Page 46 - The Jet Engine
P. 46

Combustion chambers















































        Fig. 4-1  An early combustion chamber.


        COMBUSTION PROCESS                                various devices for metering the airflow distribution
                                                          along the chamber.
        4. Air from the engine compressor enters the
        combustion chamber at a velocity up to 500 feet per  6. Approximately 20 per cent of the air mass flow is
        second, but because at this velocity the air speed is  taken in by the snout or entry section (fig. 4-2).
        far too high for combustion, the first thing that the  Immediately downstream of the snout are swirl vanes
        chamber must do is to diffuse it, i.e. decelerate it and  and a perforated flare, through which air passes into
        raise its static pressure. Since the speed of burning  the primary combustion zone.  The swirling air
        kerosine at normal mixture ratios is only a few feet  induces a flow upstream of the centre of the flame
        per second, any fuel lit even in the diffused air  tube and promotes the desired recirculation. The air
        stream, which now has a velocity of about 80 feet per  not picked up by the snout flows into the annular
        second, would be blown away. A region of low axial  space between the flame tube and the air casing.
        velocity has therefore to be created in the chamber,
        so that the flame will remain alight throughout the  7. Through the wall of the flame tube body, adjacent
        range of engine operating conditions.             to the combustion zone, are a selected number of
                                                          secondary holes through which a further 20 per cent
        5. In normal operation, the overall air/fuel ratio of a  of the main flow of air passes into the primary zone.
        combustion chamber can vary between 45:1 and      The air from the swirl vanes and that from the
        130:1, However, kerosine will only burn efficiently at,  secondary air holes interacts and creates a region of
        or close to, a ratio of 15:1, so the fuel must be burned  low velocity recirculation.  This takes the form of a
        with only part of the air entering the chamber, in what  toroidal vortex, similar to a smoke ring, which has the
        is called a primary combustion zone. This is achieved  effect of stabilizing and anchoring the flame (fig, 4-3).
        by means of a flame tube (combustion liner) that has  The recirculating gases hasten the burning of freshly

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