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Wetting droplet shape

The above information is all that is required to perform a preliminary sizing on a spray dryer. The temperature limit of the product is given at 170°F. Using 160 F as the outlet temperature of the dryer should allow us the safety necessary so as not to exceed the temperature limit of the dry powder (product). The fact that we get evaporative cooling while drying the spherically shaped droplets to a similarly shaped powder allows us to use an inlet temperature of about 320°F. Thus the temperature difference (AT) is 160°F. This is the primary driving force in motivating the water to leave the product due to the enormous difference in saturation equilibrium between the wet droplet/dry powder and the very hot dry air. [Pg.749]

Imposing A[/<3 = 0, thus seeking the equilibrium condition, then immediately leads to Equation (4.9). Such derivation is certainly simplified, not taking into account the variation of the droplet shape due to the total liquid volume conservation, however it is very intuitive, and, what matters most in this context, it can be immediately extended to describe the macroscopically observed wetting behavior on nanostructured surfaces, including coatings, mats and membranes made of polymer nanofibers. [Pg.218]

A venturi scrubber is a venturi-shaped air passage with water introduced just ahead of or into the venturi throat. The liquid-gas contact is at a maximum in the venturi throat. The relative velocity between gas and liquid aerosol droplets is high, with the gas velocities in the range of 50-100 m/s. The particles are conditioned in the throat, and condensation is the important collection mechanism. After the particles in the gas have been deposited on droplets, a comparatively simple device such as a cyclone collector can be used to collect the wetted dust. [Pg.1247]

The shape of a droplet or of the front end of a film can be determined from the surface energies and interaction forces between the interfaces. These also determine the equilibrium thickness of a liquid film that completely wets a surface. The calculation is done by minimization of the free energy of the total system. In a two-dimensional case the free energy of a cylindrical droplet can be expressed as [5] ... [Pg.245]

A very different behavior is observed when condensation occurs on a mica surface that has been exposed to air for a few hours (we will refer to it as contaminated mica ). In this case glycerol forms droplets in the shape of spherical caps, indicating that it does not completely wet the surface. This behavior is similar to that of water, which we present in detail later. The contact angle of water on mica surfaces increased from 0° on the freshly cleaved surface to a small value between 2 and 3° on the contaminated mica [51]. [Pg.259]

When a droplet is deformed asymmetrically, the ratchet motions of the droplet can be induced as demonstrated on the vibrated gradient surface and on a saw-shaped electrode on which the wetting was changed by electrowetting [48]. [Pg.284]

Figure 16.10 Photographs of nitrobenzene droplets. Vtias was fixed at 0.35 V and Eoffset was varied (a-d). The line in the photograph represents the position of the wetting boundary estimated from the shape of the droplets. Note that the current peak for the Fc /Fc reaction was observed at about —0.5 V in the cyclic voltammogram. Figure 16.10 Photographs of nitrobenzene droplets. Vtias was fixed at 0.35 V and Eoffset was varied (a-d). The line in the photograph represents the position of the wetting boundary estimated from the shape of the droplets. Note that the current peak for the Fc /Fc reaction was observed at about —0.5 V in the cyclic voltammogram.
The shape of liquid droplets emerging at the GDL/ channel interface is governed by the wetting char-... [Pg.505]

Thus we would expect water to climb up the walls of a clean (i.e. water-wetting) glass vessel for a few millimetres but not more, and we would expect a sessile water droplet to reach a height of several mm on a hydrophobic surface, before the droplet surface is flattened by gravitational forces. The curved liquid border at the perimeter of a liquid surface or film is called the Plateau border after the French scientist who studied liquid shapes after the onset of blindness, following his personal experiments on the effects of sunlight on the human eye. [Pg.19]

A practical application coming out of field ion emission is the liquid metal ion source. Ion sources of a wide variety of chemical elements, most of them low melting point metals, can be produced by using either liquid metals131,132 or liquid alloys.133 The idea of extracting charged droplets out of liquid by application of an electrostatic field is perhaps older than field ion microscopy. But the development of liquid metal ion sources from liquid capillaries, from slit shaped emitter modules and from wetted field emission tips, etc., as well as the understanding of the mechanisms of ion formation in terms of field evaporation and field ionization theories,... [Pg.360]

Wetting angle — A liquid droplet formed on a flat solid foreign substrate has the cap-shaped form of a spherical segment (Figure) with a volume,... [Pg.707]

The shape of solidified, millimetre size, droplets reflect wetting of the liquid on the solid substrate. The equilibrium shape of a solid particle M on a solid S in a vapour... [Pg.126]


See other pages where Wetting droplet shape is mentioned: [Pg.28]    [Pg.219]    [Pg.228]    [Pg.34]    [Pg.385]    [Pg.34]    [Pg.132]    [Pg.293]    [Pg.665]    [Pg.185]    [Pg.246]    [Pg.467]    [Pg.491]    [Pg.235]    [Pg.285]    [Pg.16]    [Pg.193]    [Pg.208]    [Pg.211]    [Pg.384]    [Pg.497]    [Pg.56]    [Pg.156]    [Pg.491]    [Pg.235]    [Pg.131]    [Pg.50]    [Pg.267]    [Pg.488]    [Pg.189]    [Pg.718]    [Pg.243]    [Pg.541]    [Pg.1843]    [Pg.356]    [Pg.561]    [Pg.638]    [Pg.842]   
See also in sourсe #XX -- [ Pg.104 , Pg.109 , Pg.131 ]




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