ライフサイエンスコーパス: gas bubble

1 ed and finally stabilized by an intracameral gas bubble.

2 between the anterior inferior retina and the gas bubble.

3 of systemic intravascular and extravascular gas bubbles.

4 he study of the pathophysiological aspect of gas bubbles.

5 terfaces and form protective coatings around gas bubbles.

6 face is less prone to blockage by any formed gas bubbles.

7 ts that are suspended together with numerous gas bubbles.

8 spreading of the minority liquid around the gas bubbles.

9 not higher than 2.5 V to avoid generation of gas bubbles.

10 Because evolved gas bubbles adhere and block parts of the electrodes and

11 that the relationship between an intraocular gas bubble and contact with the retina has been evaluate

12 replaced oxidation of water, eliminating O2 gas bubble and H+ formation.

13 The relationship between the gas bubble and residual vitreous fluid showed a rapid sh

14 Relationship between the gas bubble and residual vitreous fluid.

15 positioning gives better contact between the gas bubble and the inferior and anterior retina than pro

16 urvey what is known about the interaction of gas bubbles and electrode surfaces and the influence of

17 ine monomers across the interface and retain gas bubbles and heat of the reaction in the interfacial

18 Here we show that gas bubbles and liquid drops can exist in stable, non-sp

19 Here we study the merging of gas bubbles and liquid drops in an external fluid.

20 efforts to model the behavior of individual gas bubbles and multiphase flows produced at gas-evolvin

21 various species' ability to localize around gas bubbles and pipettes filled with nutrients.

22 ion of various thickness of zones denuded in gas bubbles and precipitates, and their relation to the

23 , confirming that the optical method detects gas bubbles and provides insights into the air-seeding h

24 veal contrasting interaction between growing gas bubbles and the crystal framework in crystal-rich ma

25 t is due to both contaminant partitioning to gas bubbles and to sediment resuspension.

26 blocking of the catalyst surface by evolved gas bubbles, and (iii) detachment of the catalyst from t

27 lar disorder superimposed and exacerbated by gas bubbles, and clearly differ from acute systemic gas

28 The effects of undissolved quartz particles, gas bubbles, and compositional inhomogeneity on the melt

29 he buoyant jet of petroleum liquid droplets, gas bubbles, and entrained seawater, using 279 simulated

30 que bubble layer, epithelial breakthrough of gas bubbles, and gas bubbles within the anterior chamber

31 ack between decompression rate, retention of gas bubbles, and integrity of the crystal framework lead

32 gen gas formation, entrapment and release of gas bubbles, and secondary mineral precipitation have be

33 ge transport capability, easy release oxygen gas bubbles, and strong structural stability, which are

34 transport capability, easy release of oxygen gas bubbles, and strong structural stability.

35 ensities and volumes of liquid oil droplets, gas bubbles, and two-phase droplet-bubble pairs.

36 g liquids (aqueous assay solution, oil), the gas bubbles are clearly visible from the top, when the a

37 The released gas bubbles are documented by recording videos of the as

38 phical software to obtain diameters of every gas bubble at each time point.

39 Exploring the nucleation of gas bubbles at interfaces is of fundamental interest.

40 lipid and polymer-stabilized perfluorocarbon gas bubbles before and after their destruction with high

41 locities are consistent with the presence of gas bubbles beneath the water table under valley and rid

42 s of simulated petroleum liquid droplets and gas bubbles by 3.2-fold and 3.4-fold, respectively, whic

43 demonstrate that these interactions enhance gas bubble detachment and displacement through magnetic

44 yancy in microgravity, resulting in hindered gas bubble detachment from electrodes and diminished ele

45 The behavior of fission gas bubbles dictates nuclear fuel performances, such as

46 Fish can suffer from gas bubble disease (GBD), characterized by the formation

47 d can only be attributed to the existence of gas bubbles due to the strong compressibility dependence

48 ificantly advantageous in producing a single gas bubble during shallow as well as during deep injecti

49 The evolution of electrogenerated gas bubbles during water electrolysis can significantly

50 Gas bubble dynamics and liquid/solid products were analy

51 e negative impacts such as Joule heating and gas bubble evolution from common nanosecond pulse treatm

52 R may reach a critical point at which oxygen gas bubbles fill the pores of the ACL and PTL, completel

53 ction-dominated conditions can be created by gas bubble flow in the saturated zone.

