ライフサイエンスコーパス: Young's modulus

1 on properties (such as contractile force and Young's modulus).

2 times cylindrical radius" independent of the Young's modulus.

3 nality between network conductance and fibre Young's modulus.

4 tical absorption, electrical conductance and Young's modulus.

5 rface properties but a 10-fold difference in Young's modulus.

6 mains constant, independent of the substrate Young's modulus.

7 ments based on Hertz theory overestimate the Young's modulus.

8 e as revealed by a significant difference in Young's modulus.

9 f flexural rigidity directly proportional to Young's modulus.

10 stiffness parameter measured in terms of its Young's modulus.

11 lt to compare to AFM-derived measurements of Young's modulus.

12 re, and retains similar hardness and reduced Young's modulus.

13 or to measure mechanical properties like the Young's modulus.

14 +) sensitivity, passive axial compliance and Young's modulus.

15 ish the translation of wave speed into shear/Young's modulus.

16 pendent relationship between the density and Young's modulus.

17 ne demonstrated reduced tensile strength and Young's Modulus.

18 ssue-like mechanical properties, such as low Young's modulus (0.1 to 0.3 MPa), high strength (1.1 +/-

19 (110 MJ m(-3)), yield strength (73 MPa) and Young's modulus (1 GPa).

20 The Young's modulus (1.47 MPa) and hydrophobicity (with a se

21 A flexible scaffold was observed (Young's modulus = 1.74 +/- 0.90 MPa) with 1% of water ab

22 doluminescence and high mechanical strength (Young's modulus: 1.16 +/- 0.1 TPa), reminiscent of forma

23 e (1,000 J/m(2)), high strength (1 MPa), low Young's modulus (100 kPa), and high water content (70 to

24 NDC with 2 phr glycerin provided the optimum Young's modulus (15.67 MPa) and tensile strength (1.67 M

25 er), high stretchability (> 35% strain), low Young's modulus (~2 MPa), superior mechanical, electrica

26 The high Young's modulus, 20.3 MPa, and excellent photothermal pe

27 e BNNT/PDMS composites demonstrate augmented Young's modulus (200% increase at 9 wt% BNNT) and therma

28 hydrogel skins exhibit tissue-like softness (Young's modulus ~ 30 kPa), have uniform and tunable thic

29 %) alloy with ultralow Young's modulus (36 GPa, versus ~30 GPa for human bone)

30 for implant applications exhibit much higher Young's modulus (50 ~ 120 GPa) than human bone (~30 GPa)

31 d record high tensile strength (826 MPa) and Young's modulus (65.7 GPa) owing to the large length and

32 of up to 43%, and extreme variations of the Young's modulus (a measure of the fibril's mechanical st

33 rotein toughness and a 70-fold difference in Young's modulus across a web documents the phenotypic pl

34 Differentiating the states based on the Young's modulus allowed for the mapping of the different

35 ests yields maximum values of 62 GPa for the Young's modulus and 0.70 GPa for the fracture strength,

36 ests yield maximum values of 290 GPa for the Young's modulus and 5.8 GPa for the fracture strength.

37 ic stiffness was evaluated as the product of Young's modulus and aortic wall thickness.

38 ole localization task to extract the whisker Young's modulus and damping coefficient.

39 Compared to PVA/CNTs, the tensile strength, Young's modulus and electrical conductivity of the PVA/G

40 The coating also increases Young's modulus and energy storage modulus by a factor o

41 rmeability increased while tensile strength, Young's modulus and glass transition temperature decreas

42 Young's modulus and hardness increase correspondingly.

43 on tissue mechanical properties, we compared Young's modulus and hardness of dentin in the 3 Col1a2 g

44 rior mechanical properties, including higher Young's modulus and hardness.

45 Force was computed from Young's modulus and longitudinal aortic strain; work was

46 ction, as reflected in greater values of the Young's modulus and mechanical strength.

47 ose structure is optimized, in which the low Young's modulus and particle sliding synergistically all

48 The Young's modulus and Poisson's ratio of the cells were ob

49 at demonstrate ligand crosslinking increases Young's modulus and sound velocity.

50 00 GPa, offering one of the highest specific Young's modulus and specific yield strengths among struc

51 presence of the nanosilicates increases the Young's modulus and stalls the degradation rate of the r

52 e properties of individual fibers, including Young's modulus and stiffness.

