ライフサイエンスコーパス: elastic

1 al detailed balance that the lattice remains elastic and can be thermally excited between lattice con

2 stochemical evaluation and quantification of elastic and collagen content and morphology using multip

3 rables has created a demand for lightweight, elastic and conformal energy harvesting and storage devi

4 Although both elastic and elastoplastic models can reproduce the obser

5 wo-phase composite media that link effective elastic and electromagnetic wave characteristics to one

6 ethodologies that limit the ability to print elastic and highly vascularized tissues.

7 e wide scattering resonance features in both elastic and inelastic rate coefficients at collision ene

8 Elastic and inelastic scattering measurements reveal the

9 nd that memory effects arise from coexisting elastic and pinned components of the vortex assembly.

10 and jammed states exhibit memory, while the elastic and pinning dominated regimes do not.

11 nanocomposite a higher tensile strength, and elastic and storage moduli.

12 l stress depends on the relative strength of elastic and thermodynamic driving forces: if cholesterol

13 , and how their ability to anchor the highly elastic and tough IF cytoskeleton endowed vertebrates wi

14 ethods to map at high-spatial resolution the elastic and viscoelastic properties of soft materials.

15 mucin concentrations, osmotic pressure, and elastic and viscous moduli compared with healthy sputum.

16 The elastic and viscous properties of biological membranes p

17 ehensive characterization of the structural, elastic, and viscous properties of fluid membranes compo

18 , particle-induced X-ray emission (PIXE) and elastic backscattering spectrometry (EBS), can be used t

19 We then used nudged elastic band computational methods to derive conformatio

20 The pneuRIP system uses two elastic bands: one band (RC) placed around the rib cage

21 n tropoelastin as a highly biocompatible and elastic bioink for 3D printing of complex soft tissues i

22 ese results demonstrate the potential of the elastic bioink for printing 3D functional cardiac tissue

23 Recently, we have developed elastic biomimetic cryogels, an advanced type of polymer

24 odel tissue interaction with the surrounding elastic bodies that exert these forces, raising the ques

25 This kind of tissue-elastic body interactions are also at the core of many s

26 The spider web applies the concept of elastic cables taking only axial deformation into accoun

27 ared with WT, along with a more mechanically elastic cambial zone and radial compression of xylem cel

28 Owing to the lubricative properties of the elastic carbon covering, the macroporous structure coate

29 phases induces undulations in the underlying elastic cell membrane to form patterns on the cell surfa

30 roblem into that of nonlinear interaction of elastic charges.

31 temperature- and time-tuned crossovers from elastic (collective) dynamics to plastic flow.

32 With skin-like elastic compliance and toughness, the material provides

33 They accomplish this feat by means of elastic compliance of connective tissue, which passively

34 ons, these forces are exerted or resisted by elastic compliant structures such as the own-tissue cell

35 loud platforms, such as Google Cloud, Amazon Elastic Computing Cloud, Microsoft Azure and OpenStack.

36 calable pathogen pipeline platform, enabling elastic computing for high throughput Nanopore data on H

37 wo orders of magnitude smaller than the bend elastic constant (21 pN).

38 Cs) have revealed an anomalously small twist elastic constant compared to the splay and bend constant

39 general for thermotropic nematics, the twist elastic constant is found to be one order of magnitude s

40 While the splay elastic constant is in the typical range of 1.5 pN as is

41 These results demonstrate that a small twist elastic constant is not restricted to the special case o

42 The reason for this extremely small twist elastic constant very likely originates with the flexibi

43 astic constants and do not include the twist elastic constant.

