ライフサイエンスコーパス: surface tension

1 with neutral lipids and ability to decrease surface tension.

2 tain surface-active molecules that can lower surface tension.

3 energy of the LD, as opposed to the bilayer surface tension.

4 idal droplets are inherently unstable due to surface tension.

5 riched films at air/liquid interfaces reduce surface tension.

6 ls is many times larger than the zero-strain surface tension.

7 bit sliding angles that decrease with liquid surface tension.

8 zable results and used to explain changes in surface tension.

9 fluids with different density, viscosity and surface tension.

10 dome indicative of an isotropic and uniform surface tension.

11 exhibit a long-ranged attraction mediated by surface tension.

12 ater breaks apart into droplets to lower its surface tension.

13 ticle assembly would be determined solely by surface tension.

14 surfactant as well as its ability to reduce surface tension.

15 nt tetrahydrofuran (THF), because of its low surface tension.

16 use these measurements to estimate line and surface tension.

17 ne tension decreased to a lesser extent than surface tension.

18 ers compared to a flat monolayer at the same surface tension.

19 DeltaG(vdw) can be computed with a constant surface tension.

20 by altering lipid orientation and increasing surface tension.

21 ors, especially for organic liquids with low surface tension.

22 the furrow line tension and the cell poles' surface tension.

23 control surface mechanics and determine cell surface tension.

24 creases lung compliance by reducing alveolar surface tension.

25 ion of the material to the template, and its surface tension.

26 globules due to differences in pressure and surface tension.

27 ures optimized for exploitation of the water surface tension.

28 linking intercellular adhesion and localised surface tension.

29 ed to the aqueous environment, increasing LD surface tension.

30 ke diffusivity, low viscosity, and near-zero surface tension.

31 , overcoming frictional forces, and reducing surface tension.

32 ic orifice as it deforms under the action of surface tension.

33 n ion hydration energy and the neat liquid's surface tension.

34 in vitro studies of cell sorting and tissue surface tension.

35 y length, and the line tension under varying surface tension.

36 n than for mesenchymal spheroids with higher surface tension.

37 er concentrations did not further reduce the surface tension.

38 lative to current estimates assuming a water surface tension.

39 ental constraint set by the physics of water surface tension.

40 y and depletion layers, mass diffusivity, or surface tension.

41 at the sea surface via modulation of bubble surface tension.

42 TMAO, however, reduces the surface tension.

43 d tissues and quantify their viscosities and surface tensions.

44 ility of pulmonary surfactant to sustain low surface tensions.

45 droplet, with a contact angle determined by surface tensions.

46 ral PS films at physiologically relevant low surface tensions.

47 film structures can be used to measure solid surface tensions.

48 mples having a wide range of viscosities and surface tensions.

49 stresses are less able to be counteracted by surface tension, a 3-dimensional (3D) kink-like structur

50 teristics: a surfactant property that lowers surface tension, a cell/spore antiaggregant, and an adhe

51 of the bending modulus of the bilayer to its surface tension, a size which is ~100 nm for the plasma

52 ry surfactant containing SP-A1 reaches lower surface tension after postexpansion interfacial adsorpti

53 asers could be reconfigurably manipulated by surface tension alteration originated from the tiny conc

54 The oil's performance was examined through surface tension analysis, foam formation, coalescence ra

55 ing their size, shape, viscosity, liquidity, surface tension and composition.

56 impacts of pore size and temperature on the surface tension and contact angle of water/vapor and oil

57 nate and ethylene carbonate, which have high surface tension and dipole moment values, can be used to

58 odic assembly is governed by the anisotropic surface tension and elasticity at the interface of beads

59 in electrosprays are affected by viscosity, surface tension and electrical conductivity of the semic

60 The procedure relies on competition between surface tension and fluid inertial forces, and harnesses

61 fatty acids were more efficient in lowering surface tension and gave a much higher dilatational modu

62 range of circuits passively by manipulating surface tension and hydrostatic pressure, and actively u

63 spholipids on LDs, resulting in decreased LD surface tension and impairment to form bridges to the ER

64 converts protrusions into sheets by reducing surface tension and in turn inducing membrane spreading

65 is approach, we show a reduction in membrane surface tension and increased membrane undulations when

66 other measures of solvent cohesion, such as surface tension and internal pressure, gave inferior cor

67 Surface tension and its polar component increase signifi

68 ns on both sides of the membrane affects its surface tension and leads to its lateral expansion.

69 SLIDE leverages principles of surface tension and patterned hydrophobicity to create a

70 m of phospholipids and proteins that reduces surface tension and prevents alveolar collapse during br

71 face cells simultaneously controlling tissue surface tension and radial tissue contraction.