53 ation, roughness, ultimate tensile strength, Young's modulus and strain at break.

54 ctive for nanomechanical systems because its Young's modulus and strength are both intrinsically high

55 unique combination of high tensile strength, Young's modulus and structural flexibility which arise d

56 deling indicates that the exceptionally high Young's modulus and surface conformity of 2D capping lay

57 that the force profiles collected to measure Young's modulus and surface tension can also provide bot

58 rate deposited individual sucrose particles, Young's modulus and surface tension can be quantified as

59 tion factor, psi, the ratio of the corrected Young's modulus and the Hertz modulus in the parameter r

60 a progressive increase in the glycoprotein's Young's modulus and toughness.

61 adsorption: mass, surface stress, effective Young's modulus and viscoelasticity.

62 Young's modulus and volume changes as a function of appl

63 ontrarily, in the post-yield region a higher Young's modulus (and more clearly, a higher mineral cont

64 ical elastic properties (Poisson's ratio and Young's modulus), and it can easily be extended to incor

65 istensibility, 0.99 (95% CI: 0.90, 1.09) for Young's modulus, and 0.90 (95% CI: 0.74, 1.10) for aorti

66 rease in energy to fracture, 22% increase in Young's modulus, and approximate 33% improvement in stif

67 NCC blending increased the Young's modulus, and elastic character, of the protein a

68 nt in the network, it was possible to obtain Young's modulus, and hence the stiffness, of the DNA fil

69 racterized by their low formation energy and Young's modulus, and high thermal expansion coefficients

70 ies of a solid (bulk modulus, shear modulus, Young's modulus, and Poisson's ratio) as input variables

71 ng a high entanglement molecular weight, low Young's modulus, and rapid kinetics for self-assembly.

72 , shear, bending, and compressive strengths, Young's modulus, and SEM analysis, as well as fluidity o

73 small ratio between the fracture energy and Young's modulus, and the patterns agree well with experi

74 ng dynamics to flipping behavior occurs at a Young's modulus approximately three times larger than th

75 ional forms of the temperature derivative of Young's modulus are derived and compared with experiment

76 the MT, but the elastic moduli, notably the Young's modulus, are not directly revealed in experiment

77 duces membrane stability, bilayer thickness, Young's modulus, area stretch modulus, and bending stiff

78 e whisker as a conical cantilever beam, with Young's modulus as the only free parameter.

79 A correlation between Young's modulus, as determined by using nanoindentation

80 ation between corneal acoustic impedance and Young's modulus at low strain levels.

81 The tendon stiffness and Young's modulus at maximum isometric load were 161 N mm-

82 The tensile strength and Young's modulus at MPa levels are comparable or even hig

83 rack capsid swelling and measure the shells' Young's modulus at the same time.

84 correlations between acoustic impedance and Young's modulus (at 1%-5% strains) were found in the mea

85 y viable class of synthetic materials with a Young's modulus below 100 kPa conforming to biological a

86 l results in a substantial difference of the Young's modulus between these two types of cells.

87 ce is not due to deficiencies of hardness or Young's modulus, but may be due to defects in post-yield

88 Genotype had a significant effect on Young's modulus, but there was not a simple mutant allel

89 9.3 +/- 11.5% (P < 0.005), respectively, and Young's modulus by 9.2 +/- 8.2% (P < 0.05) and 30.1 +/-

90 art the greatest improvements, enhancing the Young's modulus by a factor of 2.5 at 20 wt.%.

91 dependent control of melting temperature and Young's modulus by concurrently altering side chain leng

92 linking of curli nanofibers, we increase the Young's modulus by two times.

93 mponent system with an unprecedented drop of Young's modulus by up to six orders of magnitude from th

94 tion angle (), patellar tendon stiffness and Young's modulus (by ultrasonography) were measured befor

95 Because the gamma phase has a large Young's modulus (ca. 26 GPa), a force of 0.1 muN can be

96 Furthermore, by applying an external strain, Young's modulus can be measured in the range from 1 Pa t

97 perties including adhesion, deformation, and Young's modulus can be simultaneously mapped along with

98 er a range of 30 days to 6 months, while the Young's modulus can be varied over 3 orders of magnitude

99 y suffer from mechanical mismatch, including Young's modulus, cell adhesion, and geometric cues.

