ライフサイエンスコーパス: compressibility

1 nced Fermi velocity, and interaction-reduced compressibility.

2 amatic decrease in clot volume and a peak in compressibility.

3 ase in the lipid assemblies' total adiabatic compressibility.

4 temperature dependence of a solute's partial compressibility.

5 at velocities controlled by the interface's compressibility.

6 emoral and popliteal veins were assessed for compressibility.

7 c moment and occurrence of axial alternative compressibility.

8 properties unique to bulk materials such as compressibility.

9 ing to curvature localization and a negative compressibility.

10 pansibility while resulting in a decrease in compressibility.

11 ivity), which dictates viscosity and affects compressibility.

12 tely the same size and density but different compressibility.

13 o exhibits both positive and negative linear compressibility.

14 ime scale and suggesting regions of variable compressibility.

15 when stretched, so they have positive linear compressibilities.

16 s contain four parameters: bilayer thickness compressibility 1/B, bilayer bending rigidity Kc, the ch

17 e the density (0.1-1% relative uncertainty), compressibility (1% relative uncertainty), scattering co

18 he density (0.1-1% relative uncertainty) and compressibility (1-3% relative uncertainty) of previousl

19 is also accompanied by a positive change in compressibility, 14 x 10(-4) cm3 x mol(-1) x bar(-1), bu

20 Pressure shifts of holes allow the local compressibility about the APT to be determined.

21 X-ray diffraction data show that compressibility along the c-axis changes around 12 GPa,

22 The layer compressibility also decreased with increasing carbohydr

23 ntify a molecular basis for the variation in compressibility among globular proteins.

24 ncluding negative Poisson's ratios, negative compressibilities and phononic bandgaps.

25 Both compressibilities and relative volume fluctuations in PL

26 However, because the area compressibility and bending moduli of SM:cholesterol bil

27 m lengthscales yields the membranes' lateral compressibility and bending rigidity and demonstrates th

28 that relates etas to the pure DPPC monolayer compressibility and collapse pressure.

29 lar expansibility, apparent molar isentropic compressibility and compressibility hydration number.

30 t specific volume, isentropic apparent molar compressibility and compressibility hydration numbers an

31 Finally, from the obtained compressibility and density, the acoustic scattering coe

32 ein (CRP) has been shown to modulate protein compressibility and dynamics.

33 e that provides its mechanical properties of compressibility and elasticity, is one of the first matr

34 water-binding capacity of aggrecan provides compressibility and elasticity.

35 the data reveal interaction-driven negative compressibility and electron-hole asymmetry in N = 0, 1

36 Analysis of our compressibility and expansibility data reveals that the

37 Liquid water's isothermal compressibility and isobaric heat capacity, and the magn

38 etic surface activities, yielding lower film compressibility and lower maximum dynamic surface tensio

39 d several anomalies: maxima in the adiabatic compressibility and nonmonotonic density dependence of t

40 structural integrity of the nanotubes or the compressibility and porosity of the nanotube network.

41 The influence of the antiviral compound on compressibility and positional fluctuations is reported.

42 d result in rare properties: negative linear compressibility and stretch densification.

43 sibility reflects both the protein intrinsic compressibility and the difference between the compressi

44 capacity of unfolding infers a link between compressibility and the enthalpy of unfolding.

45 ther, a newly recognized correlation between compressibility and the heat capacity of unfolding infer

46 Both the compressibility and the thermal expansion of the eluent

47 an predicts full coexistence curves, osmotic compressibilities, and second virial coefficients under

48 the DPPC bilayer; bulk compressibility, area compressibility, and bending modulus were only perturbed

49 yer thickness (which we refer to as length), compressibility, and spacing between the individual mole

50 at low temperature in the heat capacity, the compressibility, and the coefficient of thermal expansio

51 lar atoms is somewhat larger than bulk water compressibility, and the compressibility of water around

52 he nonpolar antiviral compound increases the compressibility, and thus the conformational flexibility

53 for achieving such negative linear and area compressibilities are described for single crystals and

54 t regimes, characterized by their degrees of compressibility, are isolated in the parameter space.

