THEORY OF GAS TRUBNINE ENGINE
Gas
Turbine Engines used for aircraft propulsion are broadly speaking jet-producing
devices where a working fluid undergoes a series of thermodynamic processes.
These processes are, if it is taken ideally, isentropic compression (in air
inlet diffuser and compressor), heat addition (in combustion chamber),
isentropic expansion (in turbine and propelling nozzle). Thermodynamic cycle
for gas turbine engines comprising these processes is the Joule/Brayton
Cycle. Ref: Figure 1.1 (a).
Although
the diagram in Figure 1.1 (a) is a closed cycle, aero engines works
actually on open cycle as it is clear in Figure 1.1 (b).
Figure
1.1
Objective
of this cyclic performance of the working fluid is to produce a net propulsive
force that is used by the aircraft for its flight through the atmosphere
overcoming the drag force. Different types of engines use this working fluid
differently to have the same end result.
When a propeller turbine is
used, the net shaft work (W34 + W12) is simply
supplied to the airscrew (i.e. propeller). If propulsion is by jet, the turbine
is required to supply merely the compressor work and it uses only part of the
expansion to atmospheric pressure, from 3 to 5. The remaining expansion, from 5
to 4, occurs in the propulsion nozzle. Ref. Figure 1.1(b).
Cyclic processes consisting the Brayton cycle are
executed in different and separate working zones or sections as illustrated in Figure 1.2. These sections are the basis
of constructional build up of a turbine engine.
Figure 1.2
The mechanical arrangement of the gas turbine engine is
simple, for it consists of only two main rotating parts, a compressor and a
turbine, and one or more combustion chambers. To these three basic parts are added intake at the front and an
exhaust unit at the rear. See Figure 1.3 illustrating a gas
turbine engine (turbojet) for the aircraft.
Figure
1.3
How
this arrangement of engine sections, producing propulsive force generates
propulsive force is the theory of jet propulsion.
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