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Fluid droplets

Resistance functions have been evaluated in numerical compu-tations15831 for low Reynolds number flows past spherical particles, droplets and bubbles in cylindrical tubes. The undisturbed fluid may be at rest or subject to a pressure-driven flow. A spectral boundary element method was employed to calculate the resistance force for torque-free bodies in three cases (a) rigid solids, (b) fluid droplets with viscosity ratio of unity, and (c) bubbles with viscosity ratio of zero. A lubrication theory was developed to predict the limiting resistance of bodies near contact with the cylinder walls. Compact algebraic expressions were derived to accurately represent the numerical data over the entire range of particle positions in a tube for all particle diameters ranging from nearly zero up to almost the tube diameter. The resistance functions formulated are consistent with known analytical results and are presented in a form suitable for further studies of particle migration in cylindrical vessels. [Pg.338]

In addition to the oxygen and carbon dioxide exchanged here, this area of the lung is necessarily exposed to other gases (carbon monoxide, nitrogen, etc.) to fluid droplets and to particulates in the ambient air. The air in the lung is essentially saturated with water vapor as it passes through the nasal scrubber to the bronchi, bronchioles, and ducts to the air sacs. [Pg.109]

Consider a two-component, two-phase fluid system. Let (3 be a spherical fluid droplet of radius r surrounded by a, the second fluid phase. The equilibrium conditions are... [Pg.612]

Fig. 32. Amplitude (a,c) and phase (b,d) SFM micrographs demonstrate autophobic wetting of mica (a,b) and semifluorinated copolymer (c,d) by carbosilane dendrimer with hydroxyl end groups. Fluid droplets with a contact angle of about 8.7 degrees in (a) and 18.5 degrees in (c) were determined after 24 h equilibration at room temperature from cross sectional profiles recorded along the reference lines indicated on the (a) and (b) respectively. Reproduced from [319]... Fig. 32. Amplitude (a,c) and phase (b,d) SFM micrographs demonstrate autophobic wetting of mica (a,b) and semifluorinated copolymer (c,d) by carbosilane dendrimer with hydroxyl end groups. Fluid droplets with a contact angle of about 8.7 degrees in (a) and 18.5 degrees in (c) were determined after 24 h equilibration at room temperature from cross sectional profiles recorded along the reference lines indicated on the (a) and (b) respectively. Reproduced from [319]...
Aerosol An aerosol is the spray of small fluid droplets that can be generated particularly when the nozzle of a flow cytometer is vibrated for sorting applications. If samples contain material that may be a biological hazard, attention should be paid to containment of the aerosol by suction through small-pore, hydrophobic filters. [Pg.236]

Two-fluid droplet generation and mixing - close contact... [Pg.158]

Figure 1.120 Schematic design of the various mixing nozzles analyzed two-fluid droplet close contact (left) two-fluid droplet separated by annulus (middle) three-fluid droplet with separation layer (right) [135],... Figure 1.120 Schematic design of the various mixing nozzles analyzed two-fluid droplet close contact (left) two-fluid droplet separated by annulus (middle) three-fluid droplet with separation layer (right) [135],...
Cell cultivation has been conducted within aqueous fluid droplets embedded in a non-immiscible carrier liquid. This method that was conducted in a Si-glass microchannel was used to generate monoclonal antibodies [312]. In addition, human connective tissue progenitor (CTP) cells and human bone marrow-derived cells were cultured within PDMS channels [164], Cell culture for fibroblasts has been possible even under an AC field [896],... [Pg.288]

Tasks — Breaking down solids, polymer particles, and fluid droplets... [Pg.67]

The modification involved the rerouting of the discharge water from the barometric condenser. Rather than being discharged into a chemical sewer via a sump, the water stream had been routed to a hopper that allowed the entrained heat transfer fluid droplets to drop out of solution md be recovered. Decontaminated water overflowed to the chemical sewer (see Figure 2-17). [Pg.35]

Alireza Sai di, Celine Martin, Albert Magnin, Influence of yield stress on the fluid droplet impact control, Journal of Non-Newtonian Fluid Mechanics, vol. 165, Issues 11-12, 596-606, 2010. [Pg.36]

Eunjeong Kim, Jehyun Baek, Numerical study of the parameters governing the impact dynamics of yield-stress fluid droplets on a solid surface, Journal of Non-Newtonian Fluid Mechanics, vol. 173-174, 62-71, 2012. [Pg.36]

Next, we proceed with the case when surfactant is present and the Marangoni effect becomes operative. Classical experiments carried out by Lebedev " and Silvey show that the measured velocity of sedimentation, U, of small fluid droplets in a viscous liquid (pure liquid phases assumed) does not obey the Hadamar and Rybczynski equation ... [Pg.251]

For the purpose of assessment of macroscopic equations, DNS data are generated for evaporating droplets dispersed in homogeneous shear flows by extending the previous study [17], In this particular case, some of the statistical properties of interests are droplet Reynolds stresses, rjt fluid-droplet velocity correlations, u Vj temperature correlation, O O and mean diameter, d, of the droplets. The temporal variations of n-i t, ujr, and O O are shown in Figs. 3.4a-3.4c, respectively. The varying evaporation rate for an individual droplet, which due to the stochastic nature of fluid flow field, results in polydispersed droplets even when the monodispersed droplets are injected in the flow. The variance droplet diameter and skewness indicates the extent of polydispersity. The temporal variations of mean diameter d, variance a. and skewness are shown... [Pg.28]

Saffinan and Turner (43) considered collisions between droplets due to turbulence in rain clouds. Under turbulent conditions, droplet collision is governed by two different mechanisms isotropic turbulent shear and turbulent inertia. The choice of regime applicable to a droplet is determined by its size in relation to the Kolmogorov microscale denned earlier. Droplets of diameter d > t are subjected to die former of these processes (small-scale motion). Spatial variations in the flow give neighboring droplets different velocities and fliis result in collisions. Droplets of diameter d > T] are subjected to turbulent inertia. In this case, collisions result from the relative movement of droplets in the surrounding fluid. Droplets of different diameter will have different inertias and this results in collisions. Droplets of equal diameter, however, will not collide under this mechanism as fliey have the same inertia. [Pg.684]

C. A. Miller and L. E. Scriven, The oscillations of a fluid droplet immersed in another fluid, J. Huid Mech. 32,417, 1968. [Pg.143]

Surface tension is directly related to the Taylor cone formation and this is related to the electric field strength applied over the fluid droplet able to deform its shape (Fig. 1.9). This tension value is... [Pg.33]


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Fluid droplets measurements

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