54 rough a single pore to study the dynamics of gas bubble formation and evolution.

55 to physiological changes that contribute to gas bubble formation and growth that could lead to anima

56 t of water electrolysis, thereby eliminating gas bubble formation and/or pH drift.

57 Although gas bubble formation appeared to be more pronounced at h

58 was seen to modify the plasma properties and gas bubble formation dynamics, significantly influencing

59 ar followed by rapid decompression may cause gas bubble formation within the blood stream (embolism)

60 live oil droplets within 14.5 min, prior to gas bubble formation, during the experiments of Pesch et

61 ation of oxygen gas, effectively suppressing gas bubble formation.

62 Although gas-bubble formation may be aggravated by acoustic energ

63 We investigate the stability of gas bubbles formed at saturated (bubble-point) condition

64 , to efficiently detect and classify fission gas bubbles from scanning electron microscopic images.

65 neration by promoting the release of evolved gas bubbles from the electrode surface.

66 Gas bubbles from the mounds rise to within 300 m of the

67 vel adaptation of cryo-EM based on detecting gas bubbles generated by radiation damage was used to lo

68 Gas bubbles generated by the hydrogen evolution reaction

69 A micromixing technique based on gas bubbling generated by electrochemical micropumps was

70 ide liquid droplets by surface attachment to gas bubbles has been suggested as a mechanism to overcom

71 cept for the lowest irradiation temperature, gas bubbles have the shape of thin hexagonal prisms with

72 ose to a liquid-vapor interface of a captive gas bubble in a microchannel, interphase mass-transfer t

73 m nonlinear pulsations of an isolated vapour-gas bubble in an acoustic field.

74 Ultrasound can drive a single gas bubble in water into violent oscillation; as the bub

75 tion, growth, and coalescence of microscopic gas bubbles in a molding process.

76 ique parameters on the formation of multiple gas bubbles in a porcine eye model for pneumatic retinop

77 Cavitation, or the oscillation of small gas bubbles in a pressure-varying field, has been shown

78 achieve a supersaturated state and can form gas bubbles in blood and tissues, with resulting tissue

79 servation of the nucleation and migration of gas bubbles in iron (hydr)oxide using transmission elect

80 Historical characterization of fission gas bubbles in irradiated nuclear fuel relied on a simpl

81 The nucleation of gas bubbles in magmas is fundamental to controlling the

82 The self-organisation of void and gas bubbles in solids into superlattices is an intriguin

83 The number of gas bubbles in the eye was assessed with indirect ophtha

84 ortant in reducing the formation of multiple gas bubbles in the eye were shallow depth of injection a

85 crofluidic generation of highly monodisperse gas bubbles in the liquid reaction medium and subsequent

86 The presence of large gas bubbles in the samples with oxidizing agents may hav

87 esults in the introduction and generation of gas bubbles in the solvent.

88 Here, we explore how gas bubbles in water subjected to a thermal gradient, a

89 ater interface, stabilizing micrometer-sized gas bubbles in water, and disassemble by tuning of the a

90 The dynamics of a gas bubble inside a water conduit after a cavitation eve

91 stimuli were delivered to the tissue through gas bubbled into the brain slice chamber.

92 l tracheal trunks (DTTs) by the expulsion of gas bubbles into the body.

