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

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

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

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

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

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

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

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

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

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

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

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

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

15 %) alloy with ultralow Young's modulus (36 GPa, versus ~30 GPa for human bone)

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

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

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

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

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

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

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

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

24 Young's modulus and hardness increase correspondingly.

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

57 9.3 +/- 11.5% (P < 0.005), respectively, and Young's modulus by 9.2 +/- 8.2% (P < 0.05) and 30.1 +/-

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

85 /- 29 kPa) was approximately a tenth that of Young's modulus in the longitudinal direction, a differe

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

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

88 - 713 to 3609 +/- 1220 N mm-1; P < 0.05) and Young's modulus increased by 69 % (1.3 +/- 0.3 to 2.2 +/

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

172 >0.6 the material behaved as a solid with a Young's modulus rising from approximately 20 MPa at a ma

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

174 Young's modulus showed significant differences by region

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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