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Of constant velocities

Along with a constant velocity zone (Zone 1), there is a constant temperature zone in a jet. Heat diffusion in a jet is more intense than momentum diffusion therefore the core of constant temperatures fades away faster than that of constant velocities and the temperature profile is flatter than the velocity profile. Thus the length of the zone with constant temperature (Fig. 7.23) is shorter than the length of the constant velocity zone (Zone I... [Pg.457]

In a front-wheel-drive car, the drive wheels experience not only the road-induced vertical motion of the rear wheels hut also must rotate about a vertical axis to accommodate steering. Several different configurations of constant-velocity universal joints have been developed to manage such motion. These constant-velocity joints are larger and more expensive than the joint described above. [Pg.356]

Common geometries used to make viscosity measurements over a range of shear rates are Couette, concentric cylinder, or cup and bob systems. The gap between the two cylinders is usually small so that a constant shear rate can be assumed at all points in the gap. When the liquid is in laminar flow, any small element of the liquid moves along lines of constant velocity known as streamlines. The translational velocity of the element is the same as that of the streamline at its centre. There is of course a velocity difference across the element equal to the shear rate and this shearing action means that there is a rotational or vorticity component to the flow field which is numerically equal to the shear rate/2. The geometry is shown in Figure 1.7. [Pg.11]

The momentum equation (the Navier-Stokes equation) for fluid flow (De Groot and Mazur, 1962) is complicated and difficult to solve. It is the subject of fluid mechanics and dynamics and is not covered in this book. When fluid flow is discussed in this book, the focus is on the effect of the flow (such as a flow of constant velocity, or boundary flow) on mass transfer, not the dynamics of the flow itself. [Pg.183]

Fig. 1, Calculated lines of constant velocity in a water film flowing near the comer of a rectangular glass channel at 30° to the horizontal film thickness far from side wall is 1 mm. (F7). Fig. 1, Calculated lines of constant velocity in a water film flowing near the comer of a rectangular glass channel at 30° to the horizontal film thickness far from side wall is 1 mm. (F7).
Figure 4.S3. Locations of the lines of constant velocity at the finish of mold filling for a rate constant equal to... Figure 4.S3. Locations of the lines of constant velocity at the finish of mold filling for a rate constant equal to...
Figure 4.65. Lines of constant velocities for five positions of the stream front for a regime marked by point D in Figure 4.56. Figure 4.65. Lines of constant velocities for five positions of the stream front for a regime marked by point D in Figure 4.56.
When a fluid flow of constant velocity, u, impinges parallel to the edge of a plate, the boundary condition is such that the fluid velocity is zero on the surface of the plate. This results in the formation of a hydrodynamic boundary layer in which the flow velocity parallel to the surface varies with distance normal to the surface. The hydrodynamic boundary layer thickness increases with distance, jc, from the upstream edge of the plate as given by equation (10.5) [7] ... [Pg.376]

At very low shear rates (i.e., flow velocities), particles in a chemically stable suspension approximately follow the layers of constant velocities, as indicated in Fig. 2. But at higher shear rates hydro-dynamic forces drive particles out of layers of constant velocity. The competition between hydrodynamic forces that distort the microstructure of the suspension and drive particles together, and the Brownian motion and repulsive interparticle forces keeping particles apart, leads to a shear dependency of the viscosity of suspensions. These effects depend on the effective volume fraction of... [Pg.321]

Fig. 2. Laminar flow within a capillary Hydrodynamic forces drive particles out of layers of constant velocity. Fig. 2. Laminar flow within a capillary Hydrodynamic forces drive particles out of layers of constant velocity.
Fig. 4. Expected probability density for the particles velocities if particles follow layers of constant velocities (left) and the probability density calculated from the measured velocities of the particles (right). Fig. 4. Expected probability density for the particles velocities if particles follow layers of constant velocities (left) and the probability density calculated from the measured velocities of the particles (right).
The suspension is highly accelerated (up to several lOOm/s ) at the entrance of the capillary. Since the density of the particles is large, compared to the suspending fluid, the particles move relative to the fluid during the acceleration phase. The maximal shear rate at the border of the capillary is about /max = 80001/s. Under the assumption that the particles follow layers of constant velocities, as drawn in Fig. 2, the expected probability density of the particles velocities is calculated. The result is shown in the left panel of Fig. 4. As mentioned above, the wedge-like sector of the cross-section. [Pg.323]

For the simpler case of a capillary, as sketched in fig. 4.7 the derivation is straightforward. When the capillary is sufficiently wide, as we are assuming here, no double layer overlap occurs and there is a range of constant velocity in the centre. For wide capillaries (radius /c M. the contribution to the volume flow of the layers of variable velocity near the walls may be neglected in fact their presence Is not readily experimentally measurable. [Pg.496]