100 Indeed, it has a Young's modulus comparable to steel, on the order of 300

101 he active state of the receptor has a higher Young's modulus compared to the inactive state of the re

102 AFM images indicated a higher and increasing Young's modulus correlated with cross-linking, as well a

103 l properties of hMSCs, including the average Young's modulus determined by atomic force microscopy (3

104 Culture on softer plates (25 or 2 kPa Young's modulus) did not alter proliferation or reduce e

105 bril and fiber levels varies in rigidity and Young's modulus due to different physiological changes,

106 tures and is used to estimate the nematode's Young's modulus E and tissue viscosity eta.

107 ves for individual MWCNTs indicated that the Young's modulus E of the outermost layer varied from 270

108 Young's modulus E scales with density as E ~ rho(2), in

109 soft poly(ethylene glycol) (PEG) hydrogels (Young's modulus E ~ 2 kPa) depended on previous culture

110 ure DNA scaffolds, a tenfold increase in the Young's modulus (E modulus) of these composites was obse

111 The apparent transverse Young's modulus (E( perpendicular)) was 94 +/- 41 kPa in

112 ibrium friction coefficient (micro(eq)), and Young's modulus (E(Y)) were determined from the temporal

113 icroscopy (AFM) nanoindentation to determine Young's modulus (E) along multiple elements representing

114 rements, allowed us to propose a theoretical Young's modulus (E) between 10(6) and 10(7) dyn/cm(2) fo

115 The obtained Young's modulus (E) of 19.3 MPa and 28.1 MPa allowed us

116 xially to determine the circumferential bulk Young's modulus (E).

117 We show that softer (Young's Modulus [E] < 100 kPa) substrates stimulate an a

118 stiffness typical of normal muscle (passive Young's modulus, E approximately 12 kPa).

119 don's model, which is widely used to measure Young's modulus, E.

120 ly 600 degrees C) and mechanical properties (Young's modulus exceeding 2 GPa).

121 Here, we calculate the Young's modulus for bulk diphenylalanine peptide from fi

122 ed molecular combing techniques to determine Young's modulus for individual microfibrils and X-ray di

123 This method allowed us to determine the Young's modulus for the capsule in various conditions th

124 The calculated Young's modulus for the CPO map shows a weak mechanical

125 All behaved as Hookean springs with Young's modulus from 300 to 1500 kPa for gels with polym

126 rough surface, can be used to determine the Young's modulus from a Derjaguin-Muller-Toporov (DMT) fi

127 In contrast, on stiff substrates (Young's modulus >20 kPa), traction stress plateaus at a

128 rties of the fiber such as tensile strength, young's modulus have also been investigated.

129 uators, enabling rapid measurement (<1 s) of Young's modulus, high spatial sensing density (~1 cm(2))

130 No difference in the Young's modulus (i.e. an indicator of wall stiffness) of

131 ree independent ways: (i) an increase of the Young's modulus, (ii) a strong rise of the capsid's ulti

132 sation algorithm for the characterisation of Young's modulus, (iii) a quantification of the effects o

133 /- 29 kPa) was approximately a tenth that of Young's modulus in the longitudinal direction, a differe

134 escribed with the elastic modulus (effective Young's modulus) in a self-consistent way.

135 which leads to density increase of ~25% and Young's modulus increase of ~71% relative to that of pri

136 - 713 to 3609 +/- 1220 N mm-1; P < 0.05) and Young's modulus increased by 69 % (1.3 +/- 0.3 to 2.2 +/

137 With the increase of NaCl in gels, Young's modulus increased, swelling was reduced and dige

138 etected a positive trend versus time for the Young's modulus, indicating that aged silks are stiffer

139 trate that mESCs lacking Cltc display higher Young's modulus, indicative of greater cellular stiffnes

140 Near this transition, we observed that the Young's modulus intrinsically softens by over 30% coinci

141 Young's modulus is 0.10 GPa, less than for structural pr

142 physiological zonular tissue extensions and Young's modulus is between 78 MPa and 96 MPa, which is t

143 are based on Hertz contact mechanics, where Young's modulus is derived from the indentation force an

144 Since an increase in mineral or Young's modulus is more potent, that is deleterious, in

145 A maximum increase of 11.8% of Young's modulus is obtained.

146 A monolayer 2D capping layer with high Young's modulus is shown to be able to effectively suppr

147 rties of nanofibers aligned in arrays, whose Young's modulus is significantly enhanced upon dethreadi

148 rgodic regime, the temperature dependence of Young's modulus is solely determined by the magnetic pro

149 The magnitude of Young's modulus is strongly correlated with the relative

150 scale calculation shows that the increase in Young's modulus isn't dependent on the crosslinking betw

151 ompliance similar to soft biological tissue (Young's modulus < 100 kPa), and the capability to underg

152 On soft ACA gels (Young's modulus <20 kPa), cell-exerted substrate deforma

153 stretchability (>600%), elasticity, and low Young's modulus (<7 MPa).

