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Drag flow

An externally imposed pressure gradient may also be present along with the drag flow, as in devolatilizing screw extruders for polymers. [Pg.355]

There is an additional source of bulk flow within a separator vessel, namely a stirrer. It is an integral part of what are considered well-stirred vessels. This flow can take [Pg.355]

Open separators bulk flow parallel to force and CSTSs [Pg.356]


Additioaal uses for higher olefias iaclude the productioa of epoxides for subsequeat coaversioa iato surface-active ageats, alkylatioa of benzene to produce drag-flow reducers, alkylation of phenol to produce antioxidants, oligomeriza tion to produce synthetic waxes (qv), and the production of linear mercaptans for use in agricultural chemicals and polymer stabilizers. Aluminum alkyls can be produced from a-olefias either by direct hydroalumination or by transalkylation. In addition, a number of heavy olefin streams and olefin or paraffin streams have been sulfated or sulfonated and used in the leather (qv) iadustry. [Pg.442]

The drag flow or volumetric conveying capabiUty, for the plastic melt is dependent only on screw speed. A/, and the geometry, M, of the screw ... [Pg.137]

The drag flow is most easily visualized by unwrapping the screw and dragging a flattened barrel surface diagonally across the channel (Fig. 3). [Pg.137]

As discussed in the previous section, it is convenient to consider the output from the extruder as consisting of three components - drag flow, pressure flow and leakage. The derivation of the equation for output assumes that in the metering zone the melt has a constant viscosity and its flow is isothermal in a wide shallow channel. These conditions are most likely to be approached in the metering zone. [Pg.252]

Substituting in (4.1) and integrating over the channel depth, H, then the total drag flow, Qd, is given by... [Pg.252]

The total output is the combination of drag flow, back pressure flow and leakage. So from (4.3), (4.7) and (4.8)... [Pg.256]

If the clearance between the rolls is small in relation to their radius then at any section x the problem may be analysed as the flow between parallel plates at a distance h apart. The velocity profile at any section is thus made up of a drag flow component and a pressure flow component. [Pg.315]

For a fluid between two parallel plates, each moving at a velocity Vj, the drag flow velocity is equal to Vd- In the case of a calender with rolls of radius, R, rotating at a speed, N, the drag velocity will thus be given by InRN. [Pg.315]

The streamlines of this flow are shown by Peters and Smith (12). In this case, the effective thickness of this layer appears to be about equal to the gap with the wall, indicating a pressure flow about equal to the drag flow. It can be calculated that this would increase the maximum shear rate on the fluid passing under the agitator blade by a factor of seven. [Pg.84]

Figure 10. Pure drag flow of polymer syrup in the wall-blade clearance C of an anchor agitator in creeping flow. All velocities relative to the blade (12),... Figure 10. Pure drag flow of polymer syrup in the wall-blade clearance C of an anchor agitator in creeping flow. All velocities relative to the blade (12),...
FIGURE 8.5 Drag flow between parallel plates with the upper plate in motion and no axial pressure drop. [Pg.289]

This velocity profile is commonly called drag flow. It is used to model the flow of lubricant between sliding metal surfaces or the flow of polymer in extruders. A pressure-driven flow—typically in the opposite direction—is sometimes superimposed on the drag flow, but we will avoid this complication. Equation (8.51) also represents a limiting case of Couette flow (which is flow between coaxial cylinders, one of which is rotating) when the gap width is small. Equation (8.38) continues to govern convective diffusion in the flat-plate geometry, but the boundary conditions are different. The zero-flux condition applies at both walls, but there is no line of symmetry. Calculations must be made over the entire channel width and not just the half-width. [Pg.290]

Which is better for isothermal chemical reactions, pressure driven flow or drag flow between flat plates Assume laminar flow with first-order chemical reaction and compare systems with the same values for the slit width (2Y=H), length, mean velocity, and reaction rate constant. [Pg.307]