44 extremely rare and report only the ratios of elastic constants and do not include the twist elastic c

45 , this study presents absolute values of the elastic constants and their corresponding viscosities fo

46 Recent measurements of the elastic constants in lyotropic chromonic liquid crystals

47 Interestingly, measurements of the elastic constants in the micellar lyotropic liquid cryst

48 the influence of silicate network on all the elastic constants of C-S-H is significantly higher than

49 lly, a highly consistent dataset on the nine elastic constants of more than 300 compositions of C-S-H

50 Appreciable magneto-elastic coupling of the SOP is detected by nc-AFM and ST

51 a computational model that accounts for both elastic deformation and forces of the ECM, an active cel

52 Experimental discovery of ultralarge elastic deformation in nanoscale diamond and machine lea

53 lity of the soft material, this flow-induced elastic deformation manifests as bulging near the cell o

54 ement is fortuitous and can be attributed to elastic deformation of capillary walls(23-25), which sup

55 hrough a combination of flank slip and visco-elastic deformation.

56 operties of the pollen wall and the relative elastic differences between the exine wall and the apert

57 ing puckering) were monitored by large-angle elastic diffraction.

58 the model using agent-based simulations with elastic dynamic microtubules and molecular motors.

59 nsion and a switch from a promigratory to an elastic ECM drive valve leaflet elongation.

60 ed surface, where the resulting long-ranged, elastic, effective interactions between defects can help

61 bricating a tissue-like, high-density, fully elastic electrode (elastrode) array capable of achieving

62 ic spring in the I-band, made by an undamped elastic element in-series with damped elastic elements,

63 the cooperative work of the contractile and elastic elements within a myofibril.

64 damped elastic element in-series with damped elastic elements, adapts its length to the SL with kinet

65 in the crystal structures of 1b and 1c where elastic energy accumulates during gas release, which cor

66 provides quantitative insights into how the elastic energy and the electrostatic energy determine th

67 adaptations: the trap walls' fast release of elastic energy ensures strong and constant suction press

68 Interestingly, the single nanoparticle elastic energy landscape, which we map with attojoule pr

69 Minimizing the total elastic energy leads to a preferred spontaneous curvatur

70 opant in the perovskite lattice and (ii) the elastic energy of the dopant due to cation size mismatch

71 rmations and that this process may lower the elastic energy of the system.

72 e behavior of the plantar flexor muscles and elastic energy storage in the Achilles tendon.

73 Elastic energy stored in bent filaments, whose presence

74 shell needs to be balanced by the increasing elastic energy through ligand passivation(8-10).

75 u functional-a coarse-grained version of the elastic energy, which penalizes nonuniform wrinkle spaci

76 xtent to which an un-motorized, low-profile, elastic exosuit reduced the rate of fatigue for six lumb

77 ely demonstrate the ability of a low-profile elastic exosuit to reduce back muscle fatigue during lea

78 rent steel thicknesses by detecting both the elastic, fast-neutron backscatter and the Compton-scatte

79 c vitamin K depletion leading to accelerated elastic fiber damage and thrombosis in severe COVID-19 d

80 hich protects against pulmonary and vascular elastic fiber damage.

81 smosine was measured to quantify the rate of elastic fiber degradation.

82 irmed that variations in genes that increase elastic fiber deposition also had positive impact on aor

83 D3 + T cells, macrophages, and neutrophils), elastic fiber disruption, and an increase in smooth musc

84 Our results demonstrate a rescue of aortic elastic fiber fragmentation and disorganization accompan

85 , as in Marfan syndrome, can compromise both elastic fiber integrity and mechanosensing.

86 n; these factors include localized losses of elastic fiber integrity, aberrant collagen remodeling, r

87 comparable to those in cases of compromised elastic fiber integrity.

88 oss of FBLN5, rescued injury-induced loss of elastic fibers and biomechanical properties after partur

89 a plaques and dendrites in brain tissues and elastic fibers in developing cartilage of mice.

90 on, and obstetrical injury on FBLN5 content, elastic fibers, biomechanics, and histomorphology of the

91 dial thickening, disorganized and fragmented elastic fibers, reduced smooth muscle calponin expressio

92 ng hyaluronic acid, collagen fibers, but few elastic fibers.

93 es the elastin precursor so it is primed for elastic fibre assembly.

94 The literature on the contribution of elastic fibre deposition to alcohol-related liver diseas

95 We also investigated the composition of the elastic fibres (oxytalan, elaunin and mature elastic fib

96 The main components of elastic fibres are elastin and fibrillin, where correct

97 psies and broken dense perisinusoidal mature elastic fibres in explanted livers.

