ライフサイエンスコーパス: tensile

1 c ventilation system that is operated by the tensile actuation of the hybrid muscles caused by dew co

2 imited to bending or torsional motions or as tensile actuators with low work and energy densities.

3 model for the mycelium which reproduces the tensile and compressive behavior of the material.

4 through the nucleation of ripples under both tensile and compressive loading conditions.

5 Here we investigate tensile and compressive strain effects on the WF of rubr

6 omic positions, which reveal regions of both tensile and compressive strain.

7 e also demonstrate that alternating in-plane tensile and compressive strains (less than 0.01%) can be

8 ectrical conductivity within a wide range of tensile and compressive strains.

9 Both silks enhance the room-temperature tensile and flexural mechanical properties of the compos

10 % Ap-SFRP displays a three-fold elevation in tensile and flexural strength, as compared to pure epoxy

11 pure torsion, a competition between MAP tau tensile and MT bending energies is observed.

12 FG for shear (P = 0.013) and comparable for tensile and peel strength (P > 0.05).

13 xhibits markedly different behaviours at the tensile- and shear-type domain-wall solitons.

14 The tensile behavior of a Ni60Nb40 metallic glass (MG) has b

15 ayer graphene (FLG) to enhance conductivity, tensile behaviour and thus, the composite stability.

16 We also show that the sheets' tensile behaviour can be accurately predicted through fi

17 to determine direction- and region-dependent tensile biomechanical characteristics and regional fibri

18 The present study examined the long-term tensile bond strength of resin composite fillings perfor

19 We found that tensile cell stress leads to rapid ACKR2 down-regulation

20 To explore tensile changes across VE-cadherin in live zebrafish, we

21 high reinforcement effect in compression and tensile characteristics is achieved by the formation of

22 Tensile characteristics were determined between temporal

23 ases (decreases) significantly with in-plane tensile (compressive) strain, which agrees qualitatively

24 ed carbon nanotube yarn muscles that provide tensile contraction as high as 16.5%, which is 12.7 time

25 do not require a liquid electrolyte, provide tensile contractions of 11.6% and 5%, respectively.

26 r between the precipitate and matrix, during tensile deformation and stress relaxation at 973 K, whic

27 conductivity of polymer electrolytes during tensile deformation are not well understood.

28 ental evolution of the elastic strain during tensile deformation at 973 K.

29 fracture in pristine silicon versus ductile tensile deformation in fully lithiated silicon.

30 sport and band structure engineering through tensile deformation in low-dimensional materials, and wi

31 fluoroethylene/carbon nanotube layer) during tensile deformation is the key working principle for ele

32 Here, we combine large-scale thermoplastic tensile deformation of collections of Pt-based amorphous

33 ers can be reversibly stretched up to 50% in tensile direction while generating voltage output propor

34 aightening, fibril reorientation towards the tensile direction, elastic stretching and interfibrillar

35 e southern Wasatch Fault at c. 0.5 mm yr(-1) tensile dislocation opening in the eastern Sevier Desert

36 ach to solve for change in volume for simple tensile dislocations.

37 exhibit a combination of yield strength and tensile ductility that surpasses that of conventional 31

38 Remarkable tensile ductility was first obtained in an in-situ Ti-ba

39 At the macroscale they achieve high tensile elasticity (>20%) not found in their brittle-lik

40 anocrystalline metals with the large uniform tensile elongation characteristic of coarse-grained meta

41 wed the greatest flexibility, as measured by tensile elongation.

42 on, implying gradual accumulation of elastic tensile energy in crosslinks followed by rupture.

43 In situ tensile experiments inside scanning and transmission ele

44 Tensile extensions can enhance the thermal conductivity

45 parts can generate hundreds of piconewton of tensile force and promote intense surface-associated mot

46 Fibrotic lung strips responded to tensile force by releasing active TGF-beta1 from latent

47 icient for activation or whether exertion of tensile force by the actin cytoskeleton across the integ

48 n of integrin adhesiveness by application of tensile force by the cytoskeleton, across ligand-integri

49 nding germband, suggesting that an extrinsic tensile force contributed to body axis extension.

