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1 ticle assembly would be determined solely by surface tension.
2 surfactant as well as its ability to reduce surface tension.
3 nt tetrahydrofuran (THF), because of its low surface tension.
4 use these measurements to estimate line and surface tension.
5 ne tension decreased to a lesser extent than surface tension.
6 ers compared to a flat monolayer at the same surface tension.
7 DeltaG(vdw) can be computed with a constant surface tension.
8 ors, especially for organic liquids with low surface tension.
9 the furrow line tension and the cell poles' surface tension.
10 control surface mechanics and determine cell surface tension.
11 creases lung compliance by reducing alveolar surface tension.
12 ion of the material to the template, and its surface tension.
13 linking intercellular adhesion and localised surface tension.
14 ed to the aqueous environment, increasing LD surface tension.
15 TMAO, however, reduces the surface tension.
16 ke diffusivity, low viscosity, and near-zero surface tension.
17 , overcoming frictional forces, and reducing surface tension.
18 ic orifice as it deforms under the action of surface tension.
19 n ion hydration energy and the neat liquid's surface tension.
20 in vitro studies of cell sorting and tissue surface tension.
21 y length, and the line tension under varying surface tension.
22 is comparable to the work done by the excess surface tension.
23 hesion to cortical tension determines tissue surface tension.
24 urface area compression to reach low minimum surface tension.
25 he availability of a surfactant that reduces surface tension.
26 sure of the ratio of van der Waals forces to surface tension.
27 tain surface-active molecules that can lower surface tension.
28 boly, possibly through maintenance of tissue-surface tension.
29 macroscopic particles are considered to lack surface tension.
30 n liquid microchannel flow is constrained by surface tension.
31 occur through cell movement driven by tissue surface tension.
32 energy of the LD, as opposed to the bilayer surface tension.
33 idal droplets are inherently unstable due to surface tension.
34 ls is many times larger than the zero-strain surface tension.
35 bit sliding angles that decrease with liquid surface tension.
36 zable results and used to explain changes in surface tension.
37 fluids with different density, viscosity and surface tension.
38 dome indicative of an isotropic and uniform surface tension.
39 exhibit a long-ranged attraction mediated by surface tension.
40 ater breaks apart into droplets to lower its surface tension.
41 droplet, with a contact angle determined by surface tensions.
42 film structures can be used to measure solid surface tensions.
43 d tissues and quantify their viscosities and surface tensions.
44 lm compressibility and lower maximum dynamic surface tensions.
45 ility of cell interfaces may underlie tissue surface tensions.
46 chemical properties, such as viscosities and surface tensions.
47 nonpolar liquids possessing a wide range of surface tensions.
48 teristics: a surfactant property that lowers surface tension, a cell/spore antiaggregant, and an adhe
49 forming direct measurements of the effective surface tension, a measure of relative tissue cohesivity
50 of the bending modulus of the bilayer to its surface tension, a size which is ~100 nm for the plasma
51 es not correlate with the maximum or minimum surface tension achieved with or without serum in the su
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 ods require high PFCA concentrations in both surface tension and (19)F NMR experiments; in contrast,
56 h fatty acid membranes, inducing a change in surface tension and causing pearling and subsequent divi
57 impacts of pore size and temperature on the surface tension and contact angle of water/vapor and oil
58 nate and ethylene carbonate, which have high surface tension and dipole moment values, can be used to
59 odic assembly is governed by the anisotropic surface tension and elasticity at the interface of beads
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
70 unusual discrepancy between the CMC based on surface tension and on the two "bulk" methods was attrib
72 m of phospholipids and proteins that reduces surface tension and prevents alveolar collapse during br
76 e liquid film under the competing effects of surface tension and van der Waals forces is studied as a
77 us bacteria, the film appeared to manipulate surface tension and, as such, acted like a surfactant.
78 -standing paradox about magnitudes of tissue surface tensions and potentially explains discrepancies
79 ation modes based on the competition between surface tensions and reveal that dropwise condensation r
80 ([Formula: see text] stands for vapor-liquid surface tension, and [Formula: see text] stands for the
81 the 10% substitution level, with diminished surface tension, and a longer time was needed for both w
83 lifted on a single drop of sterile water by surface tension, and deposited onto a spinal cord lesion
87 veral physical properties, including solvent surface tension, anion viscosity B-coefficient, and anio
89 is method provides unprecedented lowering of surface tension ( approximately 500 mJ/m(2) to near zero
90 ude thicker, however, does not reach the low surface tensions ( approximately 0.001 N/m) achieved in
91 etting transitions of liquids with different surface tensions are demonstrated and the underlying phy
92 r partial wetting, of all aerosols for which surface tensions are provided in the literature, and pro
93 ons are presented for the calculation of the surface tension as a function of the temperature, pressu
94 D'Arcy Thompson emphasised the importance of surface tension as a potential driving force in establis
96 ibbs equation to the steep linear decline in surface tension as the bulk concentration increases.
