ライフサイエンスコーパス: elastic

1 properties, whereas kafirin masses were more elastic.

2 ntly viscous, whereas the cellular cortex is elastic.

3 Energy storing tendons are more elastic and extensible than positional tendons; behaviou

4 ature, isolated nuclei behaved like passive, elastic and incompressible objects, whose volume depende

5 ing out high-resolution time-of-flight quasi-elastic and inelastic neutron scattering measurements in

6 critical parameters that govern superlattice elastic and plastic deformation.

7 rough surfaces by considering the effects of elastic and plastic deformations of the fractal asperiti

8 the two rOPN forms were further compared by elastic and quasi-elastic incoherent neutron scattering.

9 We also report the elastic and shear moduli as a function of crystallograph

10 nisotropy up to the melting point, where the elastic and shear moduli vary by a factor of approximate

11 are connected in series through a network of elastic and structural proteins.

12 Due to the non-smoothness of the elastic and structural TV penalties, an efficient algori

13 g a common platform for the analysis of cell elastic and viscoelastic properties with arbitrary linea

14 onal and classic processes indicating a more elastic and viscous masa.

15 ly limits plastic flow) and (ii) between an 'elastic' and a 'plastic' film further established the ex

16 g small stacking fault energies and/or large elastic anisotropy, which induce a large anisotropy in t

17 f lipids, the modulated-intensity profile of elastic back-scattered light from an optically-trapped v

18 nd, by measuring the intensity modulation of elastic back-scattered light, changes in the biophysical

19 finder Satellite Observation (CALIPSO) is an elastic backscatter lidar that produces a global uniform

20 gation exhibits parity asymmetry, can remove elastic backscattering and provides robustness against d

21 ils to detect the ligands after calcination, elastic backscattering spectrometry characterization dem

22 s vacancy-mediated migration based on nudged elastic band density functional theory (DFT) simulations

23 Metamaterials with acoustic and elastic band gaps are of great interest to scientists an

24 Interestingly, this elastic behavior is transferable to small networks, wher

25 ed force dependence model, we determined the elastic behavior of the transition state, which we find

26 que in order to provide new insight into the elastic behavior of this material over large deformation

27 Our measurements show that the elastic behaviour of (Al,Fe)-bearing bridgmanite is mark

28 that the zebrafish tailbud is viscoelastic (elastic below a few seconds and fluid after just 1 min)

29 s (the metric tensors) for a given isotropic elastic bilayer to grow into a target shape by posing an

30 Here we apply a new model of elastic-brittle failure to test the alternative view tha

31 The resulting actuated form derives from the elastic buckling of the rods subjected to inextensibilit

32 urrently, water-rich biomedical polymers are elastic but weak.

33 The synthesis process used to make this elastic carbon foam is readily scalable to industrial ap

34 pe arises from the physical properties of an elastic cell wall inflated by internal turgor pressure.

35 a pair of guard cells which have thickened, elastic cell walls to withstand the large increases in t

36 irin visco-elastic masses have a much higher elastic character than zein masses.

37 onstrate the accessibility of a regime where elastic collisions also become relevant for suspensions

38 ation of metal-like thermal conductivity, an elastic compliance similar to soft biological tissue (Yo

39 adient, from high to low, in the plastic and elastic compliances of cell walls along the elongation z

40 e nucleus as an elastic-fluid system with an elastic component (chromatin) and fluid component that c

41 suming that the local volume fraction of the elastic component controls the rate of damage per unit v

42 d for several days at 10 degrees C but their elastic component increased.

43 erm-fluid interaction was facilitated by the elastic component of the fluid.

44 ical, chemico-mechanical biosensors or visco-elastic components.