98 in and fibrillin, where correct formation of elastic fibres requires a fibrillin microfibril scaffold

99 ss with a transition from oxytalan to mature elastic fibres usually present in explanted livers.

100 Elastic fibres were assessed in terms of their distribut

101 elastic fibres (oxytalan, elaunin and mature elastic fibres) in 20 cases.

102 and reabsorption of pericellular and septal elastic fibres, and a potential role for stratification

103 more advanced stages contained mainly mature elastic fibres.

104 phase with proteolytic activity and reduced elastic fibres.

105 d MMP9 was linked to a 50% reduction of lung elastic fibres.

106 Elastic folding, a phenomenon widely existing in nature,

107 ween particles in addition to frictional and elastic forces.

108 The line crack models, including linear elastic fracture mechanics (LEFM), cohesive crack model

109 Finally, we used linear elastic fracture mechanics theory to predict where surfa

110 ability diagram of fractures based on linear elastic fracture mechanics to predict where basal and dr

111 perties resist external forces and create an elastic gel and provides a scaffold that supports liquid

112 r, we treat it as a thin elastic layer on an elastic half-space.

113 e device and with geolocators attached using elastic harnesses.

114 mable brain tissue is modeled by means of an elastic Hooke's law.

115 romote behaviours that are not observed with elastic hydrogels in both two- and three-dimensional cul

116 ), a technology that transforms tissues into elastic hydrogels to enhance macromolecular accessibilit

117 This injectable formulation provides elastic hydrogels with higher mechanical rigidity, bette

118 eady "droplets" with hydrophilic surface and elastic hydrophobic membrane, we developed an oil-free p

119 t correlation between tagging and non-rigid, elastic image registration (r = 0.84), while correlation

120 The non-rigid, elastic image registration algorithm produces more preci

121 ftware with different algorithms (non-rigid, elastic image registration, and blood myocardial border

122 imilarly, ECM lining blood vessels is highly elastic in order to sustain the basal and pulsatile forc

123 Thin solids often develop elastic instabilities and subsequently complex, multisca

124 be improved towards normal by application of elastic kinesiology tape across the knee joints, which w

125 interplay between topology and mechanics in elastic knots remains poorly understood.

126 hat are separated by concentrically arranged elastic lamellae; a form of extracellular matrix (ECM).

127 , respectively, by the internal and external elastic laminae.

128 The resulting elastic lattice deformation that follows scanning irradi

129 ystal can generate phase-dependent transient elastic lattice deformation.

130 ix to create a composite in which ultralarge elastic lattice strains up to 6.7% are achieved in Nb na

131 ush, and in the other, we treat it as a thin elastic layer on an elastic half-space.

132 The combined effect of soft elastic layered structure, abundance of low energy optic

133 d drag force and non-Newtonian fluid induced elastic lift force, arising from symmetric acoustic micr

134 the length of the bands within the apparent elastic limit of the phase mixture.

135 cts, for systems without inertial load, that elastic load enhances positive shift of voltage dependen

136 of turgor pressure increases with increasing elastic load.

137 We report a super-soft and super-elastic magnetic DNA hydrogel-based soft robot (DNA robo

138 However, tissues and ECMs are not linearly elastic materials-they exhibit far more complex mechanic

139 gh centimeter-thick layers of bio-mimicking, elastic materials.

140 We derive a scaling law for linear elastic matrices such as basement membrane extract hydro

141 nical stress as single cells grow within the elastic matrix.

142 properties with tailored surface chemistry, elastic mechanical properties and chemical stability in

143 ntermediate forms, suggesting that incipient elastic mechanisms do not persist in evolutionary time.

144 etermine a material constant lambda(0) of an elastic medium is approximately [Formula: see text] for

145 the lipid bilayer that is strengthened by an elastic meshwork representing the cytoskeleton.

146 he study of ordered and disordered 2D porous elastic metamaterials are discussed.

