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252                                             Processing of Plastics

                        adiabatic.  This means that the system is fully insulated to prevent heat gain
                        or loss from or to the surroundings. If this ideal state was to be reached in the
                        extruder it would be necessary for the work done on the melt to produce just
                        the right amount of  heat without the need for heating or cooling. The second
                        ideal case is referred to as isothermal. In the extruder this would mean that the
                        temperature at all points is the same and would require immediate heating or
                        cooling from the barrel to compensate for any loss or gain of heat in the melt.
                        In practice the thermal processes in the extruder fall somewhere between these
                        ideals. Extruders may be run without external heating or cooling but they are
                        not truly adiabatic since heat losses will occur. Isothermal operation along the
                        whole length of  the extruder cannot be envisaged if  it is to be supplied with
                        relatively cold granules. However, particular sections may be near isothermal
                        and the metering zone is often considered as such for analysis.

                        4.2.3 Analysis of Flow in Extruder
                        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.
                          (a)  Drag Flow  Consider the  flow  of  the  melt  between parallel plates  as
                        shown in Fig. 4.7(a).
                          For the small element of fluid ABCD the volume flow rate dQ is given by

                                                  dQ= V*dy*dx                         (4.1)
                        Assuming the velocity gradient is linear, then




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








                        This may be compared to the situation in the extruder where the fluid is being
                        dragged along by the relative movement of the screw and barrel. Fig. 4.8 shows
                        the position of the element of fluid and (4.2) may be modified to include terms
                        relevant to the extruder dimensions.
                        For example               vd = RDN cos $
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