45 The polymer matrix serves as a microscale elastic connector for the rigid and brittle perovskite a

46 We determine all of the elastic constants of dsDNA and dsRNA and provide an expl

47 The 1D elastic crystals are next modified to two-dimensional (2

48 arying the interaction strengths in these 2D elastic crystals gives plastic crystals with two pairs o

49 ls are next modified to two-dimensional (2D) elastic crystals, of the type 4-bromophenyl 4'-nitrobenz

50 Fits to the elastic data show that the internal tension decreases wi

51 e advantage of the high compliance and large elastic deformability of a soft polymer gel to directly

52 at microflow sensors based on the concept of elastic deformation could be designed for in situ monito

53 It is shown that elastic deformation of the aorta and of the endoprosthes

54 arameter represents the ratio of plastic and elastic deformation rates, and provides an explicit rela

55 rms into a diamond-like film, producing both elastic deformations and sp (2) to sp (3) chemical chang

56 Our theoretical analysis of elastic deformations in a lipid bilayer shows that stiff

57 For dynamic microscopic systems, elastic deformations of the colloids are usually disrega

58 comprehensive approach for creating robust, elastic, designer Lunar and Martian regolith simulant (L

59 th a cell surface to be repelled due to cell elastic distortion, offset by tip-cell adhesion, and ind

60 are difficult to discern from pure nonlinear elastic effects.

61 t that buckled cofilactin filaments localize elastic energy at boundaries between bare and cofilin-de

62 ell-to-cell heterogeneities in SF dissipated elastic energy can be predicted from varying degrees of

63 r conformational changes of the sheath whose elastic energy drives the injection process.

64 into a target shape by posing and solving an elastic energy minimization problem.

65 t genomic delivery machine that is driven by elastic energy stored in a contractile tail sheath.

66 sed on experimentally measured alteration in elastic fiber composition, alveolar geometry and surfact

67 lteration in lung recruitment and diminished elastic fiber density were shown predictive of mechanica

68 ls show enrichment in genes for development, elastic fibers and epigenetic regulation pathways.

69 Elastic fibers are typically decreased.

70 d salt is a critical step in the assembly of elastic fibers in vivo, preceding chemical cross-linking

71 n addition to showing reduced and fragmented elastic fibers, the histopathological hallmark of cutis

72 e consisting of collagen, proteoglycans, and elastic fibers.

73 ined with Miller elastic stain had decreased elastic fibers.

74 Aortas in Adamts-4-/- mice showed reduced elastic fibre destruction, versican degradation, macroph

75 deformation as a function of the deformable elastic film thickness.

76 PA14 cells move actively without forming an elastic film.

77 PAO1 cells form elastic films of bacteria, excreted polysaccharides and

78 The resulting PDMS structures are remarkably elastic, flexible, and extensible.

79 We couple the elastic-fluid model to the kinetics of DNA breakage and

80 We treat the nucleus as an elastic-fluid system with an elastic component (chromati

81 We derived the scaling laws for the elastic force and the force for alpha-to-beta transition

82 erimental data and model demonstrate that an elastic force opposes growth of the utricular sensory ep

83 d positions are coupled by membrane-mediated elastic forces arising from the interaction between the

84 of behaviors illustrates that the degree of elastic frustration can be manipulated by molecular gues

85 gnificant increase of curd firmness and both elastic (G') and viscous (G'') moduli.

86 y(dimethylsiloxane) sponge electrodes and an elastic gel membrane is developed for the first time.

87 ith an exploration of concatenating multiple elastic gridshell building blocks.

88 ctates the zeroth-order shape of an actuated elastic gridshell.

89 Elastic gridshells comprise an initially planar network

90 e to rationalize the nonlocal deformation of elastic gridshells to point loading.

91 We study elastic gridshells with a focus on the rational design o

92 yshev nets can be further used to understand elastic gridshells.

93 address the inverse design of hemispherical elastic gridshells.

94 The theory of elastic group transfer for the binding and release rate

95 sing a periodic assembly of rigid plates and elastic hinges.

96 Previous approaches have often utilized elastic hydrogels.

97 ss to relevant thermodynamic quantities, and elastic incoherent neutron scattering (EINS) that probes

98 By combining elastic incoherent neutron scattering and advanced molec

99 s were further compared by elastic and quasi-elastic incoherent neutron scattering.

100 The mechanism by which elastic inhomogeneity reduces the yield stress is explai

101 ellular matrix protein fibronectin (FN) into elastic, insoluble fibrils is still poorly understood.