93 Protein denaturation caused by gas bubbles is a well-known phenomenon.

94 of the overall evolution behavior of fission gas bubbles is well known, lacking the quantitative data

95 fragmentation of magma, containing abundant gas bubbles, is thought to be the defining characteristi

96 ulness of this first fish model to study the gas-bubbles lesions associated to DCS from a pathologica

97 as-filled cysts, tentatively interpreted as "gas-bubble" lesions in various other cetacean species.

98 cal reactions, the formation and collapse of gas bubbles, merger of fluid droplets, and release of hy

99 an association between swelling due to inert gas bubble nucleation and growth and radiation-induced s

100 Our results suggest that the size of stable gas bubble nuclei depends only on the local concentratio

101 clear fission reactions tend to form fission gas bubbles of various shapes and sizes inside nuclear f

102 1.6%) were located outside the limits of the gas bubble on the first or third day postoperatively.

103 ible reasoning for the abundant formation of gas bubbles on intermetallic precipitates, observation o

104 Recent studies of individual gas bubbles on nanoelectrodes have resulted in unprecede

105 investigate the mechanisms of nucleation of gas bubbles on nanoelectrodes, and characterize their st

106 onic thickening and several focal intramural gas bubbles (pneumatosis intestinalis) surrounding the p

107 h/kg COD, reduced foam formation due to less gas bubble production, minimum scale formation, and lowe

108 e model scenarios suggest that 5 mm diameter gas bubbles released at a <470 m water depth can transpo

109 from the sediment into the water column via gas bubbles released from the seabed was documented.

110 , and a lack of postoperative OCT data after gas bubble resolution.

111 draulic pathways in some plants, as residual gas bubbles should expand when vessels are reconnected t

112 ed system was distinctly more robust against gas bubbles, showed a higher signal gain, and allowed us

113 of intravascular and extravascular systemic gas bubbles, similarly to that observed in DCS.

114 uires a combination of fast gas release from gas bubbles (slugs) at the top of the magma conduit and

115 he fluorinations appear to take place at the gas bubble-solution interface.

116 ful in determining size and structure of the gas bubble superlattice as a function of irradiation con

117 with our recent theoretical predictions for gas bubble superlattice formation and highlight that sup

118 pacings similar to those observable when the gas bubble superlattice has formed with very large order

119 To understand the formation of the void/gas bubble superlattices in crystals under irradiation,

120 ers on the formation and structure of helium gas bubble superlattices within a tungsten host matrix t

121 ted formation of the unusual phase in a H(2) gas bubbling system.

122 ve quantities of macroscopic and microscopic gas bubbles, systemically distributed, circulating throu

123 Otherwise, all gas bubbles that form undergo, possibly oscillatory, gro

124 egative pressure without constantly creating gas bubbles that would disable their hydraulic systems.

125 Surface tension gives gas bubbles their perfect spherical shape by minimizing

126 e mixtures were studied by exposing a single gas bubble to water.

127 It employs the carbogen gas bubbles to drive the flow circulation in a consisten

128 nced ultrasound (CEUS) uses shell-stabilized gas bubbles to provide acoustic backscatter in vasculatu

129 cts during metamorphosis, including impaired gas bubble translocation, head eversion, leg elongation,

130 Advanced characterization of fission gas bubbles using scanning electron microscopic images r

131 When the gas bubble was fully resorbed the graft started to detac

132 etermination of the size and symmetry of the gas bubbles was performed using a combination of small a

133 due to the formation of frequent embolisms (gas bubbles), which could be removed by the occurrence o

134 s such as misoriented subdomains and trapped gas bubbles, which are stabilized by molecular-scale str

135 ostructural modification is the formation of gas bubbles, which is revealed at all studied irradiatio

136 In the stable spiral case gas bubbles will achieve a steady-state finite size only

137 ing summer to -68.5 per mil during winter in gas bubbles with an average methane content of 95%.

138 model has the capability to identify fission gas bubbles with and without lanthanides to better under

139 epithelial breakthrough of gas bubbles, and gas bubbles within the anterior chamber.