55 hanical properties of the DPPC bilayer; bulk compressibility, area compressibility, and bending modul

56 their isentropic apparent molar and specific compressibilities, as well as their compressibility hydr

57 s,2,varphi, and apparent specific isentropic compressibilities, ASIC, were calculated from measured d

58 These many-body states exhibit negative compressibility but the compressibility returns to posit

59 ulted in condensed films with lower in-plane compressibilities, but consistently larger cross-section

60 ate also has no significant influence on the compressibility calculated for cyt c, although a slightl

61 aracterized by similar changes in volume and compressibility calculated per mole Co(NH(3))(6)(3+): De

62 ity), as a result of dynamic changes in bead compressibility causing the displacement of the bead fro

63 ependence of the volume change, the standard compressibility change (Delta K(o)T), is typically assum

64 a were fitted to a model that assumes a zero compressibility change, the Delta G(o) value of 4.0 +/-

65 compressive modulus), volumetric or apparent compressibility changes (as further indicated by apparen

66 The compressibility changes are consistent with changes in s

67 first transition is evidenced by noticeable compressibility changes in distinct Raman-active modes,

68 The isothermal compressibility coefficient (beta(T)(lipid)) of PLFE LUV

69 isothermal compressibility, their respective compressibility coefficients, partial specific volume, a

70 ignificantly larger bending modulus and area compressibility compared to DPPC.

71 ti-string BWT is also shown to have a higher compressibility compared with the input multi-string BWT

72 er-tetrahedral bond angle, resulting in high compressibility, continual breakup of tetrahedral connec

73 n and molten silicates, indicating that melt compressibility controls siderophile-element partitionin

74 An increase in compressibility correlates with an entropically more fav

75 Because electronic compressibility corresponds solely to the charge respons

76 Analysis of the elastic moduli of area compressibility (Cs(-1)) as a function of molecular area

77 chieved by using only density and isothermal compressibility data at atmospheric pressure through the

78 We convert our area compressibility data into interfacial tension values to:

79 We report compressibility data on single-domain, globular proteins

80 by a volume decrease of 0.014 cm3 g-1 and a compressibility decrease of 3.8 x 10(-6) cm3 g-1 bar-1.

81 olar volume (DeltaV degrees ) and isothermal compressibility (Deltabeta(T)) of conformational substat

82 artial molar volumes (DeltaV) and isothermal compressibilities (DeltakappaT ) between all the states

83 by high-precision measurements of the local compressibility, density, and pressure.

84 illouin quasilongitudinal results with axial compressibilities determined from high-pressure x-ray di

85 We also assess whether hydration water compressibility determined from small compound data can

86 ion can be incorrect and that the neglect of compressibility differences can skew the interpretation

87 olar volume and the apparent molar adiabatic compressibility due to the interaction have been obtaine

88 poly[d(A-T)].poly[d(A-T)] complex volume and compressibility effects correspond to one direct or two

89 The volume and compressibility effects of Ni(2+)-EDTA complex formation

90 Volume and compressibility effects of the first process are positiv

91 range from 11.7 to 23.9 cm(3)mol(-1)and the compressibility effects range from 19.3 x 10(-4)to 43.1

92 G+C content gives an increase in volume and compressibility effects, indicating a rise in the extent

93 g difficulties posed by woody roots and peat compressibility, enabling retrieval of relatively undist

94 The compressibility, estimated from the density fluctuations

95 Imminent divergences of compressibility etc. unfortunately cannot be confirmed d

96 e properties (solubility, thermal stability, compressibility, etc.) of both new and existing drugs.

97 creases (two- to fourfold) in the "in-plane" compressibility for all three lipid types.

