ライフサイエンスコーパス: deformation

1 ticity stabilizes neurons against mechanical deformation.

2 solid materials can cause extreme damage and deformation.

3 aining their electrochemical functions under deformation.

4 that govern superlattice elastic and plastic deformation.

5 ctive index of the polymer resulted from the deformation.

6 he east, north, and up components of surface deformation.

7 s that buffer membrane tension through their deformation.

8 ase (MMP)-independent migration, and nuclear deformation.

9 r soft robotics, e-skin) must operate during deformation.

10 erential effects along specific LV planes of deformation.

11 ) that eventually lead to irreversible viral deformation.

12 tural processes that drive shock-wave-driven deformation.

13 eta-sheets, which marks the onset of plastic deformation.

14 als demonstrate dislocation-mediated plastic deformation.

15 ignificant air trapping and reduced regional deformation.

16 le remaining slightly curved after the first deformation.

17 ectrical resistance is sensitive to physical deformation.

18 re component as a result of fatigue-assisted deformation.

19 e (Tg), by subjecting them to active plastic deformation.

20 lity of the cell to withstand forces without deformation.

21 ntity has annular dilatation without leaflet deformation.

22 ts in failure in bone formation and skeletal deformation.

23 oving C. elegans undergoing large motion and deformation.

24 is opposed by passive resistance to network deformation.

25 tracking neurons in brains undergoing large deformations.

26 elastic behavior of this material over large deformations.

27 aterials that undergo predominantly uniaxial deformations.

28 ving materials and devices, even under large deformations.

29 materials that undergo predominantly biaxial deformations.

30 cell mechanical response to large-amplitude deformations.

31 macroscopic shape after repeated mechanical deformations.

32 e devices capable of withstanding mechanical deformations.

33 of motion of the iodine atoms enables large deformations.

34 By simulating skin deformations across the palmar surface of the hand and t

35 r adverse LV remodeling and more impaired LV deformation after STEMI compared with those with normal

36 on of our theory to account for irreversible deformations allows us to explain the time scales and th

37 on of this interfacial portion to macroscale deformations along the tooth's normal is maximized when

38 rs (SLBs) as well as profiling the extent of deformation among adsorbed vesicles.

39 n was observed between the degree of droplet deformation and an increasing [Formula: see text].

40 Motion-induced neuron deformation and damage are associated with several neuro

41 ot readily explain the observed variation of deformation and deep structures along the collisional zo

42 These data revealed significant deformation and degradation of ovary tissues and associa

43 n of particle rearrangement, rotation, local deformation and diffusion, and grain growth.

44 Our model resolves the large deformation and dynamics of each individual red blood ce

45 on the evolution of the saltmarsh, coseismic deformation and earthquake recurrence in a wide area of

46 tion and evolution mechanisms during plastic deformation and failure at the mesoscales.

47 Here we explore the deformation and failure behaviour of a representative fo

48 eories to predict the anomalous behaviour in deformation and failure mechanisms of nc-silicene.

49 alyzed to reveal details of the atomic-level deformation and flow processes of amorphous creep in res

50 f cell-ECM adhesion, leading to reduced cell deformation and force transmission across amnioserosa ce

51 ravated due to bending-induced local plastic deformation and Li-filaments pulverization.

52 e and fluid pressure conditions control rock deformation and mineralization on geological faults, and

53 a high flux (85 mum/s) leads to significant deformation and mostly irreversible deposition.

54 Our results imply that deformation and mountain building significantly post-dat

55 nd presents new possibilities for controlled deformation and patterning of liquid crystals.

56 n the precipitate and matrix, during tensile deformation and stress relaxation at 973 K, which provid

57 Understanding this deformation and the associated defects that are created

58 We found three key mechanisms govern the deformation and thus mechanics of the layered C-S-H: dif

59 at excessively focus on detecting mechanical deformations and cracks.

