ライフサイエンスコーパス: shear

1 n the magnetopause features a large magnetic shear.

2 pid addition of 15 degrees C water under low shear.

3 eduction in platelet surface area under high shear.

4 rational start due to volume replacement and shear.

5 immobilized collagen in response to arterial shear.

6 into EC function in response to differential shear.

7 cadal Variability and inverted vertical wind shear.

8 ultrasound is thought to rely on convective shear.

9 ompressive strength but offers resistance to shear.

10 entry and thrombus formation under arterial shear.

11 r the gamma/gamma' interface and precipitate shearing.

12 scent labeling of filaments after mechanical shearing.

13 Shearing (1000s(-1)) had a minor impact reducing digesti

14 Arterial shear (1002.6 s(-1)) induced a sustained increase in [Ca

15 issues and that it forms on the membranes of shear-activated endothelial cells.

16 of Kir2.1 results in significant decrease in shear-activated Kir currents and inhibition of endotheli

17 Here, we show that mechanical shear acts as a cue for surface adhesion and activates c

18 For both models, irreversible capture and shearing allow us to tune the dynamic range up to 5 deca

19 rature-dependent experiments focusing on the shear and breathing motions of adjacent layers revealed

20 within Sahelian MCSs through increased wind shear and changes to the Saharan air layer.

21 The desalination performance and aggressive shear and chlorine resistance of these scalable graphene

22 ally, we simulate T2DM RBC suspensions under shear and compare the predicted viscosity with experimen

23 or deep elastic substrates that support both shear and compressional waves, together with surface Ray

24 enotypes of patrolling monocytes in the high shear and pulsatile environment of large arteries in hea

25 inetic energy shows that both the horizontal shear and vertical buoyancy flux are important energy so

26 r 90 d of immersion in water, 50 d of buffer shearing, and 30 d of water flushing, and after repeated

27 lained by describing the competition between shear banding and diffusive relaxation processes, and is

28 ticles in the glass, i.e., the appearance of shear bands of the type observed in metallic glasses def

29 system-spanning instabilities (also known as shear bands), which are typical to the mechanical yield.

30 complished through the operation of multiple shear bands.

31 well-established shear flow that arises from shearing between the reticular lamina and the tectorial

32 plores the temporal scaling behavior induced shear-branching structure in response to variant tempera

33 tests suggests that there are two states of shear-branching structures: the fractal structure with a

34 forming two-phase reactions in microdroplets sheared by sheath gas without using a phase-transfer cat

35 By comparing various conventional (e.g. shear, compression and tension) and nano-indentation loa

36 ere susceptible to disruption under the high shear conditions in glomerular capillaries.

37 g roughness and compliance under wetted high-shear conditions using an adhesive disc that evolved fro

38 modulation, in the form of dislocations and shear deformations, and nascent order in the perpendicul

39 ation to increase muscle perfusion relies on shear-dependent increases in ATP, which can act through

40 that purinergic signaling is responsible for shear-dependent increases in muscle perfusion during the

41 We propose a shear-dependent platelet adhesive model based on the Mor

42 The Piezo1 agonist, Yoda1, potentiated shear-dependent platelet Ca(2+) transients by 170%.

43 In contrast, force applied in the shear direction ([Formula: see text]10 pN per TCR molecu

44 de chains in molecular switches that mediate shear during domain motion.

45 ta to document the evolution of the bulk and shear elastic moduli associated with a polyamorphic tran

46 y of platelet aggregates to withstand a high shear environment.

47 d TMDs in bulk quantity using a liquid-based shear-exfoliation method.

48 hat antigorite dehydration triggered dynamic shear failure of the olivine load-bearing network.

49 harge transport is investigated for solution-sheared films in field-effect transistors demonstrating

50 Third, we subject the T2DM RBCs to shear flow and probe the effects of cell shape and effec

51 st that the coupling between NP geometry and shear flow is an important factor that needs to be accou

52 knob structure and the resulting movement in shear flow is not known.

53 ment of VWF under shear stress in an ex vivo shear flow microfluidic chamber.

