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Free surface shape

It is desirable to consider the interface heights of the three transducers with transducers 1 and 3 being to the left and to the right of transducer 2, respectively, as shown in Figure 9b. When only one transducer is used, the gas-liquid interface is assumed to be flat as in Figure 10a (line p-p ) then the area occupied by the liquid phase near the wall of the pipe and above the gas-liquid interface is ignored. With three transducers, however, a more accurate gas-liquid free surface shape may be obtained... [Pg.15]

We note here that although the free surface shape was set down at the outset, it could have been found directly by solving for the velocity potential (p as outlined and then determining say, from Eq. (10.4.14). [Pg.312]

The determination of the equation for the free surface shape and the eigenvalue relation between the amplification factor (3, the wave number k, and the integer n is carried out just as in the evaluation of the dispersion relation for plane waves. In particular, from the kinematic boundary condition Eq. [Pg.317]

There has been some development in the numerical modeling of the sheet formation from swirl nozzles. A fully nonlinear model using an axisymmetric boundary element formulation has been developed for simulating the free surface shape and spray formed by simplex/pressure swirl atomizers [30, 32]. A linear instability analysis by Ponstein has been used to predict the number of droplets formed from each ring-shaped ligament shed from the parent surface. [Pg.763]

The long middle region of the film offers the possibility of still further simplification. If one rescales the variables in the problem again, a much simpler equation for the (rescaled) free surface shape K Z,T) arises, which we shall call the flat film model. This model is... [Pg.244]

Surfactant transport is also important in the vertical draining film surfactant concentration gradients may develop, which may in turn strongly affect the fluid flow via the Marangoni effect. When surfactant transport is considered, lubrication theory then gives three nonlinear partial differential equations for the free surface shape k(z,t), the surface velocity w z,t) and the surface concentration of surfactant (, ). The mathematical problem to be solved for these dependent variables is ... [Pg.249]

Radiation in the transmitting and emitting media of the molten glass is a significant contributor to the overall heat transfer and cannot be accurately simulated by an effective thermal conductivity at this small size scale. The addition of a full discrete ordinates (DO) treatment of the radiative heat transfer should also improve the accuracy of the free surface shape development, but at a very high cost for simulation speed and resources required. [Pg.225]

Figure 16.6. A short catalogue of edge-free surface shapes, classified by their genus (a) genus zero, (b) two examples of genus one surfaces, and (c) two examples of genus two surfaces. Adding extra handles (or donut channels) increases the genus, and arbitrarily high genus surfaces are realizable... Figure 16.6. A short catalogue of edge-free surface shapes, classified by their genus (a) genus zero, (b) two examples of genus one surfaces, and (c) two examples of genus two surfaces. Adding extra handles (or donut channels) increases the genus, and arbitrarily high genus surfaces are realizable...
Sillinian, W. J. and Scriven, L. E., 1980. Separating flow near a static contact line slip at a wall and shape of a free surface.. /. Comput. Phys. 34, 287-313. [Pg.110]

Besides electronic effects, structure sensitivity phenomena can be understood on the basis of geometric effects. The shape of (metal) nanoparticles is determined by the minimization of the particles free surface energy. According to Wulffs law, this requirement is met if (on condition of thermodynamic equilibrium) for all surfaces that delimit the (crystalline) particle, the ratio between their corresponding energies cr, and their distance to the particle center hi is constant [153]. In (non-model) catalysts, the particles real structure however is furthermore determined by the interaction with the support [154] and by the formation of defects for which Figure 14 shows an example. [Pg.177]

Tension in the free surface of a liquid is the cause of the tendency of a liquid surface to assume the form having a minimum area, as manifested in the shape of a bubble or a drop of liquid.25 The tendency to contract is a special case of the general principle that potential energy tends toward a minimum value. [Pg.695]

Another typical example of inhomogeneity in rheometry is the oxidation of a polymer in a rotational rheometer in which a disk-shaped sample is held between metal fixtures. The oxygen enters the sample through the free surface (at the outer diameter) and diffuses radially inwards. The result is a radial gradient in properties which changes with time. If the reaction with oxygen results in... [Pg.217]

When an open tank with a free surface is stirred with an impeller, a vortex will form around the shaft. It is important to prevent this vortex from reaching the impeller, because entrainment of air in the liquid tends to cause foaming. The shape of the free surface depends upon (among other things) the fluid properties, the speed and size of the impeller, the size of the tank, and the depth of the impeller below the free surface. [Pg.46]

Just like the accelerating tank, the shape of the free surface can be determined from the fact that the pressure is constant at the surface, i.e.,... [Pg.93]


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