50 sed on Schmid's law, the equivalent uniaxial tensile force direction is revealed normal to the trace

51 In chick, the driver of cluster pattern is tensile force from developing smooth muscle, which gener

52 te vinculin activation by talin modulated by tensile force generated by transient associations with F

53 f the embryo, consistent with an AP-oriented tensile force propagating from there.

54 molecules which actin-cytoskeleton-generated tensile force takes when applied through the integrin be

55 Tension wood of angiosperms creates strong tensile force to pull stems upward, while compression wo

56 ntegrin activation, where the development of tensile force yields physiological integrin activation.

57 anical stimuli, including compressive force, tensile force, and shear force as well as indirect forma

58 imes that initially increase with increasing tensile force.

59 t endoderm invagination is the source of the tensile force.

60 dherin plays a key role in sensing polarized tensile forces across the tissue and transducing this in

61 rkably stable under physiologically relevant tensile forces and large strains.

62 uct membrane DNA tension probes to visualize tensile forces at cell junctions.

63 Mapping of tensile forces by laser cutting uncover a developmental

64 er fast loading rates relevant to TBI, large tensile forces can be transmitted to the MTs that can le

65 Thus, tensile forces determine the first spatial segregation o

66 Tensile forces during vessel formation resulted in paral

67 r spindle integrity in mitotic cells so that tensile forces generated at kinetochores do not cause mi

68 Upon experiencing tensile forces generated by neighboring cells, unfolding

69 Drosophila by defining the pattern of global tensile forces in the tissue.

70 Tensile forces increase at the invasive front of cohorts

71 Herein, we show that the exertion of tensile forces on a simplified retinal chromophore model

72 uniaxial cell-induced and externally applied tensile forces on the morphology of vascular networks fo

73 ohesive tissues, the early embryo dissipates tensile forces required by constricting cells via their

74 e we discover subcellular heterogeneities in tensile forces, generated by actomyosin cortical network

75 can be broadly used to measure intercellular tensile forces.

76 stic response of T2DM RBCs subject to static tensile forcing and their viscoelastic relaxation respon

77 tic and dynamic responses of RBCs subject to tensile forcing, using experimental information only on

78 The TC was maximised for strong tensile in-plane strain which produced weak octahedral r

79 CIL leads to collective cell motion, ensures tensile intercellular stresses, and opposes cell extrusi

80 and ligament mechanical properties - maximal tensile load (+17%, P = 0.03 vs. RestTx) and ultimate te

81 e molecular mechanisms through which dynamic tensile loading (DL) regulates changes in chromatin orga

82 ed the molecular mechanisms by which dynamic tensile loading (DL) regulates chromatin organization in

83 esponse of mesenchymal stem cells to dynamic tensile loading based on the contractility state, the pa

84 show that the failure is governed by purely tensile loading for (a/w) < 0.3 for the same (a/l); bend

85 ollagen triple helix unfolding occurs during tensile loading of collagenous tissues and thus is an im

86 ms of collagen fibril activity in skin under tensile loading that virtually eliminate the possibility

87 attering (SAXS/WAXS) during in situ repeated tensile loading to elucidate the relationship between mo

88 ar origin of strain hardening using uniaxial tensile loading, microspectroscopy of polymer chain alig

89 distributions on the specimen surface during tensile loading.

90 ng-to-ordering transition that is absent for tensile loading.

91 anism for ensuring that both compressive and tensile loads are managed well.

92 on as well as a combination of torsional and tensile loads using a coarse-grained computational model

93 ble to withstand substantial compressive and tensile loads, and exhibit a remarkable self-healing eff

94 the scaffolds while the specimens are under tensile loads.

95 t exhibits general biocompatibility and high tensile material properties.

96 tomic force microscopy (AFM) indentation and tensile measurements on acutely isolated mouse spinal co

97 Enthesis tensile mechanical properties were also assessed.

98 Tensile mechanical testing and compositional analysis re

99 With tensile moduli of approximately 9.1 MPa, ultimate tensil

100 The small tensile moduli suggest that the RDT is not resistive to

101 d region- and strain-dependent variations in tensile moduli, associated with regional differences in

102 he performance of a prototype XPL that has a tensile modulus matching normal skin responses at low st

103 ng from 350 to 1100 nm and substrates with a tensile modulus of approximately 4-8 MPa.