54 et flow, in addition to the well-established shear flow that arises from shearing between the reticul

55 ch cells passively roll along surfaces under shear flow, is a critical process involved in inflammato

56 ikely to bind to HA than nonrolling cells in shear flow.

57 n static culture or spherical particles in a shear flow.

58 t the presence of a physiologically relevant shearing flow rate results in very different size and sh

59 onent iC3b and ICAM-1 in shear-free, but not shear-flow, conditions.

60 erging on granular beds submitted to viscous shear flows.

61 robust enough to withstand strong cross-flow shear for a prolonged period (120 h) while maintaining N

62 n (nano-DESI) was developed by integrating a shear-force probe with the nano-DESI probe.

63 eassemble within seconds (self-healing) when shear forces are removed.

64 resonant oscillations due to the presence of shear forces between the probe and the sample surface en

65 ures during LC purification and suggest that shear forces may be relevant for some applications of DN

66 ng a leukocyte adhesion in vitro assay under shear forces mimicking blood flow, we observed that redu

67 t employs dielectrophoretic and hydrodynamic shear forces to overcome these thermodynamic limitations

68 ose, oxidative stress, and elevated vascular shear forces-coexist in patients with diabetes, creating

69 e leukocyte rolling in the vasculature under shear forces.

70 Albeit this alignment is achieved by the shearing forces of syringe delivery, it is also dependen

71 n to complement component iC3b and ICAM-1 in shear-free, but not shear-flow, conditions.

72 Shear heating may occur within the fault but is not requ

73 In this study, a shear horizontal surface acoustic wave (SHSAW) was used

74 is coupled into a microfluidic channel using shear-horizontal surface acoustic waves, producing an ar

75 mpact of two homogenization treatments, High Shear (HS) and High Pressure (HP), on the structure and

76 High oscillatory shear index (OSI) in the grooves between trabeculae, com

77 However, while shear-induced aggregation is important for enhancing cha

78 an glypican-1 is a primary mechanosensor for shear-induced NO production.

79 m in both phase and intensity using a Ronchi Shearing Interferometric technique.

80 roughput sequencing technology, where DNA is sheared into smaller pieces, sequenced, and then computa

81 tability driven by a super-Alfvenic velocity shear is expected to facilitate the transport.

82 cation from extreme and focused hydrodynamic shear is the driving mechanism for the generation of ene

83 However, even when the magnetic shear is too small for spontaneous reconnection, the Kel

84 differential rotation of the solar interior shear-layer (called tachocline).

85 The resistance to shear localization was studied by dynamically-loading ha

86 ility gives rise to remarkable resistance to shear localization, which makes this material an excelle

87 oading hat-shaped specimens to induce forced shear localization.

88 Damping ratio and shear loss modulus can be used to distinguish inflammati

89 ormed, and shear stiffness, storage modulus, shear loss modulus, and damping ratio were calculated fo

90 ilament ejection, whereby a region of highly sheared magnetic field near the solar surface becomes un

91 thromboembolic complications associated with shear-mediated platelet activation.

92 ng to a recently proposed numerical model of shear-mediated platelet activation.

93 by small-deformation dynamic oscillation in shear, micro- and modulated differential scanning calori

94 Shear mode devices with quality-factors at resonance, Q

95 Shear mode solidly mounted resonators (SMRs) are fabrica

96 (TCF) of -67 ppm/K are obtained using this shear mode.

97 Relationships between shear moduli and age were assessed with Spearman correla

98 We also report the elastic and shear moduli as a function of crystallographic orientati

99 No significant differences were found in shear moduli at 28, 56, or 84 Hz or frequency dependence

100 Materials and Methods Liver shear moduli in 24 healthy pediatric participants (13 ch

101 to the melting point, where the elastic and shear moduli vary by a factor of approximately 4 between

102 ulator classification, band gap energy, bulk/shear moduli, Debye temperature and heat capacities.

103 istinct pressure derivatives of the bulk and shear moduli.

104 fluidic approach which allows measurement of shear modulus (G) during flow.

