ライフサイエンスコーパス: thermal expansion

1 1183 m(2) g(-1)) and exhibits negative area thermal expansion.

2 that is responsible for the unusual negative thermal expansion.

3 ructure, giving a non-uniform coefficient of thermal expansion.

4 posting materials with positive and negative thermal expansion.

5 matic liquid crystal molecules is altered by thermal expansion.

6 that from the traditionally used mechanism, thermal expansion.

7 overcome potential problems associated with thermal expansion.

8 ery strong anisotropic positive and negative thermal expansion.

9 duce a detrimental lowering of the porcelain thermal expansion.

10 at is equivalent to free volume changes from thermal expansion.

11 and slow muscle fibers in rigor, indicating thermal expansion.

12 ch presumably was an indirect consequence of thermal expansion.

13 shrinkage due to an arbitrary coefficient of thermal expansion.

14 use only negligible shifts in porcelain bulk thermal expansion.

15 istance correlates well with the macroscopic thermal expansion.

16 al mechanics of the nuclei and the cell, and thermal expansion.

17 rmal expansion and guiding the regulation of thermal expansion.

18 mi energy, work function, and coefficient of thermal expansion.

19 tions are the driving forces of the colossal thermal expansion.

20 ual shearing, bending, and gradient modes of thermal expansion.

21 nt level, with an additional 1.6 metres from thermal expansion.

22 r, and the collapsed phase shows nearly zero thermal expansion.

23 A similar effect causes negative thermal expansion.

24 oxide due to their different coefficients of thermal expansion.

25 al and reduces the magnitude of its negative thermal expansion.

26 ice as much sea-level rise since 1900 as has thermal expansion.

27 ion vibrations, which directly controls the thermal expansion.

28 mework materials with phonon-driven negative thermal expansion.

29 ess of the sign of their contribution to the thermal expansion.

30 nsverse vibrations, thus inhibiting negative thermal expansion.

31 to sea level rise are estimated to come from thermal expansion (0.288 m) and the melting of mountain

32 s similar to that of ZrW(2)O(8) and positive thermal expansion above approximately 1100 K.

33 ept that increase in free volume acquired in thermal expansion above the main gel-liquid crystal tran

34 at this limit by compensating the intrinsic thermal expansion, allowing a sub-25 Hz linewidth and a

35 3)Ge exhibits a pronounced uniaxial negative thermal expansion along c, with a coefficient of -1.57 v

36 Herein, we report a near isotropic zero thermal expansion (alpha(l) = 1.10 x 10(-6 )K(-1), 260-3

37 analysis of variance, and the coefficient of thermal expansion, alpha, was obtained from this analysi

38 phase transition undergoes biaxial negative thermal expansion (alphaa = -54.8(8) x 10(-6) K(-1), alp

39 (-6) K(-1)) and exceptionally large uniaxial thermal expansion (alphab = 303(1) x 10(-6) K(-1)).

40 Ag3[Co(CN)6], exhibits positive and negative thermal expansion an order of magnitude greater than tha

41 The relative thermal expansion and compressibilities of the cubic and

42 nditions is significantly compromised by the thermal expansion and contraction of components of an SE

43 potential model that is able to describe the thermal expansion and elastic properties of ceria to giv

44 anion intercalation of graphite followed by thermal expansion and electrochemical hydrogen evolution

45 el for conductive 3D-printed structures with thermal expansion and external strain will lead to an ev

46 Inclusion of thermal expansion and glacier contributions results in a

47 significance for understanding the nature of thermal expansion and guiding the regulation of thermal

48 es, such as light weight, high strength, low thermal expansion and high thermal conductivity.

49 and pollucite exhibit a lower coefficient of thermal expansion and inversion temperature than leucite

50 xis, thus leading to interesting anisotropic thermal expansion and magnetic properties.

51 Our findings pave the way to tailor thermal expansion and obtain prominent mechanical proper

52 The effects of this conversion on porcelain thermal expansion and porcelain-metal thermal compatibil

53 has been taken up by the oceans, leading to thermal expansion and sea-level rise.