102 show cooperative transitions when long-range elastic interactions are present.

103 ilt competition between ferro- and antiferro-elastic interactions provides a SCO behavior that is int

104 ctions (i.e., competing ferro- and antiferro-elastic interactions) drive concerted lattice distortion

105 show that, unlike solid-supported biofilms, elastic interfacial film formation occurs in the absence

106 wearable pressure and force sensing using an elastic ionic-electronic interface.

107 e differentiation by stiffness of individual elastic lamellae and vascular smooth muscle.

108 /-)/IDO(-/-) mice, which presented decreased elastic lamina degradation and aortic expansion.

109 he supporting basement membrane and internal elastic lamina macromolecules with minimal deformation o

110 at in nanoaggregate form, asphaltenes create elastic layers around water droplets enhancing stability

111 e control experiments performed by resonance elastic light scattering (RELS) confirmed MT swelling/sh

112 Elastic light scattering is a standard method to study a

113 Tan delta findings reveal a more elastic-like behavior of the e-GSE-modified dentin matri

114 When deformed beyond their elastic limits, crystalline solids flow plastically via

115 stigated due to their superior strengths and elastic limits.

116 A robotic device applied a lateral elastic load to the object requiring large grip forces f

117 arently necessary for the retention of visco-elastic mass softness with kafirin and zein, and for ela

118 Kafirin visco-elastic masses have a much higher elastic character than

119 s composition much more readily formed visco-elastic masses in water or acetic acid solutions than eq

120 alysis of coacervated zein and kafirin visco-elastic masses showed they were initially soft.

121 shed in this report, paves the way to tailor elastic material parameters through the design of magnet

122 At short times, the bundle behaves as an elastic material, whereas at long times, filaments flow

123 through coacervation and into a cross-linked elastic material.

124 duce a numerical scheme to evolve functional elastic materials that can accomplish a specified mechan

125 retained both after phase separation and in elastic materials.

126 al demonstrating wave propagation through an elastic matrix with embedded resonating units, and nanom

127 perimental quantification captures the ultra-elastic mechanical characteristics of an open mesh micro

128 We observe a drastic elastic-mechanical softening in highly doped BDD relativ

129 Thermalized elastic membranes without distant self-avoidance are bel

130 elongates against the constraint of a thin, elastic membranous tissue, the dorsal mesentery.

131 ld reversals, demonstrating a robust magneto-elastic memory that makes uranium dioxide the hardest pi

132 ork, we design and propose a linear diatomic elastic metamaterial using dual-resonator concept to obt

133 The minimized elastic misfit strain around the particles does not cont

134 on of the force curves using a Maxwell visco-elastic model allows us to extract the bundle mechanical

135 In this work, a three-dimensional continuum elastic model for gramicidin A in a lipid bilayer is sho

136 The resulting elastic model provides a common quantitative way to desc

137 HA is known to swell, fitting a linear elastic model with total tissue pressure (TTP) increasin

138 Moreover, elastic models are much less computationally demanding t

139 Continuum elastic models of the membrane have been widely used to

140 and heat-affected zone exhibit very similar elastic moduli and hardness when compared to the base ma

141 document the evolution of the bulk and shear elastic moduli associated with a polyamorphic transition

142 mple means to extract absolute values of the elastic moduli from purely optical observations.

143 Experimental trends showed elastic moduli increased with body mass, except for huma

144 dies is used to investigate the variation of elastic moduli of lignocellulosic (bamboo) fiber cell wa

145 18 kPa at 5% strain, which is comparable to elastic moduli of mammalian vocal folds.

146 We found that the average elastic moduli of non-neoplastic and tumor-bearing optic

147 loped a simple analytical model for the bulk elastic moduli of skin, which correlated well with exper

148 differences suggest that, in addition to the elastic moduli of the double helix, other factors contri

149 thelial cells observed by measuring cellular elastic moduli using atomic force microscopy.