60 tify a wide range of qualitatively different deformations and internal rearrangements.

61 a diamond-like film, producing both elastic deformations and sp (2) to sp (3) chemical changes.

62 TV deformations and their association with right heart remo

63 herent precipitates and thus produce plastic deformation), and we envisage that this lattice misfit d

64 ane shapes, energy estimates for the cost of deformation, and a snapshot of the equilibrium configura

65 irect observation of oil droplet deposition, deformation, and detachment during separation and cleani

66 ell migration, proliferation, rearrangement, deformation, and ECM dynamics have varied roles in drivi

67 main controls the largest monitored seismic, deformation, and geochemical unrest at the caldera.

68 tion to circular shape, shear stress-induced deformation, and rapid fluorescence recovery after photo

69 examined the microstructure of samples after deformation, and so are complicated by post-shock anneal

70 ation, in the form of dislocations and shear deformations, and nascent order in the perpendicular mod

71 achitic changes, hypomineralized long bones, deformations, and signs of fractures.

72 otropic bulk nanocomposite using a multistep deformation approach, which consists of oriented hard-ph

73 ttice level, the basic mechanisms of plastic deformation are twinning (whereby crystallites with a mi

74 Out-of-plane tissue deformations are key morphogenetic events during plant a

75 Networks dominated by biaxial deformations are robustly contractile over a wide range

76 Speckle tracking-based deformation as a feasible and sensitive LA mechanical as

77 anding of the electrically-induced wrinkling deformation as a function of the deformable elastic film

78 egrees of flow shear stress-induced membrane deformation, as determined by different bubble standoff

79 d gravitational forces to study time-varying deformation associated with normal faulting.

80 ducers, ensure resilience against mechanical deformations associated with textile and skin-based on-b

81 olution of the elastic strain during tensile deformation at 973 K.

82 extent of ionic strength-modulated liposome deformation at both low and high surface coverages.

83 examine the nonlinear flow of a glass under deformation at finite strain rate.

84 the heterogeneous nature of MG structure and deformation at the atomic scale.

85 Deformation-based morphometry analyses confirmed early p

86 The deformation behavior is driven by a diffusion-controlled

87 l to understanding and analyzing the plastic deformation behavior of omega-Zr or mixed alpha-omega ph

88 rs at decreasing size leads to the different deformation behaviors.

89 ves greater accuracy for proteins with large deformations but also runs as fast or faster than many o

90 ains, suggesting a possible role in membrane deformation, but they have been relatively uncharacteriz

91 s study, we estimated the extent of caveolar deformation by measuring the density of caveolin-1 proje

92 sized that measures of regional longitudinal deformation by speckle-tracking echocardiography predict

93 ose a model for a mechanism by which nuclear deformation can lead to DNA damage.

94 This morpholine moiety deformation can take place largely independently from th

95 Bending and twisting deformations can be created under IR irradiation, throug

96 vities, while networks dominated by uniaxial deformations can be tuned from extensile to contractile

97 le rats develop early subclinical myocardial deformation, cardiac hypertrophy via elevated expression

98 n model to demonstrate that short-wavelength deformation causes drainage directions to diverge from l

99 e present a hypothesis in which the membrane deformation changes upon channel opening.

100 hery and the bulk can be enhanced by dynamic deformation comparable to that observed in neutrophils.

101 We found that flow-induced microchannel deformation contributes significantly to the change in e

102 ate that fluid flow associated with the cell deformation contributes to the motion of small acidic or

103 flow sensors based on the concept of elastic deformation could be designed for in situ monitoring and

104 iffening and/or dependence of mechanotype on deformation depth.

105 Local mechanical tissue deformation determines PVEM induction via stretch-activa

106 ity switching is realized by controlling the deformation direction and kinematics.

107 The boundary condition affects the deformation dramatically, potentially much more than typ

108 nging, as the abdominal organs undergo major deformations due to manipulation, respiratory motion, an

109 use they undergo very large brain motion and deformation during animal movement.