72 rovides an internal tamponade effect through surface tension and swelling counter-forces.

73 cholesterol were investigated under varying surface tension and temperature.

74 aqueous solutions, including those with low surface tension and those containing bioanalytes.

75 residue serine 63 affects the ratio between surface tension and viscosity and cause sorting between

76 -standing paradox about magnitudes of tissue surface tensions and potentially explains discrepancies

77 ation modes based on the competition between surface tensions and reveal that dropwise condensation r

78 mechanisms by which the PS film attains low surface tensions and stabilizes the alveolar surface.

79 ([Formula: see text] stands for vapor-liquid surface tension, and [Formula: see text] stands for the

80 the 10% substitution level, with diminished surface tension, and a longer time was needed for both w

81 chanical properties such as viscoelasticity, surface tension, and adhesion.

82 lifted on a single drop of sterile water by surface tension, and deposited onto a spinal cord lesion

83 y, dynamic light scattering, zeta potential, surface tension, and FTIR spectroscopic characterization

84 odel that balances the hydrostatic pressure, surface tension, and optical pressure across the air-dro

85 BC, PM mass, surface tension, and water-soluble organic mass (WSOM) f

86 ing their relatively low boiling points, low surface tensions, and poor solvent properties.

87 veral physical properties, including solvent surface tension, anion viscosity B-coefficient, and anio

88 is method provides unprecedented lowering of surface tension ( approximately 500 mJ/m(2) to near zero

89 etting transitions of liquids with different surface tensions are demonstrated and the underlying phy

90 r partial wetting, of all aerosols for which surface tensions are provided in the literature, and pro

91 confirms the observed finite-size-dependent surface tension arises from the high surface-to-volume r

92 ons are presented for the calculation of the surface tension as a function of the temperature, pressu

93 D'Arcy Thompson emphasised the importance of surface tension as a potential driving force in establis

94 nt with the tail of an exponential growth in surface tension as temperature decreases.

95 process, a high-throughput technique called surface tension-assisted epitaxial lift-off was develope

96 nt-assisted, and that it originates from the surface tension associated with differences in the netwo

97 ments, betaine and glycine both increase the surface tension at the air-water interface.

98 Pulmonary surfactant lipoproteins lower the surface tension at the alveolar-airway interface of the

99 ctant is a lipid-protein complex that lowers surface tension at the respiratory air-liquid interface,

100 Using a 3D surface tension-based vertex model, we reproduce the cha

101 ambers, each having a volume of 25 pL, using surface-tension-based sample partitioning.

102 rystallization suppression is related to the surface tension between fluid and crystal.

103 ned surfactants to reduce the high intrinsic surface tension between the LCs and the fluorocarbon oil

104 Muller-Toporov model, adhesive vesicles with surface tension (Brochard-Wyart and de Gennes derivation

105 cal not only for their role in lowering lung surface tension but also in innate host defense.

106 operate below the thermal limit at ultra-low surface tensions but also yields structures that are sta

107 gger blastoderm expansion by reducing tissue surface tension, but also drive blastoderm thinning by i

108 supply of PLs is limited, SURF-TG may reduce surface tension by behaving as a secondary membrane comp

109 and the role of domains in the regulation of surface tension by lung surfactant.

110 nation of saline feed solutions with varying surface tensions by membrane distillation (MD).

111 les collected to measure Young's modulus and surface tension can also provide both qualitative and qu

112 idual sucrose particles, Young's modulus and surface tension can be quantified as a function of RH.

113 ties that are independent of polarity (e.g., surface tension) can be responsible for supercharging an

114 ole of physical factors such as differential surface tension, cell rearrangements, and tissue growth.

115 lifetime is the result of surfactant-induced surface tension changes.

116 esion to the substrate while providing a low surface tension coating at the air interface.

117 robe liquids suggested that TolC altered the surface tension components of E. coli cells and lead to

118 Surface-tension components, polarity, and coordination e

119 ndustrial wastewaters containing diverse low surface tension contaminants.