98 id mixtures yield smaller molecular area and compressibility for monolayers containing more saturated

99 ts of Co(NH(3))(6)(3+) binding on volume and compressibility have been obtained.

100 s, such as flyweight density, 80% reversible compressibility, high fatigue resistance, high electrica

101 pparent molar isentropic compressibility and compressibility hydration number.

102 sentropic apparent molar compressibility and compressibility hydration numbers and reported.

103 specific compressibilities, as well as their compressibility hydration numbers have been calculated a

104 We present results for the local compressibility in all phases, observing a strong suppre

105 is for an adhesive-cohesive model of protein compressibility in which attractive forces from solvent

106 The Compressibility Index (CI=29.09-32.25%) and Hausner Rati

107 Negative compressibility is a sign of thermodynamic instability o

108 l dependence of local lipid area and bilayer compressibility is also nonmonotonic in the first shell

109 ulated for cyt c, although a slightly larger compressibility is predicted for myoglobin.

110 Because isothermal compressibility is related to volume fluctuation, this s

111 es, for example heat capacity and isothermal compressibility kappaT, show a large increase.

112 reflected in an 8% increase in the intrinsic compressibility, kM, of the protein "native" state.

113 v(zero), and the partial specific adiabatic compressibilities, ks(zero), of globular proteins from t

114 V2( degrees ), and partial molar isentropic compressibilities, Ks,2( degrees ) at infinite dilution,

115 ific volumes, ASV, apparent molar isentropic compressibilities, Ks,2,varphi, and apparent specific is

116 ogether with the adhesive-cohesive model for compressibility, leads to the conclusion that folded pro

117 the macroscopic current density relation and compressibility matrix of the system and hence accessibl

118 oid intermediate formation, and the negative compressibility may be due to the effect of pressure on

119 The increased compressibility may be due to the high concentrations of

120 Here, by performing dual conductance and compressibility measurements in the Kondo regime, we unc

121 Here, we present local electronic compressibility measurements of the FQH effect in the lo

122 Here we perform compressibility measurements on electrons on liquid heli

123 Absolute volumetric and compressibility measurements reveal that all three hairp

124 e compared by determining their elastic area compressibility moduli (Cs-1) as a function of lateral p

125 ft bilayers are thicker and have larger area compressibility moduli than nonraft bilayers.

126 uid-condensed and liquid-expanded phase area compressibility moduli that are significantly larger tha

127 e provided by analyzing the interfacial area compressibility moduli.

128 for area/lipid (A = 47.2 +/- 0.5 A(2)), the compressibility modulus (K(A) = 500 +/- 100 dyn/cm), var

129 etics of bilayer bending, including the area compressibility modulus (K(a)), bilayer bending modulus

130 sition and ethanol concentration on the area compressibility modulus (K(a)), overall mechanical behav

131 cylate effectively reduces the apparent area compressibility modulus and bending modulus of membranes

132 ematically decreased with increasing bilayer compressibility modulus and bilayer thickness.

133 in the absence of tubule formation, the area compressibility modulus and, as such, the bending rigidi

134 tension, dipole density difference, and the compressibility modulus at surface pressures up to the s

135 ut does not greatly alter the actual elastic compressibility modulus at the maximal tested concentrat

136 Quantitatively, the trend in area compressibility modulus follows Traube's rule of interfa

137 Our area compressibility modulus K(A) decreased with increasing t

138 rements indicate that the lipid bilayer area compressibility modulus KA is increased by a large amoun

139 mainly attributed to a decrease in the area compressibility modulus KA We propose that the insertion

140 oncentration required to reach the same area compressibility modulus was reduced roughly by a factor

141 The elastic area compressibility modulus was unaffected between pH 3 and

142 atches to the pore rim and the apparent area compressibility modulus, an intrinsic elastic modulus mo

143 cohol concentration in the bilayer, and area compressibility modulus, as a function of alcohol chain

144 ette aspiration to directly measure the area compressibility modulus, bending modulus, lysis tension,

145 dependent on the bilayer area per molecule, compressibility modulus, or dipole potential, but did de

146 ted proteins by proteases decreases the area compressibility modulus, whereas fixation and cross-link

147 ding to lower lateral diffusion and a higher compressibility modulus, which agrees well with availabl

148 bilayer midplane) and k(m) is the monolayer compressibility modulus.