110 Visco-plastic deformation during cooling was found to be dependent on

111 erials and devices, which frequently undergo deformations during applications.

112 tabilizes interpolar MTs, preventing spindle deformations during movement, and we show that this acti

113 f the four honey types, as recorded by small-deformation dynamic oscillation in shear, micro- and mod

114 materials, we uncover a regime of universal deformation dynamics.

115 The deformation-enabled energy-generating process makes the

116 nnel, which partially alleviates the bilayer deformation energy associated with channel formation.

117 Brownian motion, gravity, and cell membrane deformation energy.

118 re the driving pressure Deltap, maximum cell deformation epsilonmax, and entry time tentry of cells i

119 e created honeycombs with different modes of deformation, exceptional specific stiffness, and stiffne

120 gneiss, by combining the results of triaxial deformation experiments carried out while monitoring mic

121 Here we have carried out the deformation experiments of pPv-(Mg0.75,Fe0.25)SiO3 using

122 mechanism of these earthquakes by performing deformation experiments on dehydrating serpentinized per

123 n vivo population average templates; 2) used deformation fields obtained during optimized nonlinear r

124 extension velocities increase over time and deformation focuses along lithosphere-scale detachment f

125 the maximum size for pure diffusion-mediated deformation (for example, Coble-type creep).

126 The characteristics of surface deformation from field surveys are consistent with dike-

127 m of uplift of the seafloor landward of the deformation front, at the eastern edge of the trench.

128 ng seaward, at least, to within 6 km of the deformation front.

129 zation above a threshold stress and that the deformation-generated heat leads to nanocrystallization.

130 kPa), and the capability to undergo extreme deformations (>600% strain).

131 hear-sliding process, reflecting the plastic deformation has fractal structure at the temperature of

132 ng large-scale sliding of CTBs to facilitate deformation has thus far not been reported.

133 of impressive examples, demonstrating large deformations, high motion complexities, and varied multi

134 sed to investigate the mechanics of particle deformation history.

135 Correspondence between surface deformation, hydrological loading and seismicity rates a

136 Time dependent plastic deformation in a single crystal nickel-base superalloy d

137 of stresses at interfaces and reduce contact deformation in manmade materials.

138 fundamental mechanism of stimuli-responsive deformation in plants, namely that inflexible elements w

139 nsequences as indicated by profoundly higher deformation in real-time deformability cytometry.

140 ity beta (the power-law exponent of the cell deformation in response to a step change in pressure).

141 ells can form an actin cap to resist nuclear deformation in response to physiological mechanical stre

142 us phase, which was mainly driven by plastic deformation in solid state introduced by ultrasonic vibr

143 sessment of regional longitudinal myocardial deformation in the inferior region provided incremental

144 ld induces force on the micro-magnet causing deformation in the polymer around the microcavity.

145 her established the explicit role of plastic deformation in this newly reported sub-Tg solid-state bo

146 urvature of FtsZ filaments promotes membrane deformation in vitro, but its role in division in vivo r

147 and that CAFs generated significantly larger deformations in 3D gels compared to normal fibroblasts.

148 es to analyze cell motion and compute tissue deformations in 4D.

149 Our theoretical analysis of elastic deformations in a lipid bilayer shows that stiffer lipid

150 quid crystalline phase arise from defects or deformations in another phase upon crossing a phase tran

151 Through tracking of tissue-level deformations in the heart-forming region (HFR) as well a

152 The nanopillars create localized deformations in the material resulting in the quantum co

153 ntrations and is relieved via twist and bend deformations in this unique configuration.