120 and can influence CCN activity by depressing surface tension, contributing solute, and influencing dr

121 tu Langmuir-Blodgett transfer, and real-time surface tension control using closed-loop axisymmetric d

122 The absolute surface tension curves and critical micelle concentratio

123 This critical review analyses most of the surface tension data reported between 2001 and 2010 (187

124 The monolayer minimum surface tension decreased in the presence of solid domai

125 We find that an increase in the surface tension decreases the temperature of the transit

126 formation, is interpreted as the solid-fluid surface tension, demonstrating that compliant thin-film

127 DL pronouncedly increased the A-W interface surface tension, demonstrating that lipids are the promi

128 It was found that changes in surface tension, density, viscosity (resulting from mixi

129 A compressed film model explains how surface tension depression by interfacial organic molecu

130 Recent empirical evidence suggests surface tension depression by organic aerosol to signifi

131 Accounting for surface tension depression can lower the calculated kapp

132 This work provides evidence for surface tension depression in an important aerosol syste

133 yde to the gas-aerosol interface, leading to surface tension depression of the aerosol.

134 ained (3 x 10(-5)-9 x 10(-3) M) implies that surface tension depression should be significant for all

135 9) provide evidence that asymmetric membrane surface tension determines the directionality of lipid d

136 The balance between elasticity and surface tension dictates the helical radius dimension.

137 The effects of surface tension, dipole moment, and dielectric constant

138 urface tension until activation, and (2) the surface tension does not follow the Szyszkowski equation

139 To reproduce this feat in a surface tension-dominant jumping robot, we elucidated th

140 ptures this behaviour and explains how solid surface tension dominates elasticity for small-scale ind

141 bilize nematic droplets with handles against surface tension-driven instabilities, using a yield-stre

142 -stabilizing mechanisms are the liquid-vapor surface tension-driven transport of vapor mass and the e

143 On a microscopic scale, one expects the surface-tension-driven flows produced during bubble rupt

144 We found that surface tension drives the collapse and initiates a dyna

145 wer healing kinetics, attributed to a weaker surface tension driving force.

146 ility to continuously manipulate various low-surface-tension droplets from free-sliding to pinned.

147 adius, indicating that both line tension and surface tension dropped, but the line tension decreased

148 Surface tension due to water adsorption within the aggre

149 However, changes in surface tension during the experiment can potentially in

150 device resolution of 55 um not restricted by surface tension effects.

151 nts are reconstituted and combined through a surface-tension-enabled mixing (STEM) mechanism.

152 g and bridging bonds in our model provides a surface tension ensuring the condensation of the ParB-DN

153 models assuming activating particles have a surface tension equal to that of water.

154 t, while maintaining substantial lowering of surface tension, even for partial surface coverage.

155 containing saline water as the feed with low surface tension, experiments reveal that the number of p

156 nes exhibited stable MD performance with low surface tension feed waters, demonstrating the potential

157 hobic substrate from being wetted by the low-surface-tension feed water.

158 properties, including spheroid shapes due to surface tension, fluidity due to deformations, and fast

159 al biophysical techniques (oxidative stress, surface tension, fluorescence spectroscopy and HPLC) wer

160 pillary number, Ca e , (ratio of electric to surface tension forces) up to Ca e approximately 1.0.

161 oplet interface, we can accurately determine surface tension from our measurements.

162 d an optical tensiometer that calculates the surface tension from the axisymmetric drop shape and the

163 facial systems and of the calculation of the surface tension from the underlying intermolecular poten

164 and low sliding angles for liquids that span surface tensions from 78.2 to 18.4 mN m(-1).

165 The surface tension (gamma) of xylem sap plays a key role in

166 ent-accessible surface area, with a positive surface tension (gamma) that is independent of the prope

167 n of hydrophobic peptides can create a large surface-tension gradient around the MOF that can efficie

168 n of the motors is induced by self-generated surface tension gradients along their bodies.

169 ring evaporation, and in the process creates surface tension gradients and significant density and vi

170 oplets are stabilized by evaporation-induced surface tension gradients and that they move in response

171 ors, whose motions are driven by anisotropic surface tension gradients created via peptide self-assem

172 to a certain destination through the use of surface tension gradients.

173 ent, to coupled interface-fluid motion under surface tension, gravity, and incompressible fluid dynam

174 ked change in overall surface properties for surface tensions >10 mN/m, indicative of a bimodal behav

175 omer using immiscible filtration assisted by surface tension (IFAST) immunoprecipitation.

176 hod called immiscible filtration assisted by surface tension (IFAST) to isolate proteins under define

177 Using immiscible filtration assisted by surface tension (IFAST), a technique developed for nucle

178 pplications, and also to measure the droplet surface tension, important for quantitative development

179 critically important for maintenance of low surface tension in airway fluids.

180 evelopment of surface stresses (analogous to surface tension in fluids) coordinates with bulk contrac

181 oviding hydrostatic back pressure to balance surface tension in order to form a electrolyte meniscus

182 learance in conducting airways, reduction of surface tension in the alveoli, and maintenance of near

183 ce of the line tension in the arc and of the surface tension in the cell bulk.