154 For uniform, multidomain gels, Young's modulus mainly depended on the terminal concentr

155 ment of the nanoMIP stiffness, with the mean Young's modulus measured by AFM passing from 17 +/- 6 kP

156 etween the Brillouin elastic modulus and the Young's modulus measured by conventional mechanical tech

157 of composite materials which not only has a Young's modulus much larger than the Voigt limit, but al

158 ss, we show that gelatin-mTG substrates with Young's modulus near that of healthy glomeruli elicit a

159 ere comparable to native cartilage, with the Young's modulus of >800 kPa and equilibrium friction coe

160 and have a rigidity similar to that of silk (Young's modulus of 0.2-14 GPa).

161 duced anisotropic mechanical behavior with a Young's modulus of 0.33 +/- 0.1 MPa, very similar to tha

162 to match Bashtanov's experiment: stereocilia Young's modulus of 0.74 GPa, tip link assembly (gating s

163 Individual nanoribbons have a Young's modulus of 1.7 GPa and tensile strength of 1.9 G

164 RG growth cones growing on substrates with a Young's modulus of 1000 Pa strengthen considerably after

165 micrometer-thick porous carbon films with a Young's modulus of 14.5 gigapascals, with the possibilit

166 verage stiffness of 69.6 +/- 6.8 N m(-1) and Young's modulus of 17.8 +/- 2.5 GPa, higher than any pre

167 indentation of the surface showed an average Young's modulus of 189 kPa, falling in a range that is c

168 ysiological levels of mechanical resistance (Young's modulus of 4 kPa).

169 ith a high tensile strength of 342 MPa and a Young's modulus of 43.6 GPa, respectively.

170 aves as an isotropic elastic material with a Young's modulus of 50 +/- 10 MPa inflated by a turgor pr

171 imulations yield low-velocity values for the Young's modulus of 6.0 GPa.

172 cells tested and among the lowest reported (Young's modulus of 85 +/- 5 Pa).

173 A Young's modulus of 9.8 MPa was achieved and the maximum

174 he single coiled coil of HMM has an apparent Young's modulus of about 0.5 GPa.

175 ple helices into fibrils perhaps reduces the Young's modulus of an individual triple helix, which res

176 splay maximal outgrowth on substrates with a Young's modulus of approximately 1000 Pa, whereas hippoc

177 in the stiffer gels rapidly develop a higher Young's modulus of approximately 20 kPa, sixfold greater

178 of up to 1000 MPa, plasticity over 10%, and Young's modulus of approximately 200 GPa, offering one o

179 axation modulus is <5 kPa exhibit a cellular Young's modulus of approximately 5 kPa.

180 istical difference between the values of the Young's modulus of both poorly attached (round) and firm

181 l that can be applied to extract the correct Young's modulus of cells loosely attached to a substrate

182 These quantities correspond to a Young's modulus of E = 1.0 terapascals, third-order elas

183 The Young's modulus of elasticity (E) at each temperature fo

184 Stress-strain relations and Young's modulus of elasticity, a measure of tissue stiff

185 the Fermi energy landscape and increases the Young's modulus of elasticity.

186 We find that the perpendicular Young's modulus of graphene oxide films reaches a maximu

187 pabilities of this procedure to evaluate the Young's modulus of highly stiff materials with greater a

188 ining in old age increases the stiffness and Young's modulus of human tendons.

189 The Young's modulus of immature and mature capsids, as deter

190 was used to quantify the CTFs by associating Young's modulus of LC to the cell induced stresses and b

191 Finally, we use EOF to map the Young's modulus of living cells, which gives similar res

192 Here, we examine the Young's modulus of nanocomposites based on a common bloc

193 at uses strain fluctuations to determine the Young's modulus of nucleosomes from all-atom molecular d

194 hanically tested by compression to determine Young's modulus of pigmented, nonpigmented, and OA carti

195 The experiments show that the average Young's modulus of polyethylene nanofibers with diameter

196 olecular dynamics simulations to predict the Young's modulus of silicate glasses.