147 The focus of this paper is on elastic metamaterials characterised by the presence of w

148 , we present a design strategy for aperiodic elastic metamaterials in order to achieve the same perfo

149 human-soft actuators interaction, including elastic metamaterials with human gesture-controlled band

150 as a fundamental mechanism to design passive elastic metasurfaces capable of an exceptionally broadba

151 While elastic metasurfaces offer a remarkable and very effecti

152 We design elastic metasurfaces, consisting of a graded array of ro

153 ing a radial dyke swarm, and propose a visco-elastic model for their accommodation.

154 The poro-elastic model of extensional quartz vein formation indic

155 An adjustable thermo-elastic model with the ability to control stability cond

156 ated cell motility coupled to the collective elastic modes of the cell sheet is sufficient to produce

157 We compare the measured elastic moduli along the stem length and between adaxial

158 Elastic moduli and failure strains of fibrin and PEG (60

159 Very different elastic moduli are found.

160 rix and alginate, which presented a range of elastic moduli from 0.4 to 9.3 kPa.

161 ter-size, heterogeneous domains at different elastic moduli in tissue sections by AFM has remained el

162 odulus is shown to be in good agreement with elastic moduli measurements performed on the gallium-sta

163 ermine the spatial distributions of apparent elastic moduli of living spinal cord tissue sections obt

164 ations; and nondestructive evaluation of the elastic moduli of materials from the effective dielectri

165 nificant increase of the respective apparent elastic moduli that transiently obliterated the mechanic

166 g heterogeneous cell-layer contractility and elastic moduli values based on experimentally measured b

167 it the same vibrational spectrum and related elastic moduli.

168 SilDNs simultaneously possess low elastic modulus (E(100%) < 700kPa) as well as large ulti

169 A sharp increase in elastic modulus after the incorporation of PCL in the co

170 ell culture conditions, including substratum elastic modulus and extracellular matrix composition.

171 e film expands nearly 30% in volume, and the elastic modulus and hardness decrease by a factor of two

172 erties of the CAGE gel were dominated by the elastic modulus and suggested a solid-like viscoelastic

173 ation time by one order of magnitude and the elastic modulus by a factor of two compared with the fib

174 n-softening response, where its steady state elastic modulus decreases with increasing strain.

175 If the substrate is compliant, with an elastic modulus G < 100 kPa, the droplet will markedly s

176 tributions, with glucomannans increasing the elastic modulus in compression, and xylans contributing

177 The mean elastic modulus of DM adipose tissue was twice that of N

178 s have been developed which aim to match the elastic modulus of the brain for improved interfacing.

179 The hardness and elastic modulus of the four films were insensitive to st

180 this method to retrieve the local, interior elastic modulus of these hydrogels and both the radial a

181 actin cytoskeleton and the substrate-to-cell elastic modulus ratio.

182 Similarly, elastic modulus values increased by an average of 17% in

183 mple stained for collagen allows correlating elastic modulus with collagen amount and position with h

184 ulting in significant softening (85% reduced elastic modulus) of the 3D-printed constructs.

185 We found that the size, thickness, elastic modulus, and ultimate stress in both the radial

186 se glasses exhibit higher density, hardness, elastic modulus, and yield stress.

187 elation point was shown, as well as a higher elastic modulus, compared to control suspensions.

188 thesis that fibrosis, evidenced by increased elastic modulus, is enhanced in DM adipose tissue, and s

189 ct of polymer structure and concentration on elastic modulus, tensile strength, and ultimate strain.

190 present in human and mouse tissues, by their elastic modulus.

191 Elastic monopoles are formed by relatively large asymmet

192 colloidal system, ranging from de-mixing of elastic monopoles to a zoo of unusual colloidal crystals

193 mally gated (OG) and fully motion-corrected (elastic motion correction [EMOCO]) reconstructions.

194 fully automated fashion, employing rigid and elastic MSI image registration using structured and plaq

195 f mesostructures of gold capable of inducing elastic multipoles of different order.

196 als can be described as interactions between elastic multipoles that depend on particle shape, topolo

197 epistasis analysis using Empirical Bayesian Elastic Net (EBEN) models.