150 Such properties may include anisotropic elastic moduli, the Schmid factor for primary slip, and

151 -steepening and reduction of the theoretical elastic moduli.

152 manipulated over a relatively wide range of elastic moduli.

153 freestanding membranes with remarkably high elastic modulus (>10 GPa) have been fabricated through t

154 nd tunability of the local piezoresponse and elastic modulus (>23%).

155 A 114% increase in elastic modulus (dry condition), 160% increase in proton

156 k) to decrease monotonically with decreasing elastic modulus (E).

157 cant correlation between tumour necrosis and elastic modulus (r = -0.73, p = 0.026).

158 ng nuclear volume, Poisson's ratio, apparent elastic modulus and chromatin condensation.

159 We find a dose-dependent increase in cell elastic modulus and decrease in cell fluidity with incre

160 measurement parameters on the resulting cell elastic modulus and fluidity.

161 y derive its material properties such as the elastic modulus and poisson's ratio.

162 aller network mesh size, which increases the elastic modulus and robustness, but critically inhibits

163 rol showed a time-dependent increment of the elastic modulus and the tensile strength.

164 Diaphragm elastic modulus assessed by OCT-based indentation was re

165 l actin ring, and diminishes the increase in elastic modulus at the periphery and cytoplasm.

166 Refractive results and the theoretical elastic modulus calculations were evaluated.

167 The reduction of the theoretical elastic modulus correlated with the preoperative SI inde

168 drop tensiometer for interfacial tension and elastic modulus determination with oscillating bubbles.

169 urements, we estimate population averages of elastic modulus E and fluidity beta (the power-law expon

170 lity gives rise to a temperature independent elastic modulus for ceramic and single crystalline super

171 hy (SWE) in assessing the relative change in elastic modulus in colorectal adenocarcinoma xenograft m

172 dentation results show that the longitudinal elastic modulus initially increased to a maximum value a

173 y strengthened with the maximal hardness and elastic modulus of 46.1 GPa and 425 GPa, respectively.

174 ontaining 3-20 vol % Au are found to have an elastic modulus of approximately 6-19 GPa, and hardness

175 These effects correlated with changes in the elastic modulus of fibrin clots.

176 In contrast, elastic modulus of hemicellulose decreases constantly wi

177 of hydrogen bond bridges causes a growth in elastic modulus of lignin at low MC.

178 Elastic modulus of lignin, calculated by molecular dynam

179 Using OCT-based indentation, the elastic modulus of mouse diaphragm was measured from cha

180 he metallic 1T phase of MoS2 nanosheets, the elastic modulus of restacked MoS2 layers (2 to 4 gigapas

181 nd to be responsible for the increase in the elastic modulus of the films.

182 eat-treated chemically-crosslinked gels, the elastic modulus of the physical cryogels was found to in

183 The elastic modulus of the zebra finch ML is 18 kPa at 5% st

184 e mean PTA of 14.42% generated a theoretical elastic modulus reduction of 10.25% in the asymmetrical

185 of soft hydrogel samples with a well-defined elastic modulus using different AFMs revealed that the u

186 requency scanning probe microscopy, collagen elastic modulus was lower in cecal ligation and puncture

187 An average Young's elastic modulus was measured for nucleated cells, enucle

188 Bone mineral elastic modulus was similar at 24 hours but reduced in c

189 ell walls have key roles in the variation of elastic modulus with increasing MC.

190 elf-assembled superlattices have the highest elastic modulus, despite containing significant structur

191 nabling single-cell measurements of apparent elastic modulus, Ea, and power-law exponent, beta.

192 de in diameter and 13 orders of magnitude in elastic modulus.

193 ted with a reduction in collagen and mineral elastic modulus.

194 Despite the elastic nature of Rayleigh scattering, the feedback mech

195 h an additional sparse regression step using elastic net (MCR-ENALS) to distinguish relevant m/z sign

196 An elastic net algorithm applied to the high-dimensional ma

197 An elastic net classifier with 10-14 predictors optimized s

198 andom forests, support vector regression and elastic net penalized regression) were explored.

