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Flow balancing channels

S based on experiments with water in turbulent flow, in channels icient roughness that there is no Reynolds number effect. The hydraulic radius approach may be used to estimate a friction factor with which to compute friction losses. Under conditions of uniform flow where liquid depth and cross-sectional area do not vary significantly with position in the flow direction, there is a balance between gravitational forces and wall stress, or equivalently between frictional fosses and potential energy change. The mechanical energy balance reduces to tv = g(zx — z2). In terms of the friction factor and hydraulic diameter or hydraulic radius,... [Pg.13]

The assumptions for the heat balance along the channel are (1) steady-state flow (2) constant properties (3) closed channel analysis, no cross-flow between channels (4) channel flow area is constant in the axial direction (5) no boiling in the coolant, single-phase flow (6) constant heat transfer coefficient between the coolant and the heated surface (7) the channel is vertical channel and (8) the volumetric heat generation rate is independent of radial position in the fuel pellet. [Pg.786]

While an experienced die designer may intuitively know where flow balancing is required within a profile, it is difficult to quantify this. This is compounded if a requirement comes along for a profile to be produced from a new material with which the designer has little experience. The ability to simulate the flow distribution based on the geometry and the flow characteristics of the polymer allows the designer to more accurately determine the flow channel details for successful extrusion. [Pg.883]

In current manifold design, the aim is to maintain a natural flow balance, i.e., equal flow paths to all nozzles. In line with this condition, the way the channels run in the manifold also depends on the structural layout of the manifold. Figure 4.67 shows some channel layouts that ensures that the natural balance condition is met, and thus also that the cavities are set out parallel to each other. [Pg.155]

Figure 4.67 Nozzle layout and course of HR channels in manifolds with natural flow balance. Some of the designs are two-level... Figure 4.67 Nozzle layout and course of HR channels in manifolds with natural flow balance. Some of the designs are two-level...
Channels in the manifold generally have the same diameter, although there are numerous exceptions. Flow channels linking a distributor charmel to a nozzle may have a smaller diameter adapted to the diameter of the nozzle channel. Channels in tiered manifolds may have diminishing diameters. The diameters of channels in manifolds with rheological flow balance are individually calculated to within 0.1 mm. [Pg.165]

In the classic D-M-E version, the manifold has large-diameter (24-50 mm) drilled flow channels in which cartridge heaters in a tubular body are located. The melt thus flows through an annular channel between 4 and 9 mm wide (see Chapter 1). Because of the heating pipe in the centre of the channel, the channels cannot cross over as in externally-heated manifolds, but must be connected adjacently. Torpedoes must also be connected with a butt joint to the flow channels. This creates certain restrictions as regards the mould cavity arrangement, and it is not easy to achieve a natural flow balance (see Figure 4.91). [Pg.187]

Using constant boundary conditions, the law for balancing is pretty simple In a branching, the melt flows in channels with a velocity proportional to the height h of the channel. This results in different flow path lengths fl, f2 at the same time,... [Pg.48]

Distribution of the melt flow velocity in the flow channel can directly influence the flow balance which is said to be an important factor affecting the final products quality. Fig.7 shows the velocity distribution on the outlet with different metal insert moving rate. It is clearly that the distribution tendency of the melt flow velocity is similar to each other. The maximum velocity symmetrically appears in the left and right sides of the outlet cross-section. The melts flow velocity in the lower part is relatively slower for its longer flow path. In addition, the maximum outlet flow velocity is increasing with the increase of the metal insert moving rate. [Pg.122]

Isothermal Gas Flow in Pipes and Channels Isothermal compressible flow is often encountered in long transport lines, where there is sufficient heat transfer to maintain constant temperature. Velocities and Mach numbers are usually small, yet compressibihty effects are important when the total pressure drop is a large fraction of the absolute pressure. For an ideal gas with p = pM. JKT, integration of the differential form of the momentum or mechanical energy balance equations, assuming a constant fric tion factor/over a length L of a channel of constant cross section and hydraulic diameter D, yields,... [Pg.648]

Assuming laminar flow through the filter channels, the basic equation of filtration as obtained from a force balance is ... [Pg.163]

Available data sets for flow boiling critical heat flux (CHF) of water in small-diameter tubes are shown in Table 6.9. There are 13 collected data sets in all. Only taking data for tube diameters less than 6.22 mm, and then eliminating duplicate data and those not meeting the heat balance calculation, the collected database included a total of 3,837 data points (2,539 points for saturated CHF, and 1,298 points for subcooled CHF), covering a wide range of parameters, such as outlet pressures from 0.101 to 19.0 MPa, mass fluxes from 5.33 to 1.34 x lO kg/m s, critical heat fluxes from 0.094 to 276 MW/m, hydraulic diameters of channels from 0.330 to 6.22 mm, length-to-diameter ratios from 1.00 to 975, inlet qualities from —2.35 to 0, and outlet thermal equilibrium qualities from -1.75 to 1.00. [Pg.305]

At steady flow in a heated micro-channel the conditions at the evaporation front may be expressed by the continuity of mass, thermal fluxes on the interface surface and the equilibrium of all acting forces (Landau and Lifshitz 1959). With reference to the evaporative meniscus the balance equations have the following form (Peles et al. 1998) ... [Pg.383]

Estimates (9.12) and (9.14) effectively reduce the problem of flow in a heated micro-channel to solving a system of one-dimensional mass, momentum and energy balance equations. They have the following form ... [Pg.384]

The time course of an action potential reflects net current flow and thus the balance of open ion channels. The rate of change of membrane voltage is proportional to transmembrane current flow, according to the equation ... [Pg.194]

With decreasing cell size, the temperature difference between the wall of the cell and the eatalyst partiele in the cell would decrease to zero. For sufficiently small cell dimensions, we may assume the two temperatures are the same. In this case, the heat conduction through the wall becomes dominant and affects the axial temperature profile. As the external heat exchange is absent and the outside of the reactor is normally insulated, the temperature profile is flat along the direction transverse to the reactant flow, and the conditions in all channels are identical to each other. The energy balance is... [Pg.686]


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