154 On a larger scale, deformations in Type I collagen vary with a periodicity

155 an be programmed to undergo stimulus-induced deformations in various geometries, including in respons

156 tter includes a 3D structural sensitivity to deformation, including microscale muscle filament overla

157 h of the coastline; and widespread anelastic deformation, including the 8-meter uplift of a fault-bo

158 regional cell behaviours may lead to tissue deformations, including anisotropies and curvatures, whi

159 akotsubo cardiomyopathy had impaired cardiac deformation indices (reduced apical circumferential stra

160 ndices, and (3) evaluate the potential of RA deformation indices to predict clinical outcomes.

161 s compared with controls, (2) compare the RA deformation indices with Doppler indices of diastolic dy

162 water storage to produce observable surface deformation, induce crustal stresses and modulate seismi

163 Our results show that brain tissue deformation induced by head impact loading is greatest i

164 tile impact testing technique, we discover a deformation-induced 9R phase with tens of nm in width in

165 s that allow the hole to be closed after the deformation-induced strains are reduced by leakage of th

166 ry air trapping, and registration-based lung deformation (inspiration vs expiration).

167 to base-pair slippage of this sequence upon deformation into a catalytically relevant geometry.

168 g which of these mechanisms is active during deformation is challenging.

169 rminants of cell migration show that nuclear deformation is not a critical factor associated with the

170 rropericlase, we suggest that 50% or less of deformation is sufficient to explain the origin of the s

171 sible damage to microstructure during cyclic deformation, leading to cyclic responses that are unstab

172 als in these regions fail to sustain further deformation, leading to voids formation and cracks propa

173 ct with the erythrocyte followed by dramatic deformations linked to the function of the Erythrocyte b

174 ent resilience against mechanical stress and deformation, making it a promising wearable platform for

175 zation boundary through a well-characterized deformation matrix.

176 sensors are tested for robustness for cyclic deformation, maximum stretchability, durability, and bio

177 icles and that is able to perform mechanical deformation measurements.

178 This study sheds lights on a deformation mechanism in metals with high stacking fault

179 This cyclic deformation mechanism is distinct from the conventional

180 In this work, we investigate the deformation mechanism of auxetic hierarchical rotating s

181 -resistant materials due to a unique layered deformation mechanism that emerges in these architecture

182 d conflicting information about the dominant deformation mechanism.

183 cs of the wave propagation behavior, plastic deformation mechanisms (dislocation nucleation, dissocia

184 simulations to uncover the interface-driven deformation mechanisms in biphase nanolayered composites

185 transmission electron microscopy to examine deformation mechanisms in the medium-entropy alloy CrCoN

186 -depth understanding of its high-temperature deformation mechanisms is essential to further optimize

187 and reveal the temperature intervals of the deformation mechanisms of shape memory alloys.

188 Understanding the deformation mechanisms underlying the mechanical behavio

189 ffusive-controlled and displacive-controlled deformation mechanisms, and strain gradient with local p

190 he atomic-scale coupled diffusive-displacive deformation mechanisms, maximizing ductility and strengt

191 raises fundamental questions regarding creep deformation mechanisms.

192 key features in understanding the governing deformation mechanisms.

193 t to provide detailed insight into competing deformation mechanisms.

194 ess exceeds the yield stress undergo plastic deformation mediated by GND activations.

195 hese hydrogels, including self-healing after deformation, microporous architecture, and stability aga

196 nucleation of recrystallization to the local deformation microstructure in the bulk of a sample of co

197 , as micropipette penetration induces tissue deformation, moving target cells from their initial loca

198 As an example, the deformation of a membrane bilayer following the gel-to-f

199 a dynamically reconfigurable zigzag pattern deformation of a soft helical superstructure is demonstr

200 echanical properties, one must determine the deformation of a tissue in response to a known force wit

201 M experiments can quantitatively measure the deformation of adsorbed particles at low surface coverag

202 The morphogenesis of tissues, like the deformation of an object, results from the interplay bet

203 e same pressure under a much lower force and deformation of anvils.

204 Few quantitative studies on the deformation of caveolae have been reported.

205 hich we then use to rationalize the nonlocal deformation of elastic gridshells to point loading.