97 process, a high-throughput technique called surface tension-assisted epitaxial lift-off was develope
98 nt-assisted, and that it originates from the surface tension associated with differences in the netwo
99 tant phospholipids are essential in reducing surface tension at the air-liquid interface and preventi
101 Pulmonary surfactant lipoproteins lower the surface tension at the alveolar-airway interface of the
102 h the channel due to the large difference in surface tension at the interface of the hydrophilic chan
103 ctant is a lipid-protein complex that lowers surface tension at the respiratory air-liquid interface,
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 the surfactant film, rather than decreasing surface tension by increasing its surface density, becom
110 regated interfacial surfactant phases at low surface tensions by inducing 3D structural transitions i
112 les collected to measure Young's modulus and surface tension can also provide both qualitative and qu
113 idual sucrose particles, Young's modulus and surface tension can be quantified as a function of RH.
114 ties that are independent of polarity (e.g., surface tension) can be responsible for supercharging an
116 bble walls move under the influence of their surface tension (capillarity), with a velocity proportio
119 robe liquids suggested that TolC altered the surface tension components of E. coli cells and lead to
123 and can influence CCN activity by depressing surface tension, contributing solute, and influencing dr
125 This critical review analyses most of the surface tension data reported between 2001 and 2010 (187
129 formation, is interpreted as the solid-fluid surface tension, demonstrating that compliant thin-film
136 urface tension until activation, and (2) the surface tension does not follow the Szyszkowski equation
138 ptures this behaviour and explains how solid surface tension dominates elasticity for small-scale ind
139 bilize nematic droplets with handles against surface tension-driven instabilities, using a yield-stre
140 On a microscopic scale, one expects the surface-tension-driven flows produced during bubble rupt
141 characteristic droplet patterns owing to the surface-tension-driven Plateau-Rayleigh instability.
143 ility to continuously manipulate various low-surface-tension droplets from free-sliding to pinned.
144 adius, indicating that both line tension and surface tension dropped, but the line tension decreased
148 as derived to take both charge screening and surface tension effects into account at the protein/wate
151 g and bridging bonds in our model provides a surface tension ensuring the condensation of the ParB-DN
153 t, while maintaining substantial lowering of surface tension, even for partial surface coverage.
154 nes exhibited stable MD performance with low surface tension feed waters, demonstrating the potential
155 that we measure correspond to an equivalent surface tension five orders of magnitude below that of o
157 pillary number, Ca e , (ratio of electric to surface tension forces) up to Ca e approximately 1.0.
159 d an optical tensiometer that calculates the surface tension from the axisymmetric drop shape and the
160 facial systems and of the calculation of the surface tension from the underlying intermolecular poten
163 ent-accessible surface area, with a positive surface tension (gamma) that is independent of the prope
164 on model, DeltaG = gamma(T)DeltaA, where the surface tension, gamma, is lengthscale-dependent and dec
166 nanostructured composite, creating a thermal surface tension gradient and, subsequently, motion.
167 n of hydrophobic peptides can create a large surface-tension gradient around the MOF that can efficie
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
174 ent, to coupled interface-fluid motion under surface tension, gravity, and incompressible fluid dynam
175 ked change in overall surface properties for surface tensions >10 mN/m, indicative of a bimodal behav
176 ties of the wetting solutions, including the surface tension (>40 mM/m), salt concentration (>10 mM),
178 hod called immiscible filtration assisted by surface tension (IFAST) to isolate proteins under define
179 Using immiscible filtration assisted by surface tension (IFAST), a technique developed for nucle
180 pplications, and also to measure the droplet surface tension, important for quantitative development
182 tion, from which we extract a liquid-crystal surface tension in excellent agreement with experiments.
183 learance in conducting airways, reduction of surface tension in the alveoli, and maintenance of near
189 is suggested that healing is driven by high surface tension in the films and occurs through viscoela
190 to wetting from a number of liquids with low surface tension, including alkanes such as decane and oc
192 uch feeding mechanism in shorebirds involves surface tension-induced transport of prey in millimetric
194 shapes of a rotating liquid droplet bound by surface tension is an archetypal problem in the study of
196 Unlike liquids, for crystalline solids the surface tension is known to be different from the surfac
197 ility and a passive elastic component, while surface tension is largely due to active contractility.