198 classifiers including random forests (RFs), elastic net (ELNET), support vector machines (SVMs) and

199 The Elastic Net (EN) model was built to predict SA extent, d

200 eferred to as self-optimizing support vector elastic net (SOSVEN).

201 abases to enhance functional annotation, and elastic net and a gene expression composite score to aid

202 e variance compared with area p24 using both elastic net and partial least-squares regression.

203 robust logistic regression (Rlogreg), robust elastic net based on the least trimmed square (enetLTS),

204 The elastic net model showed better performance compared to

205 rformance of the new cnCV with standard nCV, Elastic Net optimized by cross-validation, differential

206 We find that elastic net penalized logistic regression performs parti

207 mble learning that combined predictions from elastic net penalized logistic regression, random forest

208 Elastic net penalized regression was used to select 94 C

209 line-derived transcriptomic datasets through elastic net regression analysis to identify a gene signa

210 espectively; corresponding figures using the elastic net regression approach were 91% and 76% (Raine)

211 ing a regularised regression technique (i.e. elastic net regression based on the local-level similari

212 Elastic net regression was used to identify the most imp

213 e on DNA methylation at specific sites using elastic net regression, a supervised machine learning me

214 r machine learning models: Lasso regression, elastic net regression, random forest, and gradient boos

215 inal score was developed with 204 CpGs using elastic net regression.

216 ance by regularised logistic regression with elastic net regularisation, with an area under the curve

217 this report, a parameter-free support vector elastic net that self-optimizes two key regularization c

218 A feature analysis framework utilizing Elastic Net was implemented to reduce the features gener

219 used ML algorithms-logistic regression (LR), elastic net, random forest, artificial neural network (A

220 Using elastic net, we make novel predictions of pro- and anti-

221 We used an elastic-net regression for variable selection, and a ran

222 Elastic-Net regression was used to build Base (sociodemo

223 Elastic-net regression was used to develop a DNA-methyla

224 dels were fit to MCCV training samples using Elastic-Net.

225 Statistical learning methods (elastic nets/principal components analysis) and Cox regr

226 ty profiles inferred from Hi-C data using an elastic network model representation of the chromatin.

227 Elastic network modelling suggests that the effect of CO

228 Elastic network modelling suggests that the lowest entro

229 r modeling for the last few decades, such as elastic network models (ENMs) that are widely used for n

230 Elastic network models were constructed to compare the d

231 tune its mechanics from highly cross-linked, elastic networks to weakly cross-linked viscous networks

232 The anode is composed of an elastic outermost carbon covering, a nonfilling porous s

233 From elastic P- and S-wave velocity and electrical resistivit

234 e pollen, we delineate the regions of pollen elastic parameters where desiccation leads to a regular,

235 rtures leads to a reduction of the region of elastic parameters where the apertures close in a regula

236 significant reductions in tensile stress and elastic-plastic deformation during dicing, thanks to a l

237 Linearly elastic polyacrylamide hydrogels and polydimethylsiloxan

238 improve tissue regeneration, we developed an elastic polymeric material poly(xylitol dodecanedioic ac

239 hable, and solderable fibers that consist of elastic polyurethane (PU) fibers and conductive Cu fiber

240 formalism that maps the two-dimensional (2D) elastic problem into that of nonlinear interaction of el

241 , but the function of cross-linking on their elastic properties is yet to be elucidated.

242 rmore, the electronic, optical, thermal, and elastic properties of borophene are thoroughly discussed

243 Here, we report ab initio results for the elastic properties of calcium ferrite-type phases and de

244 Here, we studied the elastic properties of chromatin by dynamic measurements

245 ging from directly measuring the dynamic and elastic properties of chromatin to studying the interact

246 ntially due to the lower nonlinearity in the elastic properties of ex vivo tissue.