54 tates of proteins impose constraints against thermal expansion and that, hence, knowledge of site-spe

55 Oceanic thermal expansion and the Antarctic Ice Sheet contribute

56 sibly useful collective properties: negative thermal expansion and tuneable porosity of the liposome

57 ociated with changes in ocean volume (mostly thermal expansion) and in ocean mass (melting and contin

58 catalysis, postsynthetic exchange, negative thermal expansion, and crystal growth.

59 rmonic effects, including thermal softening, thermal expansion, and soft vibrational modes of the dis

60 The elastic modulus and coefficient of thermal expansion are fundamental properties of elastica

61 ng network that undergo strongly anisotropic thermal expansion around the phase transition.

62 r loss or humidity change due to heating, 6) thermal expansion at various humidities, and 7) water lo

63 ce of argentophilic interactions and extreme thermal expansion behavior may explain a variety of ther

64 The thermal expansion behavior of isostructural variants of

65 The thermal expansion behavior of the materials was measured

66 ition metal site did not strongly affect the thermal expansion behavior, giving Ag3[FeIII(CN)6] as a

67 l-strain gradients caused by the mismatch in thermal expansion behaviour between different fuel cell

68 The existence of asymmetric elastic and thermal expansion behaviour has fundamental implications

69 hermore, both positive and abnormal-negative thermal expansion behaviours on medium-range order are o

70 al conductivity of nylon and its anisotropic thermal expansion, bending occurs when a nylon beam is d

71 arises from poorly understood differences in thermal expansion between the folded and unfolded states

72 hick polyimide patches with nearly identical thermal expansion but different gas absorption character

73 chieve a negative or ultralow coefficient of thermal expansion, but very few demonstrate tunability o

74 an additional 320% sea level rise caused by thermal expansion by the end of the 21st century.

75 sed as a simple illustration of how negative thermal expansion can arise from the thermally induced r

76 gh-power pulsed RF/microwave energy, a rapid thermal expansion can lead to stress waves within the bo

77 Even minor external mechanical stress or thermal expansion can result in membrane delamination an

78 However, it has been poorly understood how thermal expansion can show anomalies such as colossal po

79 Materials with engineered thermal expansion, capable of achieving targeted area/vo

80 oisson's ratio (-0.25) and a negative linear thermal expansion coefficient (-1.8 x 10(-6) per degrees

81 nce of the polar halocline, namely, that the thermal expansion coefficient (TEC) of seawater increase

82 itions and making use of graphene's negative thermal expansion coefficient (TEC), which we measure to

83 ermal expansion (NTE) with an average linear thermal expansion coefficient alpha = (-2.4 +/- 0.4) x 1

84 there is no distinct peak in the plot of the thermal expansion coefficient alpha versus temperature n

85 A small difference in the thermal expansion coefficient between these steels creat

86 , Zr1-xSnxMo2O8 (0 < x < 1), whose isotropic thermal expansion coefficient can be systematically vari

87 l differentialT(2)) as Hepler's constant and thermal expansion coefficient have been estimated.

88 ential(2)V(0)/ partial differentialT(2)) and thermal expansion coefficient have been estimated.

89 the 25-1300 degrees C temperature range, its thermal expansion coefficient is 9.5 x 10(-6 )K(-1).

90 Graphene's negative thermal expansion coefficient is generally explained by

91 g that it occurs irrespective of whether the thermal expansion coefficient is positive, negative, or

92 ures up to 300 degrees C which is due to the thermal expansion coefficient mismatch generating intern

93 The films exhibit a giant negative thermal expansion coefficient of approximately -1,200 pp

94 The negative thermal expansion coefficient of graphene is an essentia

95 mal equilibrium with the well-known negative thermal expansion coefficient of graphene.

96 can be used to measure the unusual negative thermal expansion coefficient of graphene.

97 The room temperature thermal expansion coefficient of Hf2CO2 is 6.094 x 10(-6

98 The thermal expansion coefficient of the composite nanofiber

99 ties for which the anomalous diffusivity and thermal expansion coefficient of water are observed, and

100 ined with materials demonstrating a positive thermal expansion coefficient to fabricate composites ex

101 t molar volume, apparent molar expansion and thermal expansion coefficient were calculated.