105 Benefiting from extremely high shear modulus and high ionic transference number, solid

106 re pronounced, the step-like increase of the shear modulus diminishes and the Poisson's ratio becomes

107 Shear modulus is used as the representative parameter to

108 was significantly higher when measuring the shear modulus rather than the apparent diffusion coeffic

109 d agreement with the experimentally measured shear modulus.

110 und to make the dominant contribution to the shear modulus.

111 eters (beta = 0.6, P < .001, R(2) = 0.33 for shear modulus; beta = 0.6, P < .001, R(2) = 0.32 for ela

112 nt fluctuations, and mechanical responses to shear, motor motilities, and network rearrangements.

113 suggesting that the treatment process of LS shears MP particles.

114 y extracting kinetic energy from the lateral shear of the background oceanic flow.

115 ted to be related to the horizontal velocity shear of the Kuroshio when it flows northeastward along

116 n break leads to a reduction in the vertical shear of zonal winds and an increase in the static stabi

117 while showing neither cationic migration nor shearing of atomic layers as seen in 2D-layered Li-rich

118 for triple helix unfolding is intermolecular shearing of collagen alpha-chains.

119 The oxygen uptake promotes a reconstructive shearing of the [YbO2] sub-units controlled by the adapt

120 acking fault energy surfaces associated with shearing on nine distinct crystallographic slip modes in

121 ex defect structures, e.g., crystallographic shear planes or modules with differing compositions, whi

122 er porosities, second phase, crystallography shear-planes and oxygen vacancies during sintering.

123 Shear-printing is a promising processing technique in or

124 file and demonstrated the tuneability of the shear profile in the device.

125 anochemical activation achieved by grinding, shearing, pulling, or milling opens unique opportunities

126 ts had six-fold greater baseline retrograde shear rate (P < 0.05) and lower FMD (P < 0.05).

127 ximetry), and brachial artery blood flow and shear rate (ultrasound) were recorded before, during and

128 cylglycerol (TAG) composition and effects of shear rate on the microstructure and texture of fats.

129 As the DNA concentration and shear rate were increased there was a stable wall slip r

130 ion and affected thrombus growth at arterial shear rate, indicating a role for Vps34 kinase activity

131 port in the near-surface layer drives rapid, shear rate-dependent advective segregation.

132 a vacuum-driven capillary viscometer at high shear rates (>500 s(-1)), at which the power law exponen

133 ed to a fibrin matrix over a range of venous shear rates (46-184 s(-1)) for upwards of 30 min, and th

134 ta and can be used over a wide range of flow shear rates ([Formula: see text]).

135 t (p < 0.001) changes during the increase in shear rates and an immediate change after thromboplastin

136 blood was perfused over collagen at arterial shear rates, elevating the hematocrit increased the rate

137 At lower DNA concentrations and low shear rates, the velocity fluctuations were well describ

138 lasma under flow at low to sub-physiological shear rates.

139 Although mechanisms of endothelial shear response have been extensively studied, most studi

140 simulations to determine the nonequilibrium shear response of a typical glass-former, squalane.

141 like factor 2 (KLF2), the major regulator of shear responses, and PROX1, the master regulator of lymp

142 Here, we show that the shear-responsive transcription factor KLF2 is required i

143 lving temperature is given for depicting the shear-sliding process, reflecting the plastic deformatio

144 nt differences between morning and afternoon shear stiffness across all levels and there was very goo

145 ique, we measure phase disorder strength and shear stiffness across five cellular populations with va

146 4), and there were weak correlations between shear stiffness and age across all levels (R </= 0.32).

147 Results Correlations between liver shear stiffness and histologic features were higher at h

148 Further, liver shear stiffness decreased with steatosis and increased w

149 Conclusion Liver shear stiffness measured with US elastography provided b

150 lts demonstrate that MR elastography-derived shear stiffness measurements are highly repeatable, weak

151 magnetic resonance (MR) elastography-derived shear stiffness measurements of the intervertebral disc

152 generation grade and MR elastography-derived shear stiffness of the nucleus pulposus and annulus fibr

153 Liver shear stiffness was assessed in vivo by using US elastog

154 and annulus fibrosus MR elastography-derived shear stiffness with increasing Pfirrmann degeneration g

155 mensional MR elastography was performed, and shear stiffness, storage modulus, shear loss modulus, an

156 erties (e.g., approximately 600% increase in shear storage modulus).

