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Layer viscous

The above set of equations is similar to that used in traditional computational fluid dynamics (CFD) (except for the electron energy balance and the EM equations), and advances made in that field can be used to benefit the plasma reactor simulation problem. As an example, the sheath near the wall can be thought of as similar to a boundary layer in fluid flow (chemically reacting or not) [130]. Separating the flow into bulk (inviscid) and boundary layer (viscous) and then patching the two solutions (asymptotic analysis) has long been practiced in fluid mechanics and may also be applied to the plasma problem [102, 103, 151]. [Pg.285]

Buffer layer Viscous sub layer Wox particles Solid paraffin wax Tube woll... [Pg.129]

For external flow such as flow over a flat stationary plate whose surface temperature is different from the bulk fluid temperature, both hydrodynamic and thermal boundary layers develop along the direction of the flow. Inside the hydrodynamic boundary layer viscous forces are dominant resulting in velocity profile. Similarly as thermal boundary layer develops along the flow direction and heat is being transferred to or from the surface results in a temperature profile. In Figure 22.8 the hydrod5mamic and thermal boundary layers are shown for flow over a heated flat plate. Both velocity and temperature inside the boundary layer reach 99% of the free stream velocity (Vf) and temperature (T ), respectively, at the edge of the boundary layer. [Pg.741]

D 4796 BOND STRENGTH OF TRAFFIC MARKING MATERIALS D 4946 BLOCKING RESISTANCE OF ARCHITECTURAL PAINTS D 4948 DETERMINATION OF UPPER LAYER VISCOUS... [Pg.626]

The comparison of flow conductivity coefficients obtained from Equation (5.76) with their counterparts, found assuming flat boundary surfaces in a thin-layer flow, provides a quantitative estimate for the error involved in ignoring the cui"vature of the layer. For highly viscous flows, the derived pressure potential equation should be solved in conjunction with an energy equation, obtained using an asymptotic expansion similar to the outlined procedure. This derivation is routine and to avoid repetition is not given here. [Pg.182]

Into a 500 ml. three-necked flask, provided with a mechanical stirrer, a gas inlet tube and a reflux condenser, place 57 g. of anhydrous stannous chloride (Section 11,50,11) and 200 ml. of anhydrous ether. Pass in dry hydrogen chloride gas (Section 11,48,1) until the mixture is saturated and separates into two layers the lower viscous layer consists of stannous chloride dissolved in ethereal hydrogen chloride. Set the stirrer in motion and add 19 5 g. of n-amyl cyanide (Sections III,112 and III,113) through the separatory funnel. Separation of the crystalline aldimine hydrochloride commences after a few minutes continue the stirring for 15 minutes. Filter oflF the crystalline solid, suspend it in about 50 ml. of water and heat under reflux until it is completely hydrolysed. Allow to cool and extract with ether dry the ethereal extract with anhydrous magnesium or calcium sulphate and remove the ether slowly (Fig. II, 13, 4, but with the distilling flask replaced by a Claisen flask with fractionating side arm). Finally, distil the residue and collect the n-hexaldehyde at 127-129°. The yield is 19 g. [Pg.324]

In a wide-mouthed test-tube ( boiling tube ) place 5 g. of phenol, 15 ml. of 40 per cent, formaldehyde solution and 3 ml. of concentrated ammonia solution (sp. gr. 0-88). Warm the mixtme with a small flame until it becomes opaque. Cool, discard the aqueous layer, but retain the viscous material in the tube. Heat the latter in a water bath at 60° for 30 minutes and then heat the pasty mass in an air oven at 75° for 4-6 hours. A hard sohd resin is produced. [Pg.1023]

The yellow solution was poured into 150 ml of water. After addition of 20 g of ammonium chloride and vigorous shaking, the layers were separated. The aqueous layer was extracted twice with diethyl ether. The combined solutions were dried over magnesium sulfate and concentrated in a water-pump vacuum. The residue was distilled at low pressure giving the desired carbinol, (b.p. 40°C/0.1 mmHg), n 1.5505 in 66-702 yield. A small viscous residue remained in the distillation flask. [Pg.80]

Slip casting of metal powders closely follows ceramic slip casting techniques (see Ceramics). SHp, which is a viscous Hquid containing finely divided metal particles in a stable suspension, is poured into a plaster-of-Paris mold of the shape desired. As the Hquid is absorbed by the mold, the metal particles are carried to the wall and deposited there. This occurs equally in all directions and equally for metal particles of all sizes which gives a uniformly thick layer of powder deposited at the mold wall. [Pg.185]

Ko//M //s. When dispersion is requited ia exceedingly viscous materials, the large surface area and small mixing volume of roU mills allow maximum shear to be maintained as the thin layer of material passiag through the nip is continuously cooled. The roUs rotate at different speeds and temperatures to generate the shear force with preferential adhesion to the warmer roU. [Pg.441]

Tar sand, also variously called oil sand (in Canada) or bituminous sand, is the term commonly used to describe a sandstone reservoir that is impregnated with a heavy, viscous black extra heavy cmde oil, referred to as bitumen (or, incorrectly, as native asphalt). Tar sand is a mixture of sand, water, and bitumen, but many of the tar sand deposits in the United States lack the water layer that is beHeved to cover the Athabasca sand in Alberta, Canada, thereby faciHtating the hot-water recovery process from the latter deposit. The heavy asphaltic organic material has a high viscosity under reservoir conditions and caimot be retrieved through a weU by conventional production techniques. [Pg.351]

The concentration boundary layer forms because of the convective transport of solutes toward the membrane due to the viscous drag exerted by the flux. A diffusive back-transport is produced by the concentration gradient between the membranes surface and the bulk. At equiUbrium the two transport mechanisms are equal to each other. Solving the equations leads to an expression of the flux ... [Pg.296]


See other pages where Layer viscous is mentioned: [Pg.53]    [Pg.77]    [Pg.61]    [Pg.235]    [Pg.235]    [Pg.29]    [Pg.139]    [Pg.127]    [Pg.285]    [Pg.53]    [Pg.77]    [Pg.61]    [Pg.235]    [Pg.235]    [Pg.29]    [Pg.139]    [Pg.127]    [Pg.285]    [Pg.122]    [Pg.184]    [Pg.242]    [Pg.189]    [Pg.253]    [Pg.698]    [Pg.698]    [Pg.899]    [Pg.1008]    [Pg.33]    [Pg.34]    [Pg.68]    [Pg.228]    [Pg.510]    [Pg.81]    [Pg.255]    [Pg.476]    [Pg.89]    [Pg.90]    [Pg.102]    [Pg.431]    [Pg.199]    [Pg.298]    [Pg.193]    [Pg.372]    [Pg.457]    [Pg.306]    [Pg.249]    [Pg.147]   
See also in sourсe #XX -- [ Pg.80 , Pg.112 ]




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