Theory Flashcards
Describe the operation of a gas turbine engine
Compressor - Generates low air pressure as it turns which sucks ambient air into the inlet. Airflow is then squezed by the blades in the compressor raising density, pressure and temperature
Combustion Chamber - Fuel is added to form an air-fuel mixture which is burnt at constant pressure to generate high velocity flow
Turbine - Connected to the compressor and converts some kinetic energy into mechanical energy to the drive shaft
Nozzle - Turns remaining kinetic energy into thrust
Gas turbine engines are split into turbojets, turbofans, turboprops, turboshafts and ramjets. Describe each and explain how they’re used
Turbojet and Ramjet - Thrust generated from a fluid jet leaving the aircraft
Turbojet - Rotating compressors compress the airflow, mostly used in supersonic aircraft with operating speeds of less than Mach 3
Ramjet - Uses ram effect for compression, used in supersonic planes and missiles, operates at mach speeds greater than Mach 3
Turbofan/prop/shaft - Adaptation of the turbojet which supplies thrust using fans, propellors or shafts
Turbofan - Used in civil aviation
Turboprop - Used in small Civil aviation and large cargoplanes
Turboshaft - Used in helicopters
Draw a plot of altitude against Mach number for propulsion systems, indicating limitations of different engine types
Accurately Draw plots of how pressure, temperature and velocity change through a gas turbine engine
Lecture 8, page 16
What is bypass ratio and how is bypass air beneficial to the overall efficiency
Bypass ratio is the mass flow rate of air through fans, propellors, or helicopter blades divided by the mass flow rate of air through the gas generator
High Bypass Ratio indicates a larger mass of air accelerated to a lower velocