ライフサイエンスコーパス: bubble

1 n opposite directions within the replication bubble.

2 ds to the non-damaged strand within a repair bubble.

3 to spontaneous DNA unwinding to form a seed-bubble.

4 face interfacial characteristics of a single bubble.

5 o the flow observed in a droplet without the bubble.

6 non-template strand within the transcription bubble.

7 , resulting in the formation of a cavitation bubble.

8 upstream of RNAPII and in the transcription bubble.

9 es and scrunching of the transcriptional DNA bubble.

10 the non-template strand in the transcription bubble.

11 ing by stabilizing the minimal transcription bubble.

12 pansion and contraction of the transcription bubble.

13 m diameter), and reached 100% for the larger bubbles.

14 can lead to net migration of these embryonic bubbles.

15 h bubble dissolution is arrested for armored bubbles.

16 ted to the formation and collapse of gaseous bubbles.

17 % of the total emissions were due to methane bubbles.

18 ally flat substrate lead to the formation of bubbles.

19 found to reach tens of MPa inside submicron bubbles.

20 sult of viscosity or perturbations caused by bubbles.

21 urrounding oil matrix forming tiny spherical bubbles.

22 erface or within the liquid film between the bubbles.

23 er-coated vesicles/liposomes, and gas-filled bubbles.

24 ssure on the microscopic details of graphene bubbles.

25 astic modulus determination with oscillating bubbles.

26 viscous aqueous and organic samples without bubbling.

27 is exceptionally prone to radiation-induced bubbling.

28 ption with pulsed focused ultrasound-induced bubble activity significantly increases the plasma abund

29 The stability of the bubble allows us to measure the contact-angle and perfor

30 n bubble core moment applies pressure to the bubble and gradually compresses it to a diameter of appr

31 e the DNA is melted out into a transcription bubble and the single-stranded template DNA is delivered

32 machinery is required for formation of these bubbles and acts to sustain survival of the cell when ML

33 carbons and also influence the buoyancies of bubbles and droplets.

34 y cells can be impacted thermally by the hot bubbles and mechanically by fluid mechanical forces to t

35 We study the effect of gravity on giant soap bubbles and show that it becomes dominant above the crit

36 es larger surface contact between cavitation bubbles and solids.

37 coiling, including the existence of multiple bubbles and that RPA molecules are mis-registered on the

38 ic perfluorocarbon chain stretching into air bubbles and the polar head in water.

39 he interfacial volume surrounding cavitation bubbles and using the Arrhenius equation, an effective m

40 an open state (engaged with a transcription bubble), and an initially transcribing complex (containi

41 ) containing a single-stranded transcription bubble, and selects a template-strand nucleotide to serv

42 uoyant jet of petroleum liquid droplets, gas bubbles, and entrained seawater, using 279 simulated che

43 ransport capability, easy release oxygen gas bubbles, and strong structural stability, which are adva

44 tal that is disrupted by the shear forces of bubbling, and we observed liquid-crystal phase transitio

45 containing a single-stranded 'transcription bubble,' and selects a transcription start site (TSS).

46 quids (aqueous assay solution, oil), the gas bubbles are clearly visible from the top, when the assay

47 The released gas bubbles are documented by recording videos of the assay

48 In this step, many bubbles are instantly formed in the sample matrix.

49 find that in the early stages of cavitation, bubbles are irregularly shaped and become more spherical

50 , jet drops formed from the base of bursting bubbles are postulated to mainly produce larger supermic

51 These bubbles are subject to dissolution as they rise, and dis

52 ach to develop nanosized oxygen encapsulated bubbles as an ultrasound contrast agent for methylation

53 al-masking reagent, and buoyant silica micro-bubbles as the capture antibody carriers.

54 al software to obtain diameters of every gas bubble at each time point.

55 e formation of a thin liquid film around the bubble at higher Ca.