197 sensing sheet, for dynamically measuring the Young's modulus of skin and of other soft tissues at dep

198 a guide in understanding the changes in the Young's modulus of such composites as a function of fill

199 port the first measurement of the changes in Young's modulus of T-cells during their activation, show

200 Accordingly, Young's modulus of t/t thick filaments was approximately

201 mechanics testing further confirmed that the Young's modulus of the adhesive increased by nearly 4 fo

202 accurately simulates the median value of the Young's modulus of the axon plasma membrane determined b

203 RB powder was also found to increase the Young's modulus of the bio-elastomers without compromisi

204 weight ratio boosts the tensile strength and Young's modulus of the buckypaper/Parmax composite to 11

205 conformational sampling simulations that the Young's modulus of the buried core of the fibril is of t

206 The results indicate that the Young's modulus of the capsule decreases with its size a

207 ing force deflection method, we quantify the Young's modulus of the cell and estimate the swimming an

208 model to extract the effective longitudinal Young's modulus of the cell envelope of Escherichia coli

209 nd velocity is a measure of the stiffness or Young's modulus of the cell.

210 The average tensile strength and Young's modulus of the CNTs investigated in this study a

211 The Young's modulus of the composite Parylene C/PDMS was eva

212 Young's modulus of the cornea increased with age, with t

213 ng demonstrated significant increases in the Young's Modulus of the decellularized ECM scaffold; prov

214 G increased the elongation and decreased the young's modulus of the films.

215 ies of carbon nanotubes (CNT), reporting the Young's modulus of the individual CNT up to 1 TPa.

216 Young's modulus of the LC was profiled by using spherica

217 astic deformations is mainly affected by the Young's modulus of the material, due to a change in its

218 e relaxed and contracted muscle cell and the Young's modulus of the matrix without further knowledge

219 mbrane, which resulted in an increase in the Young's modulus of the membrane from 0.9+/-0.4 to 1.85+/

220 crochannel, by changing the geometry and the Young's modulus of the microchannel, enhances the sensit

221 th nanofiber and silicon substrate yield the Young's modulus of the nanofiber.

222 meter gold nanocrystal monolayers, we find a Young's modulus of the order of several GPa.

223 ness is primarily dependent on the effective Young's modulus of the polymerized material and the effe

224 The Young's modulus of the printed stick is found to compare

225 was verified by explicit measurements of the Young's modulus of the protein film by conventional AFM

226 to ascertain due to potential changes in the Young's modulus of the sensor upon a change in mass load

227 TiO2) induces large changes in the effective Young's modulus of the sensor.

228 d through analytical modeling, we derive the Young's modulus of the unfixed cell and unravel the depe

229 The Young's modulus of this silicone jacket matched with the

230 s were well ordered and highly rigid, with a Young's modulus of up to 5-7 GPa, which is comparable to

231 that manifests remarkable flexibility and a Young's modulus of ~33 GPa.

232 When measuring the elastic (Young's) modulus of cells using AFM, good attachment of

233 ows a reliable determination of the elastic (Young's) modulus of soft samples, including living cells

234 bending rigidity measurement, a stretching (Young's) modulus of the same chromosome was measured in

235 crostructure, specifically the pore size and Young's modulus, of collagen-glycosaminoglycan scaffolds

236 irectly testing the effects of varying strut Young's modulus on cell motility showed a biphasic relat

237 l reproduced the quadratic dependence of the Young's modulus on the concentration of polymerized hemo

238 macroscopic material properties such as the Young's modulus or Poisson's ratio for different types o

239 rtery distensibility (P < .01) and increased Young's modulus (P = .02).

240 Elastic (Young's) modulus prior to treatment was correlated with

241 The magnitude of the Young's modulus provides quantitative support for the do

242 fected by stiffness within the physiological Young's modulus range of 0.5 kPa to 100 kPa.

243 to quote a single parameter quantity, e.g., Young's modulus, rather than the minimum of two terms of

244 >0.6 the material behaved as a solid with a Young's modulus rising from approximately 20 MPa at a ma

245 ver the relative density range, 0.5 to 0.65, Young's modulus scales as (density)n where n(C)<n(H)<n(D

246 Young's modulus showed significant differences by region

247 ate the structure with the anisotropy in the Young's modulus, showed that the high stiffness arises a

248 which provide information on their strength, Young's modulus, strain at break and toughness modulus.