199 re Independence Screening (ISIS) method with elastic net penalty to DNA methylation levels at 484,548

200 Elastic net regression was used to define the most optim

201 Two generalized linear models with elastic net regularization (14VF and 14GT), based on the

202 The model for CVD chosen through elastic net regularization included interaction terms su

203 el for serious adverse events chosen through elastic net regularization suggested that male sex, curr

204 We perform model selection using elastic net regularization to prevent overfitting.

205 aim was to test if the statistical method of elastic net regularization would improve the estimation

206 We compared the method of elastic net regularization, which uses repeated internal

207 o predictive models (support vector machine, elastic net) and validated those models in an independen

208 significantly improve the performance of the elastic net.

209 Using elastic-net penalized logistic regression, 118 baseline

210 pping genes by a functional extension of the elastic-net regression.

211 systematic coarse-grained modeling using an elastic network model and related modeling/analysis tool

212 rison with the anisotropic network model (an elastic network model) highlights the importance of flex

213 ENM 1.0 integrates two widely used elastic network models (ENMs)-the Gaussian Network Model

214 ary structure of RNA is constrained using an elastic network.

215 The rigidity of elastic networks is characterized by a topological invar

216 del to simulate a force-based destruction of elastic networks representing emphysema progression, whi

217 Quasi-elastic neutron scattering provided quantitative details

218 motion and ion transport by combining Quasi Elastic Neutron Scattering, Pulsed Field Gradient Nuclea

219 eveal a very narrow window of electrical and elastic parameters that allow the existence of bubble do

220 The elastic penalty in the model is introduced for the spars

221 morphological features associated with high elastic performance.

222 the superhelical axis, all superhelices show elastic, plastic, and inelastic elongation regimes and u

223 e) (PGS-PCL) blends were electrospun to form elastic polymeric sheets with fiber diameters ranging fr

224 y and activation volume, based on the thermo-elastic properties (bulk modulus and its derivatives, me

225 supramolecular polymers whose structure and elastic properties can be precisely tuned by controlling

226 heir energetics, structural, electronic, and elastic properties for both the bulk and the single laye

227 eudoxanthoma elasticum, a disease of altered elastic properties in multiple tissues.

228 robust composite material that combines the elastic properties of a polymeric matrix and the extreme

229 Here, we scrutinized the elastic properties of apical membranes separated from li

230 Elastic properties of cells are mainly derived from the

231 ameter, the Young's modulus, to describe the elastic properties of cells.

232 y (AFM) mode to measure the local, nanoscale elastic properties of soft materials like living cells.

233 analysis with force measurements to quantify elastic properties of sound producing medial labia (ML).

234 The elastic properties of such an ensemble are determined by

235 llagen solubilization and sustained the bulk elastic properties over 12 mo.

236 ion of voids in the system and diminution of elastic properties.

237 As such, they display remarkable elastic properties.

238 Here we demonstrate experimentally not only elastic Rayleigh wave rainbow trapping, by taking advant

239 basis for length-dependent activation, titin elastic recoil and refolding of titin domains as an ener

240 spectively, through thermal fluctuations and elastic recovery are key for the aging dynamics.

241 mass softness with kafirin and zein, and for elastic recovery of kafirin.

242 When extended beyond the initial linear elastic regime, the shell undergoes a hysteretic, temper

243 ed by the fabrication process, and a minimal elastic relaxation occurs during the release step, as de

244 he time evolution are identified, describing elastic response ([Formula: see text] ns), inelastic reo

245 We show that the elastic response of our model cytoskeleton, in which the

246 luate refractive results and the theoretical elastic response of photorefractive keratectomy in eyes

247 First, we examine the elastic response of T2DM RBCs subject to static tensile

248 ation could induce a premature biomechanical elastic response rather than a progressive pathologic pr

249 esults suggest that rod inextensibility, not elastic response, dictates the zeroth-order shape of an

250 umerical simulations of neurons as discrete, elastic rods provide evidence that a balance of torque,

251 ells comprise an initially planar network of elastic rods that are actuated into a shell-like structu