104 rn harvesters that electrochemically convert tensile or torsional mechanical energy into electrical e

105 action, nanotube alignment and length on the tensile performance of the composites are factored into

106 The novel cryogenic tensile plasticity is related to the effective accommoda

107 Tensile properties and micro-hardness values are also re

108 synthesis agents, leads to neocartilage with tensile properties approaching those of native tissue.

109 The as-synthesized networks exhibit tensile properties comparable to those of leading thermo

110 r of theoretical and experimental studies on tensile properties of carbon nanotubes (CNT), reporting

111 However, the tensile properties of engineered tissues have remained f

112 wledge, this is the very first report on the tensile properties of macroscopically long and continuou

113 irstly tackles the direct measurement of the tensile properties of millimeter-long MWCNTs that can be

114 chnique, we will be able to directly measure tensile properties of millimeter-long MWCNTs.

115 s and slowly through indirect changes in the tensile properties of the plasma membrane.

116 ron impurity affects the castability and the tensile properties of the recycled Al-Si alloys due to t

117 ch results in nearly sixfold improvements in tensile properties over unstimulated controls, may allow

118 d gradually with a corresponding decrease in tensile properties.

119 anisotropic human neocartilage with enhanced tensile properties.

120 dimensions, employing the CNTs in their high tensile properties.

121 including length, diameter and volume on the tensile properties.

122 at decrease P311 levels could result in less tensile scars, which could potentially lead to higher in

123 lying strain, using a microelectromechanical tensile stage, to the outer shell of a double-walled car

124 2) vs 0.055+/-0.009 mN/mm(2) for no stress), tensile stiffness, construct alignment, and cell size.

125 Tensile storage modulus and heat flow measurements were

126 ion can promote the motion of MVs, while the tensile strain along the armchair direction has the oppo

127 ise of the WF, occurs at approximately 0.05% tensile strain along the rubrene pi-stacking direction.

128 NiAs structure, by applying compressive and tensile strain along the symmetry axis, and calculating

129 Furthermore, we find that uniaxial tensile strain along the zigzag direction can promote th

130 e voltage of the opposite polarity generates tensile strain and switches the magnetization back to th

131 Furthermore, the dynamics of excitons under tensile strain are also investigated; we find that the B

132 for the properties is identified as in-plane tensile strain arising from oxygen vacancies.

133 s a germanium nanowire under a 1.6% uniaxial tensile strain as the gain medium.

134 This shift is indicative of a reduction in tensile strain by ~0.25%.

135 Micro-Raman studies reveal a large tensile strain change with GeSn thickness, which arises

136 alf-fluorination of the GaBi honeycomb under tensile strain could provide a new platform for developi

137 First-principle calculations suggested the tensile strain drastically alters the band gap, and the

138 additional oxygen vacancies created through tensile strain enhance the cobaltite's catalytic activit

139 deplete either in the compressive or in the tensile strain fields around the dislocation.

140 Our data demonstrate a direct role for tensile strain in dictating the lineage choice of NSPCs

141 It is proposed that accumulated transient tensile strain in the excitation region plays a crucial

142 nd Raman spectroscopy reveals a 3.8% biaxial tensile strain in the germanium nanostructures.

143 in is 1.25 eV, the band gap decreases as the tensile strain increases on an average of 100 meV per 1

144 As tensile strain increases, the hole pocket centered at th

145 ological insulator transition under in-plane tensile strain of 2.6% (3.1%) due to the combination of

146 ical properties (tensile stress of 1.45 MPa, tensile strain of approximately 600%, and fracture energ

147 s in ferroelectric PbTiO3 films, mediated by tensile strain on a GdScO3 substrate.

148 y controlled to induce either compressive or tensile strain on supported catalysts.