249 Data showed that the scaffolds had a similar Young's modulus, suggesting identical stiffness, and rev

250 The Young's modulus, swelling ratio, acid uptake and digesti

251 The Young's modulus, tensile strength, and thermal stability

252 which may explain why the strain had a lower Young's modulus than the WT.

253 om submicrometre voids, and shows an average Young's modulus that is 2-3 orders of magnitude smaller

254 aterials can exhibit a viscoelastic modulus (Young's modulus) that is far greater than that of either

255 harge passed during electrode oxidation, and Young's modulus, the change in strain exhibited by Ni an

256 types produced thicker myotubes and lowered Young's modulus through extracellular matrix remodeling,

257 This combination is used to estimate Young's modulus throughout the volume.

258 ion inhibitors resulted in a decrease in the Young's modulus to values similar to those obtained with

259 tact models provides a single parameter, the Young's modulus, to describe the elastic properties of c

260 ies of the silk (ultimate stress and strain, Young's modulus, toughness) over time.

261 Young's modulus trended higher in the temporal region an

262 ent to stiffen the material (i.e., increased Young's modulus) under load.

263 We also demonstrated that the change in Young's modulus upon mass loading can be eliminated from

264 hase disorder strength using QPI, as well as Young's modulus using AFM, across two breast cancer cell

265 Here, we demonstrate volumetric imaging of Young's modulus using ultrahigh-resolution optical coher

266 In addition, the axial Young's modulus values derived from the persistence leng

267 hough tissues are associated with a range of Young's modulus values for bulk rigidity, at the subcell

268 hydrogel-based elastic microelectronics with Young's modulus values in the kilopascal range.

269 Greater hardness and Young's modulus values near the dento-enamel junction re

270 o and in vitro expanded COC matrices yielded Young's modulus values of 0.5 +/- 0.1 Pa and 1.6 +/- 0.3

271 Young's modulus values up to 10 times higher than existi

272 Young's modulus was <1 MPa from 5% to 20% strain, before

273 isplacements of the carotid artery wall, and Young's modulus was 2-fold greater in shams at 1 week po

274 The best estimate for Young's modulus was approximately 3-4 GPa.

275 Increasing Young's modulus was associated with: increasing stress a

276 Young's modulus was calculated as 22.6 +/- 9.2 MPa in pa

277 Also, Young's modulus was correlated with Doppler findings and

278 alculated by integration, and a bulk corneal Young's modulus was derived by mathematical analysis.

279 ar adhesion force was greatly reduced, while Young's modulus was highly elevated in resveratrol treat

280 The Young's modulus was measured based on displacements of t

281 Finally, the higher Young's modulus was most associated with higher intimal

282 Finally, Young's modulus was negatively correlated with SOST (r=-

283 The effective longitudinal Young's modulus was not significantly affected by A22 tr

284 Young's modulus was well predicted by a combination of m

285 The elastic (Young's) modulus was found to decrease by about 100-fold

286 were determined and the tendon stiffness and Young's modulus were calculated.

287 Hardness and Young's modulus were greater near the dento-enamel junct

288 nical properties including ~127% increase of Young's modulus, which is attributed to both the alignme

289 stic impedance to be used as a surrogate for Young's modulus, which is difficult to obtain in vivo.

290 The Young's modulus, which is the slope of a linear stress-s

291 Young's modulus, which was obtained from measurements pe

292 Correlation of renal tissue Young's modulus with eGFR suggests that SWE may be used

293 ion tests reveal an out-of-plane decrease in Young's modulus with increasing GO content.

294 High-resolution imaging of Young's modulus with optical coherence elastography may

295 c shells, which use only the two-dimensional Young's modulus (Y) and the bending modulus (kappa) to d

296 ence length, l(P) approximately 0.5 mum, and Young's modulus, Y approximately 9 MPa; both are consist

297 monstrate better predictive capabilities for Young's modulus, yield strength, and especially ultimate

298 Alterations of Young's modulus (YM) and Poisson's ratio (PR) in biologi

299 n films had higher tensile strength (TS) and Young's modulus (YM), but lower elongation at break (EAB

300 as a major contributor to the cardiomyocytes Young's modulus (YM).