ライフサイエンスコーパス: gas bubble

1 ts that are suspended together with numerous gas bubbles.

2 spreading of the minority liquid around the gas bubbles.

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

52 1.6%) were located outside the limits of the gas bubble on the first or third day postoperatively.

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

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

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

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

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

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

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

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

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

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