149 ent magnitude, signalling a benign effect of tensile strain on the carrier transport properties of Mo

150 Here, we investigate the effects of tensile strain on the ion conductivity of thin-film poly

151 ary Hall effect, is reduced by 10 kJ/m(3) by tensile strain out-of-plane epsilon(z) = 9 x 10(-4), ind

152 Wavy structure, of which compressive and tensile strain periodically varied along the CdS NR, lea

153 identified include BeO, GaN, and ZnO on the tensile strain side, Ge, Si, and GaP on the compressive

154 nd experimental results demonstrate that the tensile strain strongly couples the atomic, electronic s

155 redict half-fluorinated GaBi honeycomb under tensile strain to harbor a quantum anomalous Hall (QAH)

156 amplitude, and orientation as a function of tensile strain to resolve the crack-free structural tran

157 With 0.7% tensile strain we report surface-dominated conduction at

158 ypes of mechanical stimuli, such as stretch (tensile strain), occur during CNS development and trauma

159 n increases on an average of 100 meV per 1% tensile strain, and the decrease in band gap is mainly d

160 ly engineered inks that can withstand severe tensile strain, as high as 100%, without any significant

161 es (0.2 eV for HgTe and 0.05 eV for HgSe) by tensile strain, which far exceed those of current experi

162 und to further split into two branches under tensile strain-low buckled and high buckled structures,

163 g voltage output proportional to the applied tensile strain.

164 phases, their structure becomes planar under tensile strain.

165 cies and the additional effects from elastic tensile strain.

166 teady and linear growths with respect to the tensile strain.

167 pressive strain and decrease with increasing tensile strain.

168 enhanced atom density formed to relieve the tensile strain.

169 nt of T( *) in SmB6 under the application of tensile strain.

170 gs on the self-tuning of the compressive and tensile strained domain ratio along the interface depend

171 A model of coexistent compressive and tensile strained domains is proposed to understand the e

172 structural change takes place in case of the tensile strained film, which undergoes an MIT, but is ab

173 temperature is lowered that is also seen in tensile strained films.

174 e, we report self-assembled growth of highly tensile-strained Ge/In0.52Al0.48As (InAlAs) nanocomposit

175 2,1/2,1/2) appears in all LNO films, while a tensile-strained LNO film has an additional Q2 = (1/4,1/

176 le moduli of approximately 9.1 MPa, ultimate tensile strains of approximately 325%, compressive stren

177 d top (bottom)-Pt (110) facets undergo large tensile strains that help optimize the Pt-O bond strengt

178 Applying uniaxial tensile strains to the semiconducting few-layer 2H-MoS2

179 roved by 890% and 940% under compressive and tensile strains, respectively.

180 at becomes apparent in TPUs even at moderate tensile strains.

181 showed in-plane compressive and out-of-plane tensile strains.

182 ons ([110] and [-110]) under compressive and tensile strains.

183 sive strains, and reduced by 48% under 1.78% tensile strains; at 77 K, this modulating effect is furt

184 oad (+17%, P = 0.03 vs. RestTx) and ultimate tensile strength (+10%, P = 0.15 vs. RestTx).

185 better mechanical properties, such as higher tensile strength (27.5 MPa) and elongation at break (17.

186 rial cellulose macrofibers yield record high tensile strength (826 MPa) and Young's modulus (65.7 GPa

187 Yet it has astonishing mean tensile strength ([Formula: see text]150 MPa) and fractu

188 ed that Er:YAG + HF had significantly higher tensile strength (p = 0.00).

189 strength (sigma y) of 1260 MPa, and ultimate tensile strength (sigma UTS) of 1400 MPa.

190 The tensile strength (TS) increased up to 50% after the inco

191 We present estimates of ultimate tensile strength (UTS) for two engineered beta-solenoid

192 lf-heal at room temperature with a recovered tensile strength 4 MPa, which is 30% of its original val

193 Cross-linked canna starch could increase tensile strength and elongation of rice noodles.

194 At La content of 1.0 wt.%, the tensile strength and elongation of the alloy was maximum

195 ers especially in terms of low density, high tensile strength and high elongation until breaking.

196 Tensile strength and in vitro cytotoxicity showed no sig

197 The acetylation decreased the tensile strength and increased the elongation of the fil

198 d biomechanical properties by increasing its tensile strength and load.