157 While the local microstructural shear strain involved is only approximately 0.017%, the

158 he ratio of imposed shear stress to measured shear strain.

159 en occluding teeth that exceed cortical bone shear strength, thereby permitting access to marrow and

160 portionality constant of 1 over the junction shear strength.

161 wth is distinctly enhanced by elevated fluid shear stress (FSS), the underlying regulatory mechanism

162 pacity in response to acute changes in fluid shear stress (FSS); however, it is not known whether GFR

163 The ABM also considers wall shear stress (WSS) dependent leukocyte TEM and compensat

164 Our simulations reveal elevated wall shear stress (WSS) in wild type and AG1478 compared to g

165 migration; whereas intensities of fluid wall shear stress (WSS) typical of venous or arterial flow in

166 must incorporate design elements that reduce shear stress and avoid stasis to reduce the frequent adv

167 lls did not migrate against the direction of shear stress and increased proliferation rates specifica

168 and decreased by 20% and 22% with increasing shear stress and inhibition of non-muscle myosin II moto

169 sociated with the direction of the mean wall shear stress and of the gradient of harmonic phase-avera

170 es, where it integrates responses to laminar shear stress and regulates junctional integrity through

171 expression analysis after fluid flow-induced shear stress and the relocalization of components of the

172 suggest that pulsed wave stimulation induces shear stress and thus increases algal lipid production.

173 r, little is known about how cues from fluid shear stress are translated into responses that pattern

174 ew model, correlating the optically measured shear stress concentration factor and flexural strength

175 il is an essential driver of EndMT under low shear stress conditions and may promote early atherogene

176 We hypothesised that shear stress counteracts the inflammatory effects of oxi

177 the temporal correlation of the interaction shear stress determines an effective viscosity of the ti

178 , here we sense the evolution of the maximum shear stress distribution on the beams under loading.

179 ses of seabed sediments, the period when bed shear stress due to combined current-wave action under n

180 model and the experimental measurements, the shear stress exerted by the cilia is deduced.

181 llatory, normal laminar and elevated laminar shear stress for a period of 72 hours.

182 weather conditions exceeds the critical bed shear stress for erosion (tau cr ) accounts for 63% of t

183 expression change in response to oscillatory shear stress frequency.

184 sturbed blood flow with increased retrograde shear stress further deteriorates the already impaired e

185 study were: (1) to test whether oscillatory shear stress further exacerbates endothelial dysfunction

186 r stimulated platelets, even if the imparted shear stress has low magnitude and brief exposure time.

187 response of primary rat astrocytes to fluid shear stress in a model of traumatic brain injury (TBI),

188 n and A1A2A3 tridomain fragment of VWF under shear stress in an ex vivo shear flow microfluidic chamb

189 ced expression of the chemokine Cxcl12 Under shear stress in culture, Dach1 overexpression stimulated

190 telets is unclear, despite the importance of shear stress in platelet function and life-threatening t

191 traumatic brain injury (TBI), we found that shear stress induced Ca(2+) entry.

192 Low shear stress induces dedifferentiation of EC through a p

193 The oscillatory shear stress intervention induced significant decreases

194 their crosstalk with the redox system under shear stress is lacking.

195 ered to enhance hemocompatibility and reduce shear stress on blood components.

196 The effect of shear stress on Ca(2+) entry in human platelets and Meg-

197 vealed the significant effect of hemodynamic shear stress on RBC-induced microvascular injury.

198 is suggest that elevated tidal range and bed shear stress optimized mangrove development along tide-i

199 Here, we assessed the impact of shear stress patterns and flow directionality on the beh

200 Blood flow and vascular shear stress patterns play a significant role in inducin

201 ange their migratory behavior in response to shear stress patterns, according to flow directionality.