102 and its derivatives, mean atomic volume and thermal expansion coefficient) of the two end-members of

103 The linear thermal expansion coefficient, a, over the range from ro

104 lizable to materials of low modulus and high thermal expansion coefficient, and we use it here to ach

105 rmal dependence of lattice parameter, linear thermal expansion coefficient, enthalpy and specific hea

106 coefficient, k , analogous with the isobaric thermal expansion coefficient, established the rate of r

107 utcomes in terms of the relevant parameters (thermal expansion coefficient, glass transition temperat

108 aric heat capacity, and the magnitude of its thermal expansion coefficient, increase sharply on cooli

109 composite) may be used to achieve a tunable thermal expansion coefficient.

110 tibility, the Gruneisen coefficient, and the thermal expansion coefficient.

111 ransitions are manifested differently in the thermal expansion coefficient.

112 Because of the large mismatch in the thermal-expansion coefficient between the metal contacts

113 M) polymorphs effects unusually large linear thermal expansion coefficients (a (a) , a (b) , a (c) ,

114 In this Communication, very large negative thermal expansion coefficients (alpha(T)) are reported f

115 Materials with colossal thermal expansion coefficients (CTEs) hold a significant

116 asured densities, partial molar volumes, and thermal expansion coefficients are also reported.

117 Materials with zero/near zero thermal expansion coefficients are technologically impor

118 ively, at 25 degrees C, and their respective thermal expansion coefficients are within 20% of the mon

119 high-entropy Invar alloys with extremely low thermal expansion coefficients around 2 x 10(-6) per deg

120 henomenon of strain induced by a mismatch in thermal expansion coefficients between a thin film and i

121 ur interfacial layer reduces the mismatch of thermal expansion coefficients between the different lay

122 t the Ag site (by D) was shown to reduce the thermal expansion coefficients by an order of magnitude.

123 propanol, showing that fine control over the thermal expansion coefficients can be achieved and that

124 tes and creases, an extremely broad range of thermal expansion coefficients can be obtained.

125 se their high lattice mismatch and different thermal expansion coefficients cause the epitaxial layer

126 ssure-volume-temperature space and near-zero thermal expansion coefficients comparable to or even sma

127 ) demonstrates one of the largest volumetric thermal expansion coefficients for inorganic solids.

128 In connection with the NLO properties the thermal expansion coefficients for K2P2Se6 are reported.

129 This study of the thermal expansion coefficients of different inclusion co

130 e amorphous nature of SiO2 and the differing thermal expansion coefficients of the two materials.

131 The obtained gruneisen parameter and thermal expansion coefficients show the maximum value am

132 Linear thermal expansion coefficients, alphal, ranging from -7.

133 Mechanical strength, heat capacities, thermal expansion coefficients, and thermal conductiviti

134 rmation energy and Young's modulus, and high thermal expansion coefficients, not only enables thin fi

135 alpha-K(2)Hg(3)Ge(2)S(8) shows anisotropic thermal expansion coefficients.

136 r the design of systems with a wide range of thermal expansion coefficients.

137 sion, limiting its usefulness for controlled thermal expansion composites.

138 rystals of 2 showed the large and reversible thermal expansion/compression anisotropy, which accounts

139 ed structures with engineered coefficient of thermal expansion consist of bi-material 2D or 3D lattic

140 predominantly driven by thermal stresses via thermal expansion/contraction during heat cycling.

141 such as colossal positive, zero, or negative thermal expansion (CPTE, ZTE, or NTE), especially in qua

142 The coefficient of thermal expansion (CTE) is a physical quantity that indi

143 Ultra-low coefficient of thermal expansion (CTE) is an elusive property, and narr

144 by the mismatch between the coefficients of thermal expansion (CTE) of the consecutive device layers

145 On heating, its coefficient of thermal expansion (CTE) smoothly increases, leading to a

146 erials with large or ultralow coefficient of thermal expansion (CTE), achieving a broad range of CTE

147 ng-standing challenge of high coefficient of thermal expansion (CTE), limiting the applications in hi

148 Thermal expansion, defined as the temperature dependence

149 lf-organized fracture mechanism analogous to thermal expansion-driven lithospheric uplift, in which g

150 ctical merit as thermal offsets for positive thermal expansion due to its metallic properties.