206 degrees C showed darker coloration, surface deformation of granules, and a significant reduction in

207 The diverse structure and regulated deformation of lipid bilayer membranes are among a cell'

208 ructure, which in turn affect the mechanical deformation of Mg.

209 The plasticity and endothermicity during deformation of MOFs shows a surprising potential for abs

210 esonant photoexcitation enable the selective deformation of N-H and N-C chemical bonds in 2-thiopyrid

211 tic simulations to correlate the anisotropic deformation of nanocrystalline C-S-H to its atomic-scale

212 ally and theoretically to govern the plastic deformation of nanocrystals over a material-dependent sa

213 tion change of Ag@Au NPLs is impelled by the deformation of polymer matrix under pressure, resulting

214 or hemocompatibility due to reduced membrane deformation of red blood cells and decreased level of re

215 It is shown that elastic deformation of the aorta and of the endoprosthesis induc

216 he success of this approach is metal-induced deformation of the arene ring, which creates temporary r

217 Hence, deformation of the CA hexamer lattice results from the v

218 architecture have suggested that multiphase deformation of the crust and mantle lithosphere leads to

219 droplet are observed to cause a controllable deformation of the droplet and/or oscillation along the

220 olarized photo-carriers that only leads to a deformation of the initial domain wall structure.

221 Focused flow in the upper mantle imposed by deformation of the lower crust localizes uplift, which i

222 Complex deformation of the mechanical structure results in charg

223 lysed by solving Laplace's equation, and the deformation of the medium during the transformation is t

224 The deformation of the Miura-ori unit along the third dimens

225 This can induce deformation of the nucleus which, according to recent ex

226 To ascertain deformation of the optic nerve head (ONH) and peripapill

227 find that only the latter, subject to larger deformation of the Pb-X bond length and X-Pb-X bond angl

228 alues between 78.3 and 161.6 mumol L(-1) and deformation of the protective cuticle.

229 tates integration site selection by favoring deformation of the repeat and the flanking sequences.

230 intramolecular hydrogen bond formation, and deformation of the reverse micelle surface to facilitate

231 l elastic lamina macromolecules with minimal deformation of the sensitive endothelial cell.

232 riginate from the coupling between the local deformation of the tissues (bending) and the water press

233 The deformation of these chains along the b-axis occurs main

234 temperatures and strain rates during plastic deformation of Zr-based bulk metallic glass (BMG).

235 gical shapes could be related through simple deformations of a coordinate system.

236 ransient adhesion disengagement and dramatic deformations of embryonic morphology.

237 For dynamic microscopic systems, elastic deformations of the colloids are usually disregarded due

238 nsidering the effects of elastic and plastic deformations of the fractal asperities.

239 e from revealing localized and heterogeneous deformations of the membrane bilayer at the surface of t

240 odel of the evolution of a hole nucleated by deformations of the nuclear lamina and estimate the hern

241 rity in cultured cancer cells and suppresses deformations of xenograft nuclei in vivo.

242 for evaluating the effects of filament shape deformations on filament stability and interactions with

243 The ability of cells to impart forces and deformations on their surroundings underlies cell migrat

244 les were qualitatively sensitive to liposome deformation only at saturation coverage.

245 rving dynamic changes of the objects such as deformation or change in orientation.

246 ally indicate a simpler picture of continuum deformation over decades but relating this behaviour to

247 the memory of subtle differences in earlier deformation paths must be taken into account when deciph

248 nd breathing MOFs, but is unique because the deformation pattern extends beyond a single unit cell of

249 ic than previously imagined and that octamer deformation plays different roles based on the type of c

250 Then, using the deformation potential theory, we calculate the carrier i

251 op a method to measure the electron and hole deformation potentials using coherent acoustic phonons g

252 They are known to accommodate plastic deformation primarily through their migration, while exp

253 RA deformation properties are significantly altered in pedi

254 In ventricular cardiomyocytes, the membrane deformation protein cardiac bridging integrator 1 (cBIN1

255 chanical properties and underlying molecular deformations, providing new opportunities to control and

256 radius, less than the local first baroclinic deformation radius, thus categorized as submesoscale.