199 had increased stiffness, providing a higher tensile strength and lower elongation when compared to f

200 The nanoreinforcement improved the tensile strength and modulus of films when added at up t

201 pecific elasticity, contractility, adhesion, tensile strength and occlusivity.

202 al organization simultaneously achieves high tensile strength and strain at breaking by taking advant

203 interfacial fracture properties, such as the tensile strength and work of separation, using atomistic

204 frame at an optimal weight ratio boosts the tensile strength and Young's modulus of the buckypaper/P

205 The average tensile strength and Young's modulus of the CNTs investi

206 hosphonate-treated bone demonstrated reduced tensile strength and Young's Modulus.

207 mposite, in addition to a 27% improvement in tensile strength at 2 wt% addition.

208 n with marked hyperextensibility and reduced tensile strength at high strain but not at low strain.

209 of these mice showed increased stiffness and tensile strength but no altered collagen cross-links.

210 anisms in one material, leading to twice the tensile strength compared to a single-phase HEA with sim

211 Tensile strength for gelatin film significantly increase

212 0 mum and widths exceeding 50 mm and biaxial tensile strength in excess of 3 MPa, were produced by pu

213 antly accelerated closure time and increased tensile strength in mice, and was validated in the porci

214 Tensile strength increased from 0.018N/mm(2) in the cont

215 , the single-phase CrMnFeCoNi alloy displays tensile strength levels of approximately 1 GPa, excellen

216 microscopy, scanning electron microscopy and tensile strength measurements.

217 As a result, an ultra-high tensile strength of 2.4-2.6 GPa, a significant elongatio

218 grees C) and superior mechanical properties (tensile strength of 250 MPa) are achieved due to the int

219 The yield strength of 244 MPa and tensile strength of 274 MPa were achieved in the composi

220 shaped specimens yielded an average ultimate tensile strength of 6.60 MPa and an average failure stra

221 ecombinant GH, enhances collagen content and tensile strength of engineered ligaments, in association

222 ork that causes stresses far beyond the bulk tensile strength of gold.

223 ty of 2.58 mWh g(-1) or 3.6 mWh cm(-3), high tensile strength of over 1000 MPa, and bearable pressure

224 P also provides a mechanism for lowering the tensile strength of the dust layer and aiding dust relea

225 The tensile strength of the film was significantly lower but

226 The tensile strength of the graphene fiber reaches 1080 mega

227 When normalized by weight, the specific tensile strength of the macrofiber is as high as 598 MPa

228 cyclic stress amplitudes much lower than the tensile strength of the materials involved.

229 eriments at stress amplitudes lower than the tensile strength of the metal, we report a history-indep

230 ng buffers (pH < 9) in order to preserve the tensile strength of the polyimide coated fused-silica ca

231 The tensile strength of the resultant fibers reaches ~729 MP

232 o determine whether the collagen content and tensile strength of tissue-engineered ligaments is enhan

233 ligned cellulose nanofibers has a mechanical tensile strength of up to 350 MPa, nearly three times of

234 ntiation in vitro, and exhibit stiffness and tensile strength similar to existing dental materials.

235 the production of flexible fibres with high tensile strength such as polyester and nylon.

236 by intertwining filaments confers shear and tensile strength to the caprock, contributing to its duc

237 to evaluate both the elastic modulus and the tensile strength with a single mechanical test, without

238 rsional ultimate strength, a 29% increase in tensile strength, and a 24% increase in energy to failur

239 orders of magnitude increases in stiffness, tensile strength, and tensile toughness compared to its

240 sity, high electrical conductivity, and good tensile strength, can be synthesized by a method combini

241 sisted nucleation of alpha resulting in high tensile strength, greater than any current commercial ti

242 mpressive properties such as remarkable unit tensile strength, modulus, and resistance to heat, flame

243 For bodies with low tensile strength, our results can explain key morphologi

244 Compared to PVA/CNTs, the tensile strength, Young's modulus and electrical conduct

245 he water vapour permeability increased while tensile strength, Young's modulus and glass transition t

246 ons thanks to its unique combination of high tensile strength, Young's modulus and structural flexibi

247 collagen fibrillogenesis, organization, and tensile strength.

248 Adding fat induced a twice decrease of the tensile strength.

249 igands that interlock as spacers and provide tensile strength.