202 alcium channel, was identified to induce the shear stress phenotypes and cell proliferation in LECs r

203 Haemodynamic shear stress plays a critical role in maintaining endoth

204 We also examined the velocity and shear stress profiles for flow over the permeable layer

205 and platelets with endothelia under vascular shear stress requires mechanically specialized interacti

206 experimental study and mechanistic model of shear stress response.

207 Steady laminar flow induced the classic shear stress responses commonly in blood vascular endoth

208 te laminar flow commonly induces the classic shear stress responses in blood endothelial cells and ly

209 ption rates, nitric oxide production levels, shear stress responses, and TNFalpha-induced leukocyte a

210 release nitric oxide in response to elevated shear stress secondary to metabolic dilatation of arteri

211 spatial and temporal complexity of the wall shear stress should be taken into account when studying

212 at Snail was expressed preferentially at low shear stress sites that are predisposed to atheroscleros

213 s, and improved FMD after accounting for the shear stress stimulus.

214 pathway that translates laminar flow-induced shear stress to activation of lymphatic sprouting.

215 s and G was computed as the ratio of imposed shear stress to measured shear strain.

216 er permeability can be modulated by applying shear stress to the droplet interfaces, inducing flow pa

217 eutrophil rolling over E-selectin at precise shear stress transmits tension and catch-bond formation

218 Shear stress triggers DLL4-dependent proteolytic activat

219 Indeed, shear stress triggers rapid increases in force across PE

220 (TM) cells might detect aqueous humor fluid shear stress via interaction of the extracellular matrix

221 TP in response to changes in blood flow (via shear stress) or hypoxia, to act on P2 receptors on endo

222 Here we demonstrate that fluid shear stress, at arterial flow magnitudes, maximally act

223 Under physiological shear stress, caps of polymerized pFn at bacterial poles

224 essary for SDF-1alpha-induced adhesion using shear stress, cell morphology alterations, and crawling

225 stress induced by diverse mechanisms such as shear stress, DNA damage, and heat shock.

226 al concentrations of high levels of Reynolds shear stress, enstrophy, and temperature fluctuations.

227 ain- or loss-of-function phenotype and under shear stress, platelet translocation pause times on coll

228 ed, from which characteristics such as ideal shear stress, the dislocation Burgers vector, and possib

229 lectin and pilin domains are separated under shear stress, the FimH-ligand interaction switches in a

230 gical functions of S1P are tightly linked to shear stress, the key biophysical stimulus from blood fl

231 In response to oscillatory shear stress, the transcription factors Tal1, Gata2, and

232 interact with endothelia under physiological shear stress, using recently developed live cell imaging

233 nfluences atherosclerosis by generating wall shear stress, which alters endothelial cell (EC) physiol

234 Finally, this shear stress, which can easily be measured in the clinic

235 de by the endothelium in response to luminal shear stress, which increases secondary to arteriolar di

236 ion with rapid relaxation to circular shape, shear stress-induced deformation, and rapid fluorescence

237 ole of the transcription factor Snail in low shear stress-induced EndMT.

238 nction and is protective against oscillatory shear stress-induced endothelial dysfunction in patients

239 gen administration abrogated the oscillatory shear stress-induced increase in CD31+/CD41b- microparti

240 ow) types of ICWs at varying degrees of flow shear stress-induced membrane deformation, as determined

241 Shear stress-induced molecular and cellular responses we

242 siological experiments demonstrate that high shear stress-induced multimeric cochlin produces a quali

243 rosine kinase 2 restores insulin-induced and shear stress-induced NO production.

244 c core size was also reduced in the model of shear stress-modulated vulnerable plaque formation.

245 esion development was assessed in a model of shear stress-modulated vulnerable plaque formation.

246 The mechanisms underlying shear stress-regulation of EndMT are uncertain.

247 We hypothesized that downregulation of a shear stress-sensitive transcription factor, Kruppel-lik

248 in 5% O2 (>5 d) decreased histamine- but not shear stress-stimulated endothelial (e)NOS activity.

249 f superoxide, whereas insulin-stimulated and shear stress-stimulated eNOS activations were blunted.