149 ts the strongest ever observed negative area compressibility (NAC), an extremely rare property, as at

150 ined by radiography, revealed an increase in compressibility near 100 gigapascals indicative of such

151 ons at the fivefold axis and the increase in compressibility near the WIN pocket are discussed in rel

152 spectroscopy (ARPES) for negative electronic compressibility (NEC) in the quasi-three-dimensional (3D

153 ectroscopic signature of negative electronic compressibility (NEC), a result of electron-electron int

154 tructures, which may exhibit negative linear compressibility (NLC) (that is, they expand in one or mo

155 of mechanical anisotropy and negative linear compressibility (NLC) along its c axis.

156 )](3) exhibits the strongest negative linear compressibility (NLC) effect over the largest pressure r

157 unterintuitive phenomenon of negative linear compressibility (NLC) is a highly desirable but rare pro

158 lous elastic behavior (e.g., negative linear compressibility, NLC), transitions between crystalline p

159 ized in terms of differences in their linear compressibilities occasioned by changes in the degree of

160 e backbone promoted closer packing and lower compressibilities of ceramide analogs in interfaces rela

161 t, in the entire temperature range examined, compressibilities of PLFE LUVs are low, comparable to th

162 The relative thermal expansion and compressibilities of the cubic and orthorhombic forms ca

163 rmation decreases the total volume adiabatic compressibilities of the multilamellar vesicle assemblie

164 pore area (~40%) when combined with the area compressibility of alpha-HL revealed an effective membra

165 around polar atoms is about the same as the compressibility of bulk water.

166 lysis for the measurement of the density and compressibility of cells and microbeads; these being the

167 force microscope, we have measured the axial compressibility of DNA and observed the buckling of the

168 proach provides a measure of the algorithmic compressibility of each data series.

169 aluminous perovskites, I have calculated the compressibility of end-member defect-bearing perovskites

170 is for the marked extensibility and negative compressibility of fibrin gels based on the structural a

171 nt a model which incorporates effects due to compressibility of gas in magma.

172 data cannot be used directly to estimate the compressibility of hydration water surrounding proteins.

173 ll compound data can be used to estimate the compressibility of hydration water surrounding proteins.

174 56 atmospheres give an estimate for the area compressibility of KA = 188 dyn/cm.

175 The heat capacity and compressibility of liquid water anomalously increase on

176 onclusions about the origin of the anomalous compressibility of nanocrystals.

177 of multiple mutually coupled subsystems, the compressibility of one subsystem can be negative if it i

178 for adjusting quality scores to improve the compressibility of quality scores without adversely impa

179 ater reduction in sedimentation velocity and compressibility of sediment formed than corn syrup solid

180 The area per molecule and compressibility of SM condensed phases depended upon the

181 CS methods demonstrating the compressibility of spin-echo spectra are presented for s

182 or meconium, on the other hand, modifies the compressibility of surfactant films though optimal compr

183 n transistor to measure the local electronic compressibility of suspended graphene, and we observed a

184 s, the growth plates, and the elasticity and compressibility of the bone.

185 l as compressive strength while reducing the compressibility of the composite.

186 The partial volume and isothermal compressibility of the folded state are 100 mL mol(-1) a

187 on of soft gels need to account for both the compressibility of the gel network and a nonzero surface

188 to explore the dependence of the isothermal compressibility of the hydration shell surrounding globu

189 this capacitance originates from a negative compressibility of the interface electron system.