201 ations, but the evaporation of high- and low-surface-tension liquid droplets placed on such surfaces
203 obicity and showed wetting resistance to low surface tension liquids such as ethanol (22.1 mN m(-1)).
204 id-liquid-air interfaces, even with very low surface tension liquids such as pentane (gamma(lv) = 15.
210 evidence illustrating that, in ambient air, surface tension lowering can prevail over the reduction
215 combining X-ray photoelectron spectroscopy, surface tension measurements and thermodynamic modeling.
219 dration contribution can be described by the surface tension model, DeltaG = gamma(T)DeltaA, where th
220 nerally described as "substances that reduce surface tension", new evidence shows that ST may have li
222 Based on the modified Kelvin equation, the surface tension of Ag NPs was found to be approximately
226 ncreasing temperature by 5%, the same as the surface tension of dodecane/water, in agreement again wi
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
232 several recent experiments indicate that the surface tension of supercooled water follows a smooth ex
233 actant lipids to form a film that lowers the surface tension of the air/water interface in the lungs.
235 The water-soluble organic carbon content and surface tension of the extracted filter samples were mea
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
241 system, including the volume, viscosity, and surface tension of the sample solution and the tilt of t
243 onies on nutrient substrates by lowering the surface tension of the surrounding fluid, and to aid in
244 two chaparral fuels is shown to depress the surface tension of water by 30% or more at organic matte
245 We validated the method by measuring the surface tension of water in oil microdrops deposited on
247 t angle can be accurately predicted from the surface tensions of each liquid with the vapor and betwe
250 unctions, we explore the effects of a finite surface tension on phase equilibrium using a molecular t
251 ity of the network the smoothening effect of surface tension on the imbibition front roughening is ne
252 explicit model for the dependence of tissue surface tension on these mesoscopic parameters has been
257 This study examines the hygroscopic and surface tension properties as a function of photochemica
258 information about PFCA-albumin interactions, surface tension provides only qualitative information.
260 e credit to a previous figure upon which the surface-tension scheme in Fig.1 should have included the
261 g.1 should have included the following: "The surface-tension scheme in Fig.1b is adapted from Fig.1a
262 putation of time-periodic vortex sheets with surface tension separating two immiscible, irrotational,
263 dynamics simulations, we show that increased surface tension significantly impacts the dynamics of pr
264 also demonstrated that choice of a very low surface tension solvent is critical in successfully acti
265 predicted surface areas provided that lower surface tension solvents, such as n-hexane and perfluoro
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 r alcohols, that possess significantly lower surface tension than water (gamma(lv) = 72.1 mN/m).
271 ith organic liquids having appreciably lower surface tensions than that of water-are extremely rare.
272 ict regions of osmotic pressure and membrane-surface tension that produce successful engulfment.
275 xamined using three experimental approaches: surface tension titrations, (19)F NMR spectroscopy, and
276 o the alveolar air-water interface, lowering surface tension to avoid lung collapse at end-expiration
277 platform, suspended microfluidics, that uses surface tension to fill and maintain a fluid in microsca
278 showed strong surface activity that reduces surface tension to low values when concentrated as they
279 forms an interfacial monolayer reducing the surface tension to near zero values and thus preventing
280 actant is a lipoprotein complex that reduces surface tension to prevent alveolar collapse and contrib
281 essentially equivalent to applying an excess surface tension to the membrane, causing channel expansi
283 tmospheric particles to strongly depress the surface tension until activation, and (2) the surface te
284 presence of strong surfactants and evidenced surface tension values, sigma, below 40 mN m(-1), suspec
288 allenge, a microfluidic viscometer driven by surface tension was developed to reduce the sample volum
289 g P values), pKa, and the inverse calculated surface tension was significantly lower although still p
290 on of these membranes in desalination of low surface tension wastewaters by membrane distillation (MD
291 pathway and crystallization control over the surface tension, which are advantageous for beta-Ga2O3 c
292 have as liquids and possess a characteristic surface tension, which arises as a collective, macroscop
293 ntribution of gravity, centrifugal force and surface tension, which can be accounted for using only t
294 ng droplet size or increases with decreasing surface tension, which is sensitive to surfactants.
296 roperties of the phases-particularly droplet surface tension-which arises from sequence-encoded featu
298 n ion abundance and a concurrent decrease in surface tension with an increase in the applied potentia
299 nsidering the variation of contact angle and surface tension with pore size improves the agreement be
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