56 In contrast, faster bubbles at capillary numbers Ca > 10(-3), have lower det

57 The dissolution of CO2 bubbles at different pH levels and salinities was studie

58 Bubbles at very low velocities, corresponding to capilla

59 uL of 1-octanol containing of 0.5 muL of air bubble, at 40 degrees C for extraction for 20 min), the

60 in degassed water shows a completely wetted bubble base with the microlayer, and the bubble does not

61 d and polymer-stabilized perfluorocarbon gas bubbles before and after their destruction with high int

62 ormation among individuals cause speculative bubbles, behavioral cascades, and other correlated actio

63 ciency (ADA-SCID), often referred to as the "bubble boy" disease.

64 is known that bioaerosols are generated when bubbles break on the surface of water containing microbe

65 rands (SNS-seq); (ii) sequencing replication bubbles (bubble-seq) and (iii) sequencing Okazaki fragme

66 as aerosol generated from freshwater through bubble bursting, analogous to SSA from seawater.

67 boratory measurements of microbes ejected by bubble bursting, further supporting the assignment of Bi

68 Once the bubble bursts, however, the total evaporation time decre

69 gnificant increase in the dissolution of CO2 bubbles, but increasing from 30 to 50 mg L(-1) displayed

70 simulated petroleum liquid droplets and gas bubbles by 3.2-fold and 3.4-fold, respectively, which in

71 The skyrmion bubbles can be nucleated by the application of an extern

72 Bubbles can occur in the body as a result of therapeutic

73 formed by film drops produced from bursting bubble-cap films, which become enriched with hydrophobic

74 RPA, which is observed as clear steps in the bubble-closing traces.

75 [Formula: see text] 100 [Formula: see text]m bubbles coated with [Formula: see text] 1 [Formula: see

76 onic water hammer created by an asymmetrical bubble collapse may break the hyaluronan.

77 echanical loading, in the form of cavitation bubble collapse, on damage to the brain's perineuronal n

78 ilitate DNA bending and impede transcription bubble collapse.

79 Here we examined, the potential of a bubble column (BCR) and an internal loop airlift (ALR) b

80 conversion at 1065 degrees C in a 1.1-meter bubble column and produced pure hydrogen without CO2 or

81 The bubbles contain the sulfur-bearing vapour injected into

82 nscription bubble expansion or transcription bubble contraction (scrunching or antiscrunching).

83 Metered air bubbles controlled by microvalves are used to improve be

84 at opposes the magnetisation of the skyrmion bubble core moment applies pressure to the bubble and gr

85 the nontemplate strand of the transcription bubble ("core recognition element," CRE).

86 These encapsulated bubbles could therefore be used for noninvasive ultrasou

87 In this case, cavitation refers to the bubble created by pressure drop.

88 contribute to poor visual outcomes after big-bubble DALK in keratoconus.

89 onsecutive corneal donor grafts used for big-bubble DALK surgery between June 2011 and December 2014

90 This cavitation bubble damages the plasma membranes of cells it contacts

91 Bubble data was used to verify the performance of a wide

92 a clinical lung surfactant monolayer-covered bubble decreases to approximately 100 microm, the monola

93 at replication forks or within transcription bubbles depending on the physiological state of the cell

94 gments we reveal here in the body patch with Bubbles differ from those suggested in previous studies

95 and the model was then used to estimate that bubble dissolution accounts for approximately 10% of met

96 ble, we find a range of pressures over which bubble dissolution is arrested for armored bubbles.

97 d to verify the performance of a widely used bubble dissolution model, and the model was then used to

98 We first show experimentally that large soap bubbles do not retain a spherical shape but flatten when

99 ted bubble base with the microlayer, and the bubble does not depart from the surface due to reduced l

100 , we describe optical properties of bistable bubble domain (BD) texture torons in a thin layer of cho

101 art a mixed Neel-Bloch-like character to the bubble domain walls.

102 The bubble domains appear in ultrathin epitaxial PbZr0.2 Ti0

103 The existence of the bubble domains is revealed by high-resolution piezorespo

104 PFM hysteresis loops for the bubble domains reveal that they undergo an irreversible

105 nanoscale ferroelectric domains, termed as "bubble domains"-laterally confined spheroids of sub-10 n

106 as a smooth transition from single stripe to bubble domains, which opens the door to future applicati

107 astic parameters that allow the existence of bubble domains.

