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1 ynamics, experiencing both thermal kicks and viscous drag.
2 ting equilibrium before coming to stop under viscous drag.
3 be expected if the dynamics were governed by viscous drag.
4 endent relaxation spectrum, as expected from viscous drag.
5 phases for outer hair cells' force to cancel viscous drag.
6 xternally and when the enzyme is loaded by a viscous drag.
7 enerates viscosity and single-molecule-scale viscous drag.
8 more lipid molecules and experienced greater viscous drag.
9       These lags may contribute to canceling viscous drag, a requirement for many models of cochlear
10 iments is presented here, which includes the viscous drag acting on the moving fiber and the interact
11 erated by transcription could be retained by viscous drag against the long template, these results ar
12 nt degradation of sensing performance due to viscous drag and relies on the availability of capture m
13 insensitivity of kinetochore velocity to its viscous drag and the large redundancy in its stalling fo
14 aser power because of the anisotropy of both viscous drag and trapping forces.
15 icrotubules, including their charge density, viscous drag, and flexural rigidity.
16 escribes the dependence on the elastic load, viscous drag, and the mass.
17 tive resistive force theory with an acquired viscous drag anisotropy.
18 opagation mechanism while avoiding the large viscous drag associated with a net rotation of the broad
19   With continuing flow into the mantle drip, viscous drag at the base of the remaining approximately
20 n is generally thought to result mainly from viscous drag by the surrounding fluid.
21 higher-flow states, inertial forces overcome viscous drag, causing a flatter profile.
22 considers the angular dependence of both the viscous drag coefficient of the cell and the torque prod
23 ion, the polymer persistence length, and the viscous drag coefficient.
24                   In the described method, a viscous drag created by transient rotational flow stretc
25 s radius of elastase moiety, indicating that viscous drag directly affects the protease translocation
26                  However, propulsion in such viscous drag-dominated fluid environments is highly cons
27 nsport of mass at low Reynolds numbers where viscous drag dominates inertia.
28             Because the energy dissipated by viscous drag exceeded the work provided by the stimulus
29 endence of rotation indicated that the lower viscous drag experienced by spherical spindles prevented
30               Moreover, it is shown that the viscous drag force exerted by flow on a translocating DN
31 ical traps, but the addition of a continuous viscous drag force from the microfluidic flow introduces
32                                  By applying viscous drag force to contracting V. convallaria in a mi
33 g protease translocation and a counteracting viscous drag force.
34 ude of an applied force and on the effective viscous drag force.
35 orces due to pH-dependent protein charge and viscous drag forces caused by electro-osmosis.
36                       Competing magnetic and viscous drag forces helped to enhance the interaction be
37                                              Viscous drag forces on deflecting microtubules in electr
38 esumably due to the high shear stress or/and viscous drag forces operating there.
39             This phase lag is largely due to viscous drag forces, which are higher during crawling as
40 ary forces, lithospheric body forces, and/or viscous drag from mantle flow.
41             This may be due to the effect of viscous drag from surrounding nurse cells together with
42 ow models predict symmetric upwelling due to viscous drag from the diverging tectonic plates, but hav
43  produces negative damping that counters the viscous drag impeding traveling waves; targeted photoina
44 ermined the distance-dependent change of the viscous drag in directions perpendicular and parallel to
45 ed, non-monotonic variation in run length as viscous drag increases.
46 ved spread in this distribution is caused by viscous-drag-induced velocity fluctuations that are corr
47                            It was found that viscous drag is more effective than elastic load in enha
48 s diffusion-based shortening is countered by viscous drag, leading to an unexpected, non-monotonic va
49 alysis of bead motion showed the increase in viscous drag near the surface; we also found that any el
50 tional fog collectors remains low due to the viscous drag of fog-laden wind deflected around the coll
51 tate) that drives actin movement against the viscous drag of myosin heads strongly bound to actin (Hi
52 of the resting tension: to help overcome the viscous drag of the hair bundle during the oscillatory m
53 cal analysis shows how the interplay between viscous drag on filaments and motor-induced forces gover
54 he self-organizing fast phase is a result of viscous drag on kinesin-driven cargoes that mediates equ
55 tudy this problem, we suddenly increased the viscous drag on motors by a large factor, from very low
56 imulations included physiologically relevant viscous drag on the cargo and interrogated a large param
57 internal frictional forces that can dominate viscous drag on the micrometer-sized hair bundle.
58  of single semiflexible filaments subject to viscous drag or point forcing.
59 ale, where locomotion is challenged by large viscous drag, organisms must generate time-irreversible
60                         eNOS is activated by viscous drag/shear stress in blood vessels to produce NO
61 hat OHCs are more effective in counteracting viscous drag than providing elastic energy to the system
62 at these cell-surface interactions provide a viscous drag that increases with the elastic modulus of
63         With a reasonable assumption for the viscous drag, the estimated limit is 10-13 kHz, exceedin