151 potential source of change in bulk porcelain thermal expansion during fabrication of porcelain-fused-

152 s in fact fully consistent with heat-induced thermal expansion during illumination.

153 itionally, we develop a model linking sample thermal expansion dynamics to cantilever excitation ampl

154 Thermal expansion, electrical resistivity, magnetization

155 Because the coefficient of thermal expansion for sanidine is substantially lower th

156 erate behavior, such that the coefficient of thermal expansion for the host Zn[M(CN)(2)](2) framework

157 their elastic modulus (E) and coefficient of thermal expansion [Formula: see text] The inks are print

158 nsertion of Li ions into the simple negative thermal expansion framework material ScF3, doped with 10

159 The high-pressure phase shows negative thermal expansion from 20 to 300 kelvin.

160 lation offers an effective method to control thermal expansion from positive to zero to negative by i

161 over, the phenomenon of atomic diffusion and thermal expansion generates joints which were initially

162 ic framework (MOF) that displays anisotropic thermal expansion has been prepared and characterized by

163 Atomic mechanisms of anomalous thermal expansion have been studied by a comprehensive s

164 The negative thermal expansion--heating from 4.2 to 32 K leads to con

165 however, it increases their coefficients of thermal expansion, imposing constraints on the processin

166 d, hydrophobic thickness, and coefficient of thermal expansion in a manner that varies with lipid typ

167 ng the tip of an AFM probe to locally detect thermal expansion in a sample resulting from absorption

168 magnetic field dependence, and the negative thermal expansion in all three lattice parameters, sugge

169 ern sheds light on the mechanism of negative thermal expansion in ambient-pressure Zn(CN)2.

170 electric transition-metal formates, negative thermal expansion in cyanide frameworks, and the mechani

171 nce of solvent effects in the latter (larger thermal expansion in H(2)O than in D(2)O), whereas in ou

172 Thermal expansion in magnetic fields and magnetostrictio

173 likely a general strategy for the control of thermal expansion in MOFs.

174 ective method is demonstrated to control the thermal expansion in open-framework materials by adjusti

175 smooth transition from negative to positive thermal expansion in the a-b plane of this tetragonal ma

176 hat the high-temperature phase has zero area thermal expansion in the ab-plane.

177 general and effective method for controlling thermal expansion in the many known framework materials

178 invariant with temperature, and the negative thermal expansion in this case is caused by transverse v

179 acterized both NLC and extremely anisotropic thermal expansion, including negative thermal expansion

180 m temperature, the coefficient of volumetric thermal expansion is among the largest for any extended

181 l guest-dependence of the framework negative thermal expansion is documented.

182 s are of fundamental interest and control of thermal expansion is important for practical application

183 A tunable thermal expansion is reported in nanosized anatase by ta

184 s that are up to twice those in 2, while the thermal expansion is substantially smaller.

185 the compressibility, and the coefficient of thermal expansion, is unknown.

186 ncluding broad band gap tunability, negative thermal expansion, largely reduced thermal conductivity,

187 This results in positive thermal expansion, limiting its usefulness for controlle

188 may be generally applicable to regions where thermal expansion lowers crustal density with depth.

189 ltimate strain), which outperforms other low thermal expansion (LTE) metallic materials.

190 We report on neutron diffraction, thermal expansion, magnetostriction, dielectric, and spe

191 esign principle of barrier layers beyond the thermal expansion matching criterion.

192 or of isostructural variants of the colossal thermal expansion material Ag3[CoIII(CN)6] has been inve

193 or, giving Ag3[FeIII(CN)6] as a new colossal thermal expansion material.

194 r is seen, and ferrierite becomes a negative thermal expansion material.