108 amics and quantify the effectiveness of this bubble-driven detachment process for the bacterial strai

109 des direct evidence of O2 formation in these bubbles due to the incorporation of H2O into BSCF.

110 , and then used in studying the pool boiling bubble dynamics of a single bubble from nucleation to de

111 Comparison of the observed bubble dynamics to the predictions of the macroscopic Ra

112 ous configurations were fabricated and their bubble dynamics were examined at elevated heat flux, rev

113 derstanding and developing models of in vivo bubble dynamics.

114 The bubble ebullition cycle, which occurs over millisecond t

115 The resulting DPPS has the shape of a bubble, elongated asymmetrically along the rostro-caudal

116 estigate the structure and dynamics of vapor bubbles emerging from metastable water at negative press

117 8 degrees C) or atmospheric conditions up to bubble-end point, maintaining a thermal driving force of

118 By coupling bubbling-enhanced ventilation to a coastal ecosystem met

119 ng to an efficient removal of evolved oxygen bubbles even at high current densities of up to 250 mA/c

120 TSS selection, which involves transcription bubble expansion or transcription bubble contraction (sc

121 or more precisely how much volume around the bubble experiences these large energy dissipation rates.

122 esults also showed that the mass flux due to bubble-facilitated transport was intermittent, and incre

123 Results showed that the VOC mass flux due to bubble-facilitated transport was orders-of-magnitude hig

124 s were conducted to measure mass flux due to bubble-facilitated VOC transport from light nonaqueous p

125 r enrichment in fine SSA likely derives from bubble films.

126 Only reporters captured on micro-bubbles float above the dye and become visible in an ana

127 n-dominated conditions can be created by gas bubble flow in the saturated zone.

128 erstand the atomistic processes that lead to bubble formation and subsequent microstructural changes.

129 Nevertheless, the free energy of bubble formation can be perfectly reproduced in the fram

130 ollowed by rapid decompression may cause gas bubble formation within the blood stream (embolism) and

131 looping flow, no electrode corrosion, and no bubble formation), but also achieves a wider sustainable

132 e DNA distortions required for transcription bubble formation, and how the activator interacts with R

133 tificial systems almost invariably result in bubble formation, except under highly controlled conditi

134 barrier against strand unpeeling and melting-bubble formation.

135 c force microscopy, we analysed a variety of bubbles formed by monolayers of graphene, boron nitride

136 stigates the interactions that occur between bubbles formed during decompression and cells in a 3D en

137 in the warm interfacial region of cavitation bubbles formed from US.

138 nificantly increase (p = 0.0116) following a bubble-forming decompression.

139 the pool boiling bubble dynamics of a single bubble from nucleation to departure.

140 adaptation of cryo-EM based on detecting gas bubbles generated by radiation damage was used to locali

141 he mechanism of evaporation involves surface bubbles growing/coalescing to form a subcritical gap-spa

142 Consequent bubble growth depends not only on DO concentration but a

143 t the microstructure of tungsten, leading to bubble growth, blistering, and/or to the formation of fu

144 which serve as the nuclei for larger helium bubble growth, over timescales reaching into the millise

145 liquid droplets by surface attachment to gas bubbles has been suggested as a mechanism to overcome th

146 The i.v. injection of oxygen bubbles has recently emerged as a potential strategy to

147 le size, on a volume-to-volume basis smaller bubbles have a more significant impact.

148 The early growth stage of vapor bubble in degassed water shows a completely wetted bubbl

149 n of the downstream end of the transcription bubble in RPo, and thereby modulate TSS selection, which

150 In the presence of the bubble in the droplet, the observed flow toward the cent

151 We find that HARP closes RPA-stabilized bubbles in a slow reaction, taking on the order of tens

152 The results are not restricted to bubbles in bioreactors and may be relevant to a variety

153 We have imaged Neel skyrmion bubbles in perpendicularly magnetised polycrystalline mu

154 The self-organisation of void and gas bubbles in solids into superlattices is an intriguing na

155 allows the initiation and spread of embolism bubbles in the leaf network to be visualized.