247 Changes in the elastic properties of living tissues during normal devel

248 of elasticity, we show how both the absolute elastic properties of the pollen wall and the relative e

249 e bonding of titin fragments could alter the elastic properties of titin; however, whether and where

250 in the water droplets allow the fundamental elastic properties of two-dimensional matter to be probe

251 sticity can be exploited to train in desired elastic properties, both in the global moduli and in loc

252 Numerically determined porosities, effective elastic properties, thermal conductivities and permeabil

253 design nanostructured materials to maximize elastic properties.

254 Loss of elastic recoil and interdependence during acute bronchoc

255 NMR quantification, Raman spectroscopy, and elastic recoil detection analysis, challenging the origi

256 HFEV(1) asthmatics had significantly reduced elastic recoil pressure (pressure-volume curve shifted u

257 With loss of elastic recoil pressure, the HFEV(1) group could generat

258 , both being emergent properties of the same elastic-recoil mechanism.

259 ffort to realize flat lenses in acoustic and elastic regimes.

260 Elastic registration between baseline and follow-up CT i

261 f ILD based on lung shrinkage detection from elastic registration of chest CT scans in patients with

262 Conclusion Elastic registration of CT scans combined with a deep le

263 hlighted the importance of apertures for the elastic response and the folding of the grain.

264 ould also prove useful for the design of the elastic response of artificial inhomogeneous shells.

265 merical models that treat the DNA helices as elastic rods are used to evaluate the local loss of stif

266 f governing electrophoretic and slip-induced/elastic/shear gradient lift forces.

267 by embedding arrays of periodic cuts into an elastic sheet.

268 panied by features typically associated with elastic sheets, including the development of radial wrin

269 ential ingredients needed to describe tissue-elastic solid interactions: an effective inertia and vis

270 In this work, we present a vastly different elastic solid model (ESM) of macromolecules that shares

271 from ENM in that it treats macromolecules as elastic solids.

272 Both signals are generated using an elastic spring system (ESS), which includes a protractor

273 on, an intragranular misorientation and high elastic strain gradients near a twin boundary.

274 r properties-such as higher yield stress and elastic strain limit(3)-are greatly improved relative to

275 to have the ability to withstand ultralarge elastic strains (4-10%) and to have ultrahigh strengths

276 rain matching between the uniform ultralarge elastic strains (4-10%) of nanomaterials and the uniform

277 ation in ferromagnetic (FM) layer induces an elastic stress in the piezoelectric (PE) layer, which ge

278 e energetic cost of the growing edge and the elastic stresses generated due to the curvature of the c

279 ing to itself and other surfaces, as a soft, elastic substrate and encapsulation coating for wireless

280 sive contact of a rigid flat surface with an elastic substrate having Weierstrass surface profile is

281 raded array of rod resonators attached to an elastic substrate that, together with critical insight f

282 A growing body of data from other elastic systems suggests that similar coevolution of tra

283 ed, we find muscle-powered and fully fledged elastic systems with enormous performance differences, b

284 ced ejection fraction were more fibrotic and elastic than myocardium from patients with HF with prese

285 s were at least two orders of magnitude more elastic than the classical plasma membrane suggesting a

286 The elastic thermoelectric material is implemented in the fi

287 s a highly prevalent disorder also involving elastic tissue dysfunction and is associated with glauco

288 To perform this function, elastic titin must change stiffness or extensible length

289 Interactions of elastic titin with sarcomeric actin filaments are reveal

290 We find a lower bound on the ratio of elastic to inelastic molecule-atom collisions that is gr

291 second magnetization peak coincides with the elastic-to-plastic crossover at low T, yet the mechanism

292 mesoflower particles, for which gravity and elastic torque balancing yields monopole-type interactio

293 ium-rubidium (KRb) polar molecules, in which elastic, tunable dipolar interactions dominate over all

294 essential for the stability and strength of elastic vessels and tissues.

295 severe drought when they have used up their elastic water storage.

296 Elastic waves guided along surfaces dominate application

297 We study the propagation of in-plane elastic waves in a soft thin strip, a specific geometric

298 A substantial challenge in guiding elastic waves is the presence of reflection and scatteri

299 sheds a new light on unsurpassed control of elastic waves, ranging from vibration protections to ult

300 oherence elastography (OCE) based on surface elastic waves.