195 ve and versatile strategy to design colossal thermal expansion materials, yet being represented by on

196 ratures, much higher than any known negative-thermal-expansion materials under similar operating cond

197 e effects of rubidium and cesium leucites on thermal expansion, microstructure, crack deflection patt

198 Dental porcelains rely on the high-thermal-expansion mineral leucite to elevate their bulk

199 instant release of devices by exploiting the thermal expansion mismatch between adjacent materials is

200 ed by microcracks that are the result of the thermal expansion mismatch between leucite and the surro

201 Mechanical strain induced by thermal expansion mismatch between the substrate and rub

202 , annealing(10-12), van der Waals force(13), thermal expansion mismatch(14), and heat-induced substra

203 nergy of the transistors and the interfacial thermal expansion mismatch, in which band-like transport

204 ition, parameters such as the coefficient of thermal expansion must be kept within a reasonable range

205 At low temperatures it shows strong negative thermal expansion (NTE) (60-110 K, alpha(l) approximatel

206 Negative thermal expansion (NTE) alloys possess great practical m

207 tropic thermal expansion, including negative thermal expansion (NTE) along the NLC axis, in a simple

208 ectance, photoluminescence, and 1-D negative thermal expansion (NTE) behaviors of all three systems a

209 The negative thermal expansion (NTE) in CuO is explained via electron

210 we find also results in anisotropic negative thermal expansion (NTE) in the same material.

211 Negative thermal expansion (NTE) is a common phenomenon in MOFs a

212 erage structures in the disordered, negative thermal expansion (NTE) material, Zn(CN)2.

213 axations of the M-M bond distances, negative thermal expansion (NTE) with an average linear thermal e

214 e transformation that gives rise to negative thermal expansion (NTE).

215 nic frameworks are known to display negative thermal expansion (NTE).

216 on cooling, and are said to exhibit negative thermal expansion (NTE); but the property is exhibited i

217 aterials which contract on heating (negative thermal expansion, NTE) are of significant interest for

218 The temperature at which zero thermal expansion occurs evolves from ~186 K for the Zn-

219 We also report the various structures and thermal expansion of "cubic" SnMo2O8, and we use time- a

220 The coefficient of thermal expansion of 4 nm TiO2 along a-axis is negative

221 lasses, there have been no reports where the thermal expansion of a MOF has been tuned continuously f

222 uccessful measurements of the coefficient of thermal expansion of a single-crystal copper sample demo

223 We studied the nanoscale thermal expansion of a suspended resistor both theoretic

224 The study demonstrates how thermal expansion of an interior air pocket causes jetti

225 f the Earth's core requires knowledge of the thermal expansion of iron-rich alloys at megabar pressur

226 heit's glass-bulb thermometer, we mapped the thermal expansion of Joule-heated, 80-nanometer-thick al

227 (the effective linear thermal coefficient of thermal expansion of leucite over the range of 25 degree

228 It was concluded that the thermal expansion of leucite-reinforced porcelain can be

229 that were measured for the bulk modulus and thermal expansion of MgSiO3 perovskite provided data tha

230 The cold compression and thermal expansion of Mo have been measured up to 80 GPa

231 42.72x10(-6) K(-1) )-a range that covers the thermal expansion of most inorganic compounds.

232 The effect of guests on the thermal expansion of open-framework structures was inves

233 The purpose of this study was to measure the thermal expansion of sanidine by high-temperature X-ray

234 due to the paucity of published data on the thermal expansion of sanidine.

235 NMR measurements, has been used to study the thermal expansion of siliceous zeolite ferrierite as it

236 The control of thermal expansion of solid compounds is intriguing but r

237 e recorded a sequence of images of the axial thermal expansion of the central bridge region of the su

238 s in materials science, as shown by colossal thermal expansion of the cocrystal involving I...Sb halo

239 Both the compressibility and the thermal expansion of the eluent were taken into account.

240 correlation was observed between the global thermal expansion of the folded proteins and the number

241 magnets owing to the existence of a negative thermal expansion of the lattice.

242 The high thermal expansion of the mineral leucite has been exploi

243 We further conclude that neither thermal expansion of the nanoparticles nor a carbon-stea

244 observed peak shifts, which we attribute to thermal expansion of the NDs and thus a total release of

245 ce the 1970s is caused by the combination of thermal expansion of the ocean and increased ice-mass lo

246 ice-mass loss, terrestrial water storage and thermal expansion of the ocean could not be reconciled w

247 f the contributions to sea-level change from thermal expansion of the ocean, ice-mass loss and change

248 -volume changes, and around 17.4 metres when thermal expansion of the oceans is included.

249 , where alkyl chain melting drove a negative thermal expansion of the surface layer spacing.