156 shift and transiently deposit 20-30mum large bubbles in the microvasculature, occluding blood flow fo

157 While approach curves to Ar bubbles in the presence of a surfactant were promising f

158 The presence of large gas bubbles in the samples with oxidizing agents may have ca

159 atial and temporal propagation of embolizing bubbles in the stem xylem during imposed water stress.

160 saltic fragments found on the inner walls of bubbles in trachytic pumices, we show that the more mafi

161 Results demonstrated deposition of activated bubbles in tumor vasculature.

162 y to halt dissolution of particle-coated air bubbles in water based on interfacial rheology design is

163 motion of individual submillimeter acoustic bubbles in water in the presence of a high frequency (50

164 Pneumatic dissection created a "big bubble" in 67 of 80 eyes (83.7%), all of them but 1 (1.5

165 t the presence of large voids (solvent vapor bubbles) in cages dissolved in nitromethane.

166 A fully automated headspace bubble-in-drop microextraction (automated HS-BID) method

167 ver, the area of fringe patterns beneath the bubble increases with time.

168 ted electron bunch through the hosing of the bubble induced by the carrier envelope phase (CEP) effec

169 elicited in single HeLa cells by the tandem bubble-induced jetting flow in a microfluidic system.

170 Understanding cell-bubble interactions is crucial for preventing bubble rel

171 r preferential adsorption at the air-liquid (bubble) interface or within the liquid film between the

172 The static contact angle is increased when a bubble is applied.

173 osition on a glass substrate in which an air bubble is entrapped.

174 When the bubble is present, the evaporation process is retarded.

175 at the upstream portion of the transcription bubble is required for efficient NPH I-mediated transcri

176 s, demonstrates that the growth of nanoscale bubbles is governed by viscous forces.

177 mulsification mechanism of PFOS based on air bubbles is proposed, and PFOS partitions to the interfac

178 Furthermore, no bubble lattice alignment was observed in the <111> direc

179 sion electron microscopy of the formation of bubble lattices under He ion bombardment.

180 We have investigated the roles of cavitation bubble location, shockwave intensity and the size of a c

181 the flow of multi-phase (melt, crystals and bubbles) magmas is of great importance for interpreting

182 cluding power-law rheology and non-diffusive bubble motion and avalanches, stems directly from the fr

183 h interest in generating nanoscale echogenic bubbles (nanobubbles), which can enable new uses of ultr

184 ction at depth triggered rapid heterogeneous bubble nucleation and growth and could have enhanced eru

185 Bubble nucleation control, growth and departure dynamics

186 theory, conditions in the xylem should favor bubble nucleation even more: there are millions of condu

187 These results show that bubble nucleation is dominated by DO concentration (affe

188 surface structure that is capable of tuning bubble nucleation, growth and departure dynamics.

189 cant (p = 0.0024) corresponding reduction in bubble nucleation.

190 Bubbling O2 into a THF solution of Co(II)(BDPP) (1) at -

191 ts showed that an increased shrinkage of CO2 bubbles occurred with higher basicity, while an increase

192 to single-stranded DNA in the transcription bubble of the OC and increases its stability.

193 the DNA in the single-stranded transcription bubble of the rrnB P1 promoter complex expands and is "s

194 The accumulation of low-density bubbles of MVP in crystal-poor magmas has implications f

195 of fifty opto-thermocapillary flow-addressed bubble (OFB) microrobots in parallel is demonstrated.

196 ) were located outside the limits of the gas bubble on the first or third day postoperatively.

197 kwave intensity and the size of a cavitation bubble on the structural evolution of PNN.

198 Here, we study the impact of such vapor bubbles on human endothelial cells in terms of cell pora

199 C capsids generate two classes of bubbles: one occupies positions beneath the vertices of

200 Whereas a bare bubble only has a single pressure at which a given radiu

201 rfaces consisted of either a submerged argon bubble or a thin polydimethylsiloxane (PDMS) layer.