The technique of continuous flow was further improved and expanded with the introduction of pulsed flow, which uses short pulses of constant-velocity flow and cuts the reagent consumption to 3-4 mL per determination [6]. The combination of large flow velocities and short times was experimentally achieved by use of a special syringe ram assembly. [Pg.475]

Fig. 4. Orientation of an ellipsoidal molecule in a flowing liquid of constant velocity gradient. The positive Z axis points perpendicularly upward from the plane of the paper. The projection of the axis of revolution of the ellipsoid on the XV plane is denoted by aa. The movement of the Liquid is parallel to the X axis, and is described by the equation GY, where is the velocity and G is the velocity gradient. The significance of the angle

Fig. 4. Orientation of an ellipsoidal molecule in a flowing liquid of constant velocity gradient. The positive Z axis points perpendicularly upward from the plane of the paper. The projection of the axis of revolution of the ellipsoid on the XV plane is denoted by aa. The movement of the Liquid is parallel to the X axis, and is described by the equation GY, where is the velocity and G is the velocity gradient. The significance of the angle <P is shown in the figure (0= 90° when the a axis of the ellipsoid lies in the. STZ plane), d is the smaller of the two angles between the a axis of the ellipsoid and the positive Z axis. The origin is taken at the center of the ellipsoid. From Bdsall (29), page 518.
The cumulative result of these disadvantages has been to restrict the continued development of constant-velocity spectrometers. One of the few major developments of recent years has been the description of an instrument which takes readings at a number of velocities pre-programmed on a length of punched tape [14]. The great majority of investigations are now made using repetitive velocity-scan systems. [Pg.21]

The estimate shows that for typical conditions and a = 0 the growth of velocity is small. For a = 0.5 this growth is about 60%. Usually a does not exceed 0.2 [14] thus the assumption of constant velocity is a quite reasonable approximation. [Pg.214]

If we start from the moment the body is released from its position of rest, the falling of the body consists of two periods the period of accelerated fall and the period of constant velocity fall. The initial acceleration period is usually very short, of the order of a tenth of a second or so. Hence, the period of constant velocity fall is the important one. The velocity is called the free settling velocity or terminal velocity v,. [Pg.817]

Were it the case that auxin transport takes place within a plant part—a stem, a petiole, a root—by travelling in a solution of constant concentration (density) in a continuous stream of constant velocity (speed), then, the efficiency of the... [Pg.86]

In order to demonstrate the use of this method, two cases of constant velocity of approach were considered where the Hertzian zone film thickness was allovfed to drop from 2.2 to 1.C microns during 2x10-8 seconds. Using the values given in table 1 for the required data and assuming steady conditions prior to the reduction in film thickness, the corresponding load variation with time... [Pg.281]

Figure 10.4. Contours of constant velocity for a Maxwell fluid with dimensionless forces B = (a) 0.5, (b) 1.0, and (c) 1.5 at z = 5do. Reprinted with permission from Keun-ings et al., Ind. Eng. Chem. Fundam., 22, 347 (1983). Copyright American Chemical Society. Figure 10.4. Contours of constant velocity for a Maxwell fluid with dimensionless forces B = (a) 0.5, (b) 1.0, and (c) 1.5 at z = 5do. Reprinted with permission from Keun-ings et al., Ind. Eng. Chem. Fundam., 22, 347 (1983). Copyright American Chemical Society.
The explosive is burned before the first time interval by assuming it to be a gamma-law explosive that has been detonated with a rear boundary of constant velocity. [Pg.379]

Figure 35 Fluid motion in the film and droplet phases. The flow in the film phase is the superposition of the Poiseuille flow and a flow of constant velocity Ug. Due to the nonuniform interfacial surfactant distribution, surface diffusion and convective fluxes appear. Figure 35 Fluid motion in the film and droplet phases. The flow in the film phase is the superposition of the Poiseuille flow and a flow of constant velocity Ug. Due to the nonuniform interfacial surfactant distribution, surface diffusion and convective fluxes appear.
The number pi of passages in the minimal distance n to is, for the stream of atoms of constant velocity Wi and concentration N which we have always considered here,... [Pg.55]

The Accelerated Particle Movement in a Flow of Constant Velocity... [Pg.413]


See other pages where Of constant velocities is mentioned: [Pg.147]    [Pg.176]    [Pg.70]    [Pg.161]    [Pg.102]    [Pg.4]    [Pg.611]    [Pg.132]    [Pg.140]    [Pg.186]    [Pg.186]    [Pg.89]    [Pg.297]    [Pg.128]    [Pg.175]    [Pg.16]    [Pg.67]    [Pg.699]    [Pg.402]    [Pg.62]    [Pg.65]    [Pg.115]    [Pg.358]    [Pg.413]   
See also in sourсe #XX -- [ Pg.195 , Pg.214 ]




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