250 l, the stress transients are consistent with thermal expansion of the tissue samples.

251 Thermal expansion of the warming ocean provides a conser

252 ts a unified approach and descriptor for the thermal expansion of TMD monolayers, which can serve as

253 ced ocean warming by directly monitoring the thermal expansion of water in the wake of cyclones, usin

254 nd molecules (H2 O) can substantially switch thermal expansion of YFe(CN)6 from negative (alphav =-33

255 e and other cell components by introducing a thermal-expansion offset.

256 In this design, during heating and thermal expansion, only oil was expelled from the compar

257 rusion of silicate magma and exclude in situ thermal expansion or pressurization of the hydrothermal

258 Thermal expansion (or contraction) causes the nematic li

259 probe pull-in effect, while HPMC showed only thermal expansion over the temperature range studied.

260 ial wells consistent with the measured large thermal expansion parameter.

261 ich accommodate the more than tenfold larger thermal expansion perpendicular to these layers, we attr

262 d 10 710 ppm K(-1) ), but also large biaxial thermal expansion properties (e.g., > 21% for 20 K tempe

263 gineered systems offer opportunities to tune thermal expansion properties in interesting ways.

264 Thermal expansion properties of solids are of fundamenta

265 e effect on the host mechanics, altering the thermal expansion properties of the material.

266 The thermal expansion properties of two isostructural zinc d

267 vanced mechanical metamaterials with unusual thermal expansion properties represent an area of growin

268 d have been resolved by changing the solvent thermal expansion properties with a series of linear alk

269 c/anisotropic, and homogeneous/heterogeneous thermal expansion properties, with additional features i

270 ligible effect of pressure on the volumetric thermal expansion properties.

271 ical mechanism of dual-phase synergy on both thermal expansion regulation and mechanical property enh

272 vities decrease with the porosity, while the thermal expansion remains unaffected.

273 erials into giant levels of biaxial/uniaxial thermal expansion/shrinkage are presented.

274 Thermal expansion, specific heat and magnetization measu

275 ferential growth, shrinkage, desiccation, or thermal expansion, spontaneously generates these pattern

276 The mechanism of such substantial thermal expansion switching is revealed by joint studies

277 Control over thermal expansion (TE) behaviors in solid materials is o

278 Achieving substantial anisotropic thermal expansion (TE) in solid-state materials is chall

279 Control over the thermal expansion tensor achieved in this way provides a

280 symmetric elastic modulus and coefficient of thermal expansion that are inherently related to termina

281 This gives negative thermal expansion that is 14 times larger than in ZrW2O8

282 t time a physical route to achieve near zero thermal expansion through application of pressure.

283 nimization of stress because of differential thermal expansion through design for high temperature op

284 ure, assumes the role of not only modulating thermal expansion through magnetic interaction but also

285 s work have implications for controlling the thermal expansion through superexchange interaction, via

286 ansion mineral leucite to elevate their bulk thermal expansion to levels compatible with dental PFM a

287 their manufacturers to be closely matched in thermal expansion to these alloys.

288 e gases contribute to sea-level rise through thermal expansion (TSLR) over much longer time scales th

289 We attribute the large negative thermal expansion, unprecedented in fullerene or other m

290 ximately 0.1, we observe two features in the thermal expansion upon cooling, one that appears to be a

291 E) is a physical quantity that indicates the thermal expansion value of a material upon heating.

292 n when internal cages are empty but positive thermal expansion when additional atoms or molecules fil

293 Many framework-type materials show negative thermal expansion when internal cages are empty but posi

294 range of anomalies in nature in addition to thermal expansion, which may include gigantic electrocal

295 Here we reveal the presence of negative thermal expansion with a large coefficient value of -14.

296 D data, Pr demonstrates a highly anisotropic thermal expansion with peak positive (+1295(22) MK(-1))

297 tion entropy at constant strain is caused by thermal expansion, with negligible contribution from the

298 These materials exhibit anisotropic thermal expansion yielding some of the largest linear ex

299 progress in modern technologies demands zero thermal expansion (ZTE) materials with multi-property pr

300 ricate composites exhibiting an overall zero thermal expansion (ZTE).