184 is suggested that healing is driven by high surface tension in the films and occurs through viscoela

185 In vivo, this surface tension increase may prime lipid droplets for re

186 Low viscosity and low surface tension induce a small daughter droplet encapsul

187 This instability is akin to the surface tension-induced breakup of a liquid jet but is d

188 Surface tension influences the fraction of atmospheric p

189 Surface tension information was then examined with Kohle

190 Surface-active properties including surface tension, interfacial tension, and contact angle

191 shapes of a rotating liquid droplet bound by surface tension is an archetypal problem in the study of

192 m can be determined here if the liquid-vapor surface tension is known independently.

193 Unlike liquids, for crystalline solids the surface tension is known to be different from the surfac

194 ility and a passive elastic component, while surface tension is largely due to active contractility.

195 ory (CNT) if the curvature dependence of the surface tension is taken into account.

196 e that the effect of gravity relative to the surface tension is weak, i.e. the Bond number (Bo) is sm

197 Surface stress, also known as surface tension, is a fundamental material property of a

198 tified and characterized via measurements of surface tension isotherms and critical micelle concentra

199 Surface tension isotherms indicate that mPMA surfactants

200 ations, but the evaporation of high- and low-surface-tension liquid droplets placed on such surfaces

201 At low surface tensions, liquid-ordered domains manifest sponta

202 obicity and showed wetting resistance to low surface tension liquids such as ethanol (22.1 mN m(-1)).

203 w durability, insufficient repellence of low surface tension liquids).

204 tting resistance of the membrane against low surface tension liquids.

205 ated by evaluating wetting resistance to low surface tension liquids.

206 lues ever reported - even with extremely low-surface-tension liquids such as n-heptane.

207 All samples showed surface tensions lower than sodium dodecyl sulfate, SDS

208 evidence illustrating that, in ambient air, surface tension lowering can prevail over the reduction

209 Surface tension lowering caused by organic surfactants,

210 Our work indicates that surface tension may play a key role in recruiting protei

211 d the SAM surface coverage fraction from the surface tension measured by other techniques.

212 Surface tension measurements and microscopic observation

213 combining X-ray photoelectron spectroscopy, surface tension measurements and thermodynamic modeling.

214 Surface tension measurements combined with a computation

215 eak (~980 cm(-1)) intensity measurements and surface tension measurements were conducted to investiga

216 e (288.15-318.15)K from the conductivity and surface tension measurements.

217 spindles are shaped by the interplay between surface tension, nematic elasticity, and motor-driven ac

218 nerally described as "substances that reduce surface tension", new evidence shows that ST may have li

219 All diastereomers exhibit a minimum surface tension of about 28 mN/m without a significant d

220 an important component of aerosol mass, the surface tension of activating aerosol particles is still

221 Based on the modified Kelvin equation, the surface tension of Ag NPs was found to be approximately

222 lm formation through its ability to modulate surface tension of airway fluids.

223 stingly, both CA and MC had no effect on the surface tension of BSA/air interfaces.

224 ing/freezing point temperature, density, and surface tension of confined water.

225 Surface tension of digesta correlated inversely (p<0.05)

226 hat surfactants can significantly reduce the surface tension of finite-sized droplets below the value

227 The surface tension of Lf tends to decrease with decrease in

228 In conjunction with the curvature-dependent surface tension of liquid droplets predicted from a theo

229 e graphene-covered substrates induced by the surface tension of liquid droplets together with the Neu

230 -FET), which was fabricated by utilizing the surface tension of liquid silver to suspend a CNT betwee

231 The surface tension of matrices, and the wettability and dif

232 ue to the relatively high volatility and low surface tension of most organic solvents.

233 several recent experiments indicate that the surface tension of supercooled water follows a smooth ex

234 actant lipids to form a film that lowers the surface tension of the air/water interface in the lungs.

235 To measure the surface tension of the drops we used an optical tensiome

236 The water-soluble organic carbon content and surface tension of the extracted filter samples were mea

237 nough to stand against gravity and the large surface tension of the liquid.

238 e device fabrication arising from the strong surface tension of the modified dielectric environment.

239 e balance between the internal viscosity and surface tension of the particle is thus disrupted, and t

240 action between the surface curvature and the surface tension of the PLGA.

241 e at pH 7 and 9 due to optimum viscosity and surface tension of the soluble complexes.

242 nd rate of drainage inversely related to the surface tension of the surfactant solution.