250 aortas with increased compliance and reduced tensile strength.

251 with reduced stiffness but also reduced scar tensile strength.

252 ent increment of the elastic modulus and the tensile strength.

253 At room temperature, the alloy shows tensile strengths of almost 1 GPa, failure strains of ap

254 s (9300 J m(-3) ), extensibility (800%), and tensile stress (2 MPa).

255 embranes demonstrated higher antifouling and tensile stress (by 31%) when compared to pure PES membra

256 inas without MG have decreased resistance to tensile stress and are softer than controls.

257 nship between cell density and intercellular tensile stress and forces the tissue into a nonmotile st

258 growth in the sepal can generate transverse tensile stress at the tip.

259 resistance of lithiated Si by lessening the tensile stress concentrations in Si structures.

260 ovides great possibilities for generation of tensile stress during femtosecond laser ablation to roll

261 ubule alignment along growth-derived maximal tensile stress in adjacent cells would mechanically isol

262 ther supported a contribution of anisotropic tensile stress in division plane orientation.

263 nd differential growth prescribe directional tensile stress in that region, we tested the putative co

264 ed, resulting in substantial increase of the tensile stress in the lipid bilayer.

265 Here tensile stress is created in thin films of potassium (up

266 ng experiments to probe the effects of large tensile stress is difficult.

267 achieve super-strong mechanical properties (tensile stress of 1.45 MPa, tensile strain of approximat

268 The maximum tensile stress of the optimal hybrid construct was 3.42

269 s propose that division plane orientation by tensile stress offers a general rule for symmetric cell

270 Thermal tensile stress perpendicular to the laser scanning direc

271 Polymer cold-drawing is a process in which tensile stress reduces the diameter of a drawn fibre (or

272 In this model, we considered the maximum tensile stress tangential to the interfacial surface, as

273 mechanical stability of nanobeams under high tensile stress to minimize thermal buckling effects, the

274 Tensile stress-strain curves and polarization light micr

275 pressive buckling should not occur given the tensile stresses across the epidermis.

276 icrotubule arrays, which align along maximal tensile stresses and restrict growth in that direction t

277 steel and highly tolerant to compressive and tensile stresses due to chemical bonding to the substrat

278 reduction in significant levels of residual tensile stresses in the graphite that are 'frozen-in' fo

279 rtening of the molecule that translates into tensile stresses in the range of several to almost 100 M

280 We suggest, therefore, that water-generated tensile stresses may play a role in living collagen-base

281 inages in 2011-2013, each of which generates tensile stresses that promote hydro-fracture beneath the

282 The muscle provides a large tensile stroke (up to 78%) and a high maximum gravimetri

283 icial muscle fibers that can match the large tensile stroke of natural muscles have been elusive.

284 ibers can deliver long-life, hysteresis-free tensile strokes of more than 30% and torsional actuation

285 Tensile (T), shear (S), and peel (P) strength were measu

286 stTx) or 15 min post-exercise (ExTx), before tensile testing and collagen content analysis.

287 hanges in fibrillar structure during in situ tensile testing of sea cucumber dermis, we investigate t

288 An in situ quantitative tensile testing platform is developed to enable the unif

289 The in situ tensile testing reveals the brittle fracture of large-ar

290 A carefully designed tensile testing technique for the MWCNTs is developed, w

291 acro-fracture to each sample using Brazilian tensile tests and measured the permeability of these mac

292 ipitates in a ferritic alloy during uniaxial tensile tests at 364 and 506 degrees C on multiple lengt

293 Tensile tests exhibited changes to mechanical properties

294 Tensile tests indicated that UFG-1 steel had high yield

295 Tensile tests on dried composite films have been rationa

296 sed on spider silk ageing, we conducted nano-tensile tests on the vertical naturally spun silk fibers

297 In addition, tensile tests performed on four dog-bone shaped specimen

298 Information gained from the subsequent tensile tests, in turn, substantiated the proposed adhes

299 rate stable built-in strains ranging from 1% tensile to 0.2% compressive on substrates with different

300 ncreases in stiffness, tensile strength, and tensile toughness compared to its iron-free precursor wh