190 The compressibility of the intermediate is larger than that

191 The compressibility of the melt after the completion of the

192 SNAREs is interpreted as an increase in the compressibility of the membranes, which translates to a

193 oparticle volume fraction, and from this the compressibility of the microparticles is inferred.

194 n be negative if it is countered by positive compressibility of the others.

195 me probed in the experiments represented the compressibility of the outer region of spectrin loops an

196 terms of an interplay between the intrinsic compressibility of the protein and solvation effects.

197 ical interferometry to examine the thickness compressibility of the red cell membrane in situ.

198 upled with mass-spectrometry (MS) to explore compressibility of the secondary structure of proteins u

199 Their presence increases the compressibility of the solvent with the added effect of

200 ntropy of the quality scores and thereby the compressibility of these data (in FASTQ or SAM/BAM/CRAM

201 flux results from the piston-like mechanism, compressibility of water (increase in density of water d

202 The density and compressibility of water adjacent to a melittin dimer is

203 ger than bulk water compressibility, and the compressibility of water around polar atoms is about the

204 s lower than bulk water compressibility, the compressibility of water hydrating apolar atoms is somew

205 The compressibility of water hydrating charged atoms is lowe

206 The compressibility of water in the protein hydration shell

207 mpressibility and the difference between the compressibility of water in the protein hydration shell

208 es may occur to the transport properties and compressibility of, e.g., fluids in planetary interiors,

209 tabilizes the negative bulk modulus (inverse compressibility) of the inclusions.

210 evealed no significant dependence of TM bulk compressibility on the presence of collagen XI.

211 y an integral role in either the diminution (compressibility) or retention (incompressibility) of ori

212 Furthermore, volume and compressibility parameters of cation binding show hydrat

213 ialV&cjs1171;H2O/ partial differentialT) and compressibility ( partial differentialV&cjs1171;H2O/ par

214 .89 mol kg(-1).The apparent molar isentropic compressibility (PhiK(s)) and hydration number (nH) conf

215 ssibility of surfactant films though optimal compressibility properties recover on repetitive compres

216 dynamic property of folded proteins, protein compressibility provides important information about the

217 The experimental determination of protein compressibility reflects both the protein intrinsic comp

218 tes exhibit negative compressibility but the compressibility returns to positive in ultrahigh B.

219 -Vdpi arrangement despite the greater c-axis compressibility, suggesting that the hydride anions act

220 ctuations consistent with water's isothermal compressibility temperature trends.

221 The data require a compressibility term, beta(o)(double dagger), to obtain

222 ygen vacancies do have significantly greater compressibilities than those without such vacancies.

223 exceptional sensitivity the dot's electronic compressibility, that is, its ability to accommodate cha

224 he onset of superfluidity is observed in the compressibility, the chemical potential, the entropy, an

225 ating charged atoms is lower than bulk water compressibility, the compressibility of water hydrating

226 to the increase in density fluctuations and compressibility, the positional fluctuations decreased d

227 In the regime of intermediate compressibility, the two different regularizations give

228 ed partial specific adiabatic and isothermal compressibility, their respective compressibility coeffi

229 We relate intrinsic compressibility to stability by using molecular dynamics

230 The strain-driven counterpart of negative compressibility transitions is a force amplification phe

231 to design metamaterials exhibiting negative compressibility transitions, during which a material und

232 20 GPa, ultimately presenting the same axial compressibility trends with those of nonmagnetic compoun

233 Not only is the duality in compressibility triggered by the availability of potenti

234 egapascal in pore pressure in rocks with low compressibility triggers earthquakes, including the 4.8-

235 f stretchability (up to approximately 100%), compressibility (up to approximately 25%) and bendabilit

236 the change in the partial specific adiabatic compressibility which accompanies the transition.

237 ers influences monolayer viscoelasticity and compressibility which, in turn, influence monolayer coll

238 he product of surface tension and isothermal compressibility, which is another fundamental lengthscal

239 gate the interplay between cell motility and compressibility within the CPM and find that the CPM pre