202 ization shows no sign of crystallization, He bubble or void formation, or segregation in all irradiat

203 ls would be damaged by a particular bursting bubble, or more precisely how much volume around the bub

204 overheating in the very near vicinity of the bubbles, overall increasing the average heating rate in

205 system can be achieved by simply tuning the bubbling parameters.

206 A subpopulation of C capsids bubbles particularly profusely and may represent particl

207 s of the geometry are less influenced by the bubble passage compared to the central region.

208 Moving air-liquid interfaces, for example, bubbles, play a significant role in the detachment and t

209 del, we demonstrate that strategically timed bubble plumes can mitigate exposure to high CO2 under pr

210 COD, reduced foam formation due to less gas bubble production, minimum scale formation, and lower ch

211 the procapsid and B capsid, is exceptionally bubbling-prone.

212 sent an optimized NMR device based on a mini bubble-pump associated with fluidics and microdetection

213 -template strand also disrupts transcription bubble reannealing.

214 ubble interactions is crucial for preventing bubble related pathologies and harnessing their potentia

215 On removing the field the skyrmion bubble returns to its original diameter via a hysteretic

216 Bubbles revealed the whole body in only a few neurons.

217 ved in matter at ambient conditions-from air bubbles (rho approximately 0) to osmium and iridium (rho

218 Consequent "bubble riding" by sulfide droplets, followed by degassin

219 rior stroma; (4) removal of the deep stroma (bubble roof) from a central 6-mm optical zone; and (5) t

220 S-seq); (ii) sequencing replication bubbles (bubble-seq) and (iii) sequencing Okazaki fragments (OK-s

221 han do sites identified by either SNS-seq or bubble-seq.

222 dentified by SNS-seq, followed by OK-seq and bubble-seq.

223 an exact analogy, it is shown how the giant bubble shapes can be realized by large inflatable struct

224 s no mechanical limit of the height of giant bubble shapes.

225 lic pathways in some plants, as residual gas bubbles should expand when vessels are reconnected to th

226 non-template strand within the transcription bubble showed that the upstream portion of the transcrip

227 ligonucleotide, and a complete transcription bubble (sigma(S)-TIC) at about 3.9-A resolution.

228 itions, it has been possible to engineer the bubble size and spacing of the superlattice leading to i

229 was investigated by monitoring change in CO2 bubble size at various Ni NPs concentrations.

230 Current understanding of natural methane bubble size distributions is limited by the difficulty i

231 There was no change in bubble size distributions over the 3 month sampling peri

232 Bubble size distributions were spatially heterogeneous e

233 Our custom optical bubble size sensors recorded bubble sizes and release ti

234 s over the 3 month sampling period, but mean bubble size was positively correlated with daily ebullit

235 me exceeding a particular EDR increases with bubble size, on a volume-to-volume basis smaller bubbles

236 dissolution rates are strongly influenced by bubble size.

237 ment conditions are important to controlling bubble size.

238 custom optical bubble size sensors recorded bubble sizes and release timing at 8 locations in Upper

239 ns is limited by the difficulty in measuring bubble sizes over wide spatial or temporal scales.

240 ing predictions for a variety of liquids and bubble sizes.

241 rates the key role of TFIIB in transcription bubble stabilization and provides strong structural supp

242 The foam ink contains bubbles stabilized by attractive colloidal particles sus

243 rane deformation, as determined by different bubble standoff distances.

244 ess this deficit of solutions by introducing bubble stripping as a novel geochemical engineering appr

245 We argue that shallow water CO2 bubble stripping should be considered among the growing

246 ermination of some important features of RPA-bubble structures at low supercoiling, including the exi

247 -A2, or both SP-A1 and SP-A2, in the captive bubble surfactometer.

248 ind that air/sea gas exchange rates within a bubbled system are 1-2 orders of magnitude higher than w

249 A continuous and scalable bubbling system to generate functional nanodroplets disp

250 s, the dissociation rate of PS in cavitating bubble systems was determined to be 3 orders of magnitud

251 to an equation of translational motion of a bubble taking the form of Mathieu's equation.

252 keratoconus who underwent DALK using the big-bubble technique.