243 two chaparral fuels is shown to depress the surface tension of water by 30% or more at organic matte

244 We validated the method by measuring the surface tension of water in oil microdrops deposited on

245 In climate models, however, surface tension of water is generally assumed when predi

246 ilt angle of the body necessary to break the surface tension of water.

247 , and the meniscus profile set by the strong surface tension of water.

248 t angle can be accurately predicted from the surface tensions of each liquid with the vapor and betwe

249 our aromatic precursors, indicating that the surface tensions of the SOA coatings are similar.

250 only towards probing water but also for low-surface-tension 'oils'.

251 unctions, we explore the effects of a finite surface tension on phase equilibrium using a molecular t

252 ity of the network the smoothening effect of surface tension on the imbibition front roughening is ne

253 We exhibit the effect of surface tensions on the formations of nanoscale droplets

254 re ordered phase was induced by lowering the surface tension or temperature.

255 thelial remodeling, and alteration of airway surface tension predisposing to collapse.

256 This study examines the hygroscopic and surface tension properties as a function of photochemica

257 Significantly, this surface tension reduction is droplet size-dependent and

258 where mu and gamma are the viscosity and the surface tension, respectively.

259 e credit to a previous figure upon which the surface-tension scheme in Fig.1 should have included the

260 g.1 should have included the following: "The surface-tension scheme in Fig.1b is adapted from Fig.1a

261 The importance of surface tension, sigma (mN m(-1)), in these processes ha

262 dynamics simulations, we show that increased surface tension significantly impacts the dynamics of pr

263 also demonstrated that choice of a very low surface tension solvent is critical in successfully acti

264 bicarbonate, rather than a conventional low surface tension solvent.

265 predicted surface areas provided that lower surface tension solvents, such as n-hexane and perfluoro

266 Surface tension (ST) has been the most important measure

267 coefficient onto banana surfaces, and lower surface tension (ST, 25.4mN/m) than the critical ST (35.

268 As the curvature is gradually increased, the surface tension stretching the sheet over the drop cause

269 bic MD membranes are prone to wetting by low surface tension substances, thereby limiting their use i

270 ds from epithelial cells with lower apparent surface tension than for mesenchymal spheroids with high

271 ict regions of osmotic pressure and membrane-surface tension that produce successful engulfment.

272 Colour, surface tension, thermal properties, particle charge and

273 on, detachment rate of myosin, and effective surface tension, this motion can be either straight or c

274 o the alveolar air-water interface, lowering surface tension to avoid lung collapse at end-expiration

275 platform, suspended microfluidics, that uses surface tension to fill and maintain a fluid in microsca

276 showed strong surface activity that reduces surface tension to low values when concentrated as they

277 forms an interfacial monolayer reducing the surface tension to near zero values and thus preventing

278 cal model suggested that contraction reduces surface tension to permit the fusion of precursors into

279 actant is a lipoprotein complex that reduces surface tension to prevent alveolar collapse and contrib

280 nal voids to there being sufficient time for surface tension to round these objects before the hot (a

281 tmospheric particles to strongly depress the surface tension until activation, and (2) the surface te

282 presence of strong surfactants and evidenced surface tension values, sigma, below 40 mN m(-1), suspec

283 From these parameters, and from surface-tension values measured previously, we estimated

284 ace behavior and distinctive trends of their surface tension versus temperature.

285 has been shown to impact viscosity, density, surface tension, volatility, solubility, chemical reacti

286 allenge, a microfluidic viscometer driven by surface tension was developed to reduce the sample volum

287 g P values), pKa, and the inverse calculated surface tension was significantly lower although still p

288 on of these membranes in desalination of low surface tension wastewaters by membrane distillation (MD

289 A water droplet surface tension (WDST) based innovative method was devel

290 teristics of the tested starches, and pastes surface tension were determined.

291 rane properties: its bending modulus and its surface tension, which arises from the membrane's connec

292 ntribution of gravity, centrifugal force and surface tension, which can be accounted for using only t

293 ng droplet size or increases with decreasing surface tension, which is sensitive to surfactants.

294 apes this ability to optimally exploit water surface tension, which might have aided adaptive radiati

295 highly correlated manner due to an effective surface tension, which restricts front broadening.

296 roperties of the phases-particularly droplet surface tension-which arises from sequence-encoded featu

297 Raw exudates had a significantly lower surface tension while not increasing overall solubility,

298 Indeed, reducing surface tension with hyperosmolar media promoted microri

299 nsidering the variation of contact angle and surface tension with pore size improves the agreement be

300 The variation of liquid-vapor surface tension with solute concentration is a key facto