252 s radiogenic heating using neutrino-electron elastic scattering and low-background, direction-sensiti

253 udy of the local structure by applying total elastic scattering and Raman scattering analyses to an i

254 The coherent elastic scattering of neutrinos off nuclei has eluded de

255 towards rational design of multifunctional, elastic SEIs that overcome the most serious limitations

256 MES (Chemical Identification through Magneto-Elastic Sensing), that can detect a broad range of targe

257 Here, we describe highly elastic sensors and interconnects formed from thin, twis

258 A thin elastic sheet lying on a soft substrate develops wrinkle

259 acked plates and shells, we constrained flat elastic sheets to adopt fixed curvature profiles.

260 of the most sensitive and reliable nonlinear elastic signatures for micro-damage assessment.

261 ble more closely the situation of disordered elastic spheres having sharp interfaces, so the glass an

262 agen fibers and 24 of 26 stained with Miller elastic stain had decreased elastic fibers.

263 or trusses, when made from materials of high elastic stiffness and low density, represent some of the

264 e characterize spatiotemporal changes of the elastic stiffness of the injured rat neocortex and spina

265 in a hyperconnected network with exceptional elastic stiffness, higher than that of fully dense silic

266 e Hashin-Shtrikman upper bounds on isotropic elastic stiffness.

267 ly compare the experimental evolution of the elastic strain during tensile deformation at 973 K.

268 imensional numerical modeling shows that the elastic strain energy plays a key role in determining th

269 It was found that the coherent elastic strain field in the matrix, created by the latti

270 Elastic strain is being increasingly employed to enhance

271 as been used to investigate the evolution of elastic strain of constitutive phases and their interact

272 mined not only by contractility, but also by elastic stress in the peripheral actin bundles.

273 n indicate that the average stored curvature elastic stress of the membrane is reduced on elongation

274 The timescale of elastic stress relaxation has a lower bound of 4 min, wh

275 ismicity variations are the direct result of elastic stresses induced by the water load.

276 els, restriction of cell volume expansion by elastic stresses led to increased secretion of IL-1beta,

277 Scissoring in thick copper traces enables elastic stretchability as large as approximately 350%, c

278 ation by coupling continuous one-dimensional elastic structures.

279 from measured displacements of an underlying elastic substrate, the spatially dependent forces that c

280 es have been performed, however not for deep elastic substrates that support both shear and compressi

281 eover, we find that the characteristic visco-elastic time is inversely proportional to the compressio

282 rofluidic experiment, allowing us to explore elastic turbulence from the perspective of particles mov

283 olymers, resulting in a chaotic flow dubbed 'elastic turbulence'.

284 in the context of small scales chaotic flows.Elastic turbulence, a random-in-time flow, can drive eff

285 e, which is finally followed by the onset of elastic turbulence.

286 ogic elements, suggests the potential use of elastic vibrations (i.e., phonons) in information proces

287 ometric nonlinearities to switch and amplify elastic vibrations, via magnetic coupling, operating at

288 e derive an analytical function based on the elastic-viscoelastic correspondence principle applied to

289 The method based on the elastic-viscoelastic correspondence principle was valida

290 A numerical method of solving for the elastic wave eigenmodes in acoustic waveguides of arbitr

291 es (field and frequency) of the vector-field elastic wave equation with a given propagation constant.

292 resonator concept to obtain large asymmetric elastic wave transmission in multiple low frequency band

293 ot expected to be carried by the fastest (P) elastic waves but by the speed-of-light changes of the g

294 ectional/asymmetric transmission of acoustic/elastic waves has recently been realized by linear struc

295 ased technique for the detection of in-plane elastic waves propagating in structural lattices.

296 The resonant elastic X-ray response at the K-edge, which was argued t

297 that the line-shape of the measured resonant elastic X-ray response can be explained with the "site-s

298 that allows a reliable determination of the elastic (Young's) modulus of soft samples, including liv

299 Elastic (Young's) modulus prior to treatment was correla

300 odel including a strong magnetic anisotropy, elastic, Zeeman, Heisenberg exchange, and magnetoelastic