes that mediates equ

44 tudy this problem, we suddenly increased the viscous drag on motors by a large factor, from very low

45 internal frictional forces that can dominate viscous drag on the micrometer-sized hair bundle.

46 of single semiflexible filaments subject to viscous drag or point forcing.

47 ale, where locomotion is challenged by large viscous drag, organisms must generate time-irreversible

48 eNOS is activated by viscous drag/shear stress in blood vessels to produce NO

49 hat OHCs are more effective in counteracting viscous drag than providing elastic energy to the system

50 at these cell-surface interactions provide a viscous drag that increases with the elastic modulus of

51 With a reasonable assumption for the viscous drag, the estimated limit is 10-13 kHz, exceedin