Page 71 - The Jet Engine
P. 71

Exhaust system





                      EXHAUST GAS FLOW

                      4. Gas from the engine turbine enters the exhaust
                      system at velocities from 750 to 1,200 feet per
                      second, but, because velocities of this order produce
                      high friction losses, the speed of flow is decreased by
                      diffusion.  This is accomplished by having an
                      increasing passage area between the exhaust cone
                      and the outer wall as shown in fig. 6-1. The cone also
                      prevents the exhaust gases from flowing across the
                      rear face of the turbine disc. It is usual to hold the
                      velocity at the exhaust unit outlet to a Mach number
                      of about 0.5, i.e. approximately 950 feet per second.
                      Additional losses occur due to the residual whirl
                      velocity in the gas stream from the turbine. To reduce
                      these losses, the turbine rear struts in the exhaust
                      unit are designed to straighten out the flow before the
                      gases pass into the jet pipe.
                      5. The exhaust gases pass to atmosphere through
                      the propelling nozzle, which is a convergent duct,
                      thus increasing the gas velocity (Part 2). In a turbo-
                      jet engine, the exit velocity of the exhaust gases is
                      subsonic at low thrust conditions only. During most
                      operating conditions, the exit velocity reaches the
                      speed of sound in relation to the exhaust gas


















                                                                       Fig. 6-4  A low by-pass air mixer unit.




                                                                       temperature and the propelling nozzle is then said to
                                                                       be 'choked'; that is, no further increase in velocity
                                                                       can be obtained unless the temperature is increased.
                                                                       As the upstream total pressure is increased above
                                                                       the value at which the propelling nozzle becomes
                                                                       'choked', the static pressure of the gases at exit
                                                                       increases above atmospheric pressure.  This
                                                                       pressure difference across the propelling nozzle
                                                                       gives what is known as 'pressure thrust' and is
                                                                       effective over the nozzle exit area. This is additional
                     Fig. 6-3   Gas flow through a convergent-         thrust to that obtained due to the momentum change
                                divergent nozzle.                      of the gas stream (Part 20).

                                                                                                                  61
   66   67   68   69   70   71   72   73   74   75   76