250 gic (5%) O2 and stimulated with histamine or shear stress.

251 scosity above a critical, material-dependent shear stress.

252 N-cadherin, alpha-SMA) in EC exposed to low shear stress.

253 plications of physiological and pathological shear stress.

254 nced by hyperglycemia, oxidative stress, and shear stress.

255 r 5 minutes in the presence of 1.0 dyn/cm(2) shear stress.

256 bsequently shown by others to be due to lung shear stress.

257 signaling scales with the magnitude of fluid shear stress.

258 an anisotropic hydrogel string under modest shear stress.

259 signaling molecule during cell migration and shear stress.

260 inutes of experimentally-induced oscillatory shear stress.

261 lignment of endothelial cells in response to shear stress.

262 ction is then applied to generate rotational shear stresses in any desired direction.

263 erfaces at the proportional limit under pure shear stresses of torsion.

264 his condensation significantly increases the shear stresses on the packaged DNA while also reducing t

265 Comparison of energy barriers and ideal shear stresses suggests that the favorable modes are pri

266 ntal arcade configurations that concentrated shear stresses, and (3) repetitive, localized biting.

267 d of the gradient of harmonic phase-averaged shear stresses, which surprisingly do not match the over

268 odstream of animals is associated with large shear stresses.

269 ducers, which generates regions of near-zero shear that allow matrix mutants to locally accumulate.

270 progressive work hardening with dislocations shearing the gamma' precipitates, a high dislocation den

271 flexible microfibers, and we demonstrate the shear thickening and gelling behavior of such microfiber

272 Thus, we find that continuous shear thickening arises from increasingly frequent local

273 Shear thickening in dense particulate suspensions was re

274 ase accounts quantitatively for the observed shear thickening.

275 ppresses the frictionless state and also the shear-thickening behavior of the suspension.

276 er gravity, we demonstrate that particles in shear-thickening suspensions are frictionless under low

277 All samples exhibited shear thinning non-Newtonian behaviour.

278 lose to that of water and exhibit negligible shear thinning, focusing occurs over a wide range of ela

279 uest-host interactions, undergo disassembly (shear-thinning) when injected through a syringe and then

280 Here we apply large-amplitude oscillatory shear to a monolayer of separated fibroblast cells suspe

281 ensitive to the density of the two Large Low Shear Velocity Provinces (LLSVPs) beneath Africa and the

282 It seismologically resembles the large low-shear velocity provinces (LLSVPs) under Africa and the P

283 tomographically imaged within the large low-shear-velocity provinces in the lower mantle.

284 fined from the temperature dependence of the shear viscosity, eta (ref.

285 canes is ambient environmental vertical wind shear (VWS).

286 n is sufficient to explain the origin of the shear wave anisotropy observed seismically in the D'' la

287 To evaluate the diagnostic performance of shear wave arrival time contour (SWATC) display for the

288 c radiation force impulse imaging (ARFI) and shear wave elasticity imaging (SWEI) are implemented.

289 luate the potential value of ultrasound (US) shear wave elastography (SWE) in assessing the relative

290 tional B-mode ultrasound characteristics and shear wave elastography parameters were computed.

291 g, acoustic radiation force pulse imaging or shear wave elastography) or steatosis (controlled attenu

292 ntify factors associated with the quality of shear wave propagation (QSWP) in breast lesions.

293 ompared with using the standard deviation of shear wave speed (SWSSD) alone, SWSSD combined with QSWP

294 itions of the D'' layer, which can produce a shear wave splitting anisotropy of approximately 3.7% wi

295 ues, hotspot buoyancy flux, and upper-mantle shear wave velocity to mean that hot plumes-which exhibi

296 nce index higher than 95% and/or no apparent shear waves imaged.

297 t also for mode conversion from surface into shear waves.

298 mode conversion of surface Rayleigh waves to shear waves.

299 ing of tumor cell adhesion under physiologic shear would lead to the development of new diagnostic as

300 43)Am was investigated in a water conductive shear zone under conditions relevant for a nuclear waste