ライフサイエンスコーパス: thermal expansion

1 matic liquid crystal molecules is altered by thermal expansion.

2 that from the traditionally used mechanism, thermal expansion.

3 overcome potential problems associated with thermal expansion.

4 ery strong anisotropic positive and negative thermal expansion.

5 ion vibrations, which directly controls the thermal expansion.

6 duce a detrimental lowering of the porcelain thermal expansion.

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

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

9 ch presumably was an indirect consequence of thermal expansion.

10 shrinkage due to an arbitrary coefficient of thermal expansion.

11 use only negligible shifts in porcelain bulk thermal expansion.

12 mework materials with phonon-driven negative thermal expansion.

13 nsverse vibrations, thus inhibiting negative thermal expansion.

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

15 that is responsible for the unusual negative thermal expansion.

16 oxide due to their different coefficients of thermal expansion.

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

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

19 posting materials with positive and negative thermal expansion.

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

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

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

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

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

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

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

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

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

29 The relative thermal expansion and compressibilities of the cubic and

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

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

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

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

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

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

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

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

38 Oceanic thermal expansion and the Antarctic Ice Sheet contribute

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

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

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

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

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

44 The thermal expansion behavior of isostructural variants of

45 The thermal expansion behavior of the materials was measured

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

64 The negative thermal expansion coefficient of graphene is an essentia

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

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

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

68 The thermal expansion coefficient of the composite nanofiber

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

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

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

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

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

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

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

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

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

78 ransitions are manifested differently in the thermal expansion coefficient.

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

103 Thermal expansion, defined as the temperature dependence

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

105 Thermal expansion, electrical resistivity, magnetization

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

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

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

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

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

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

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

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

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

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

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

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

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

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

120 Thermal expansion in magnetic fields and magnetostrictio

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

162 42.72x10(-6) K(-1) )-a range that covers the thermal expansion of most inorganic compounds.

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

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

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

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

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

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

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

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

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

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

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

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

175 Thermal expansion of the warming ocean provides a conser

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

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

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

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

180 Thermal expansion (or contraction) causes the nematic li

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

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

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

184 Thermal expansion properties of solids are of fundamenta

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

186 The thermal expansion properties of two isostructural zinc d

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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