Over the twentieth century, the mbber industry has developed special rheometers, essentially factory floor instmments either for checking process regularity or for quality control purposes, for instance, the well-known Mooney rheometer (1931), the oscillating disk rheometer (1962), and the rotorless rheometer (1976). All those instmments basically perform simple drag flow measurements but they share a common feature During the test, the sample is maintained in a closed cavity, under pressure, a practice intuitively considered essential for avoiding any wall slip effects. Indeed it has... [Pg.818]

Figure 35.34 shows a slight dependency of the pressure buildup on the calender hne speed, which equals the circumferential roll speed. The general shape of the pressure curve can be understood as follows. A converging drag flow yields a pressure buildup until a barrier has been passed. The material left (=upstream) from the pressure maximum will take part in the roUing bank flow. The material between the pressure maximum and the clearance of the calender flows by means of the drag flow and pressure flow. Each material volume element wfll pass the clearance. At the position where the pressure vanishes the sheet will be taken apart from one of the rolls. [Pg.1004]

Simple pressure/drag flow. Here we treat an idealization of the down-channel flow in a melt extruder, in which an incompressible viscous fluid constrained between two boundaries of infinite lateral extent (2). A positive pressure gradient is applied in the X-direction, and the upper boundary surface at y - H is displaced to the right at a velocity of u(H) - U this velocity is that of the barrel relative to the screw. This simple problem was solved by a 10x3 mesh of 4-node quadrilateral elements, as shown in Figure 1. [Pg.272]

The fraction of the channel that is partially full,/, can be approximated using Fig. 6, which is based on results developed by Squires (1958). The drag flow shape factor Fu is given by... [Pg.72]

Fig. 6. Drag flow shape factors for partially filled channels in a single-screw extruder. Fig. 6. Drag flow shape factors for partially filled channels in a single-screw extruder.
Knowledge of the geometry and mathematical description of a screw Is required to understand the analysis of the functional sections of the screw and the troubleshooting of case studies. In Chapter 1 the geometry and mathematical descriptions are presented. Also In this chapter, the calculation of the rotational flow (also known as drag flow) and pressure flow rates for a metering channel Is Introduced. Simple calculation problems are presented and solved so that the reader can understand the value of the calculations. [Pg.5]

Two driving forces for flow exist in the metering section of the screw. The first flow is due just to the rotation of the screw and is referred to as the rotational flow component. The second component of flow is due to the pressure gradient that exist in the z direction, and it is referred to as pressure flow. The sum of the two flows must be equal to the overall flow rate. The overall flow rate, Q, the rotational flow, 0 and the pressure flow, Qp, for a constant depth metering channel are related as shown in Eq. 1.12. The subscript d is maintained in the nomenclature for historical consistency even though the term is for screw rotational flow rather than the historical drag flow concept. [Pg.13]

Due to the complicated helical screw geometry and the assumption that the down-channel drag flow was a result of matching the screw core velocity to the modeled barrel velocity, the literature assumption that the flow occurs in a rectangular channel is reasonable only if the ratio of channel depth to width is small, that is, a channel with a small aspect ratio (H/W). A schematic of the channel depth to... [Pg.255]

The generalized Newtonian model over-predicted the rotational flow rates and pressure gradients for the channel for most conditions. This over-prediction was caused in part by the utilization of drag flow shape factors (FJ that were too large. Then in order for the sum of the rotational and pressure flows to match the actual flow In the channel, the pressure gradient was forced to be higher than actually required by the process. It has been known for a long time [9] that the power law... [Pg.286]


See other pages where Drag flow is mentioned: [Pg.137]    [Pg.1630]    [Pg.251]    [Pg.252]    [Pg.257]    [Pg.274]    [Pg.275]    [Pg.340]    [Pg.723]    [Pg.83]    [Pg.84]    [Pg.289]    [Pg.12]    [Pg.23]    [Pg.245]    [Pg.254]    [Pg.254]    [Pg.255]    [Pg.255]    [Pg.255]    [Pg.256]    [Pg.258]    [Pg.259]    [Pg.267]    [Pg.272]   
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