257 We generate extreme localized deformation rates by exciting a target particle via puls

258 represents the ratio of plastic and elastic deformation rates, and provides an explicit relationship

259 ehaviour in which metal-linker bonds undergo deformation rather than cleavage, we then consider coord

260 ding pulsed electrodeposition (PED), plastic deformation, recrystallization, phase transformation, an

261 ocardial strain using a novel cine MRI based deformation registration algorithm (DRA) in a cohort of

262 CT simultaneously records the diffusion and deformation-related morphological changes of the sinteri

263 modify cellular behaviours to generate such deformations remain to be established.

264 After an earthquake, the earliest deformation signals are not expected to be carried by th

265 We find that membrane deformation significantly stabilizes the energy of inser

266 li and migrated towards a shallower aseismic deformation source under Solfatara.

267 ion of these three modes can accommodate any deformation state.

268 lasticity model and comparing the calculated deformation texture with the measurement.

269 nstrate that the IRMOF-74 series undergoes a deformation that is similar to the mechanism behind brea

270 linear elasticity, taking into account large deformation that may arise during the vesiculation proce

271 Hence, the splay deformation that scales linearly with the aggregate leng

272 ls for localized bacteriochlorin chromophore deformations that are suggested to also be responsible f

273 Based on the cyclic deformation, the hydrogel crawlers can move peristaltica

274 between the gamma and epsilon phases during deformation, thus leading to enhanced strength and ducti

275 of global positioning system (GPS) vertical deformation time series to constrain models of monthly h

276 y unappreciated contribution of microchannel deformation to such measurements.

277 g a rheological law that relates the rate of deformation to the local stresses and actomyosin anisotr

278 trophils, bulk cytoplasmic flow couples cell deformation to the transport and dispersion of cytoplasm

279 imated from the propagation depth of plastic deformations to a value of approximately 750-800 mum, su

280 olume expansion by amplifying component-wise deformations to global configurational change via the in

281 ncogenic Hras, and even mutation-independent deformations to the tissue, can also be corrected, indic

282 Despite the glassy regime, the bulk plastic deformation triggered the requisite molecular mobility o

283 loads; instead, another mechanism, known as deformation twinning (the sudden re-orientation of the c

284 Unlike the classical twinning route, deformation twinning initiated through the formation of

285 common quantitative way to describe collagen deformations upon interacting with integrins or matrix m

286 ntegrins or matrix metalloproteinase and DNA deformations upon protein binding.

287 ) (990-940cm(-1)) related to CH out of plane deformation vibration of trans double bond.

288 olayers jam, accompanied by the emergence of deformation waves that propagate away from the boundary.

289 With deformation we find that a three-dimensional (3D) hierar

290 original shape after a significant amount of deformation when they are subjected to certain stimuli,

291 parallel to POPC/POPS 3:1 bilayers (prolate deformation) when at the same time it induces a consider

292 at creates backstresses (the forces opposing deformation) when precipitates are cut by dislocations.

293 ctural materials that accommodate mechanical deformations, which is the fundamental requirement for f

294 blunted by dislocation-slip mediated plastic deformation, while the cracks in the UFG Cu were formed

295 imination arises from the extent of liposome deformation, while the QCM-D measurements yield a more c

296 are expected to carry higher strains during deformation with increasing temperature.

297 bining mechanical measurements of global DNA deformations with FRET measurements of local conformatio

298 rating electronic distortions from intrinsic deformations within the low temperature superstructure o

299 tral shift (2.0 nm/deg twist) for morpholine deformations within these fairly flexible moieties.

300 s on the different styles of Tibetan crustal deformation, yet these do not readily explain the observ