253 Here we applied the Bubbles technique to the responses of single macaque mid

254 We also show that mismatch bubble templates could circumvent the requirement of TFB

255 Bubbles, tens of micrometres in size, formed inside the

256 Here, we create a steady-state vapor bubble that can remain stable for hours in a pool of sub

257 These diving flies are protected by an air bubble that forms around their superhydrophobic cuticle

258 We also show that bubbles that form chains along the direction of the acou

259 Bubbles that rise to the surface of a cell suspension ca

260 nrichments in SSML were attributed to rising bubbles that scavenge surface-active species from seawat

261 probability was already 40% for the smallest bubbles that were formed (<7.5 mum diameter), and reache

262 ive pressure without constantly creating gas bubbles that would disable their hydraulic systems.

263 ates (EDR) and have predicted that for small bubbles the EDR could exceed values that would kill many

264 nd suggests that for even smaller, sub-10 nm bubbles the pressure can be close to 1 GPa and may modif

265 with 50 ppb NO in a 0.5 L min(-1) air stream bubbling through a solution of 1.2 M H2O2 and 0.5 M NaOH

266 hanging from classic nucleation into gaseous bubbles to a facilitated removal through escaping gases/

267 ctors require continuous injection of oxygen bubbles to maintain cell growth.

268 energy needed to deform it, allowing to use bubbles to study elastic properties of 2D crystals and c

269 at transfer of momentum and/or heat from the bubbles to the cells are the dominant mechanisms of ener

270 believed to be required for such an "armored bubble" to resist dissolution, in fact engineering a 2D

271 ely 42%) may reach the atmosphere via direct bubble transport (0-2 kt yr(-1)) and via diffusive excha

272 on to potentially releasing sediment methane bubbles twice a day by entering and leaving the sediment

273 In general, at higher bubble velocities bacterial cells in the corners of the

274 Depending on the bubble velocity U, at least three different flow regimes

275 l increasing the average heating rate in the bubble vicinity vis-a-vis the bulk of the liquid.

276 The wall of the type 1 big bubble was excised and its grade of scrolling noted.

277 or sclerocorneal discs in which a type 1 big bubble was obtained by stromal injection of air were stu

278 erence in growth rate or maximum size of the bubbles was measured (p = 0.99 and 0.23).

279 asicity, while an increased expansion of CO2 bubbles was observed with a proportional increase in sal

280 The presence of bubbles was previously proposed in an attempt to account

281 -butyl alcohol and nitrobenzene verified the bubble-water interface as the location for PS activation

282 n effective mean temperature of 340 K at the bubble-water interface was estimated.

283 Importantly, "big" air bubbles were often located in close vicinity of a crack

284 Bubbles were removed from intervessel pits first, follow

285 BIR proceeds by a migrating bubble where asynchrony between leading and lagging stra

286 to the formation of frequent embolisms (gas bubbles), which could be removed by the occurrence of ro

287 primary wound via a laser-induced cavitation bubble, which forms and collapses within microseconds of

288 The hexadecane-loaded capsules also produced bubbles while their shell remained intact.

289 ap foam consisting of compressible spherical bubbles, whose sizes slowly evolve and whose collective

290 undamental characteristics of a stable vapor bubble will facilitate rational design of nanostructures

291 In particular, aligned and patterned bubbles with a tunable departure frequency and diameter

292 and PFOS partitions to the interfaces of air bubbles with the hydro-oleophobic perfluorocarbon chain

293 otion of large (20 mum in diameter) magnetic bubbles with two-dimensional skyrmion topology, driven b

294 Bubbles with varying particle coverages are made and the

295 LKL results in the generation of broken, PM "bubbles" with exposed PS that are released from the surf

296 ved from intervessel pits first, followed by bubbles within perforation plates, which hold the last v

297 ezers assay, we construct RPA-stabilized DNA bubbles within torsionally constrained DNA to investigat

298 ) N-pyridine at 9.4 T following parahydrogen bubbling within a magnetic shield.

299 the latter below the critical size at which bubbles would expand to form embolisms.

300 g but have been hindered by the inability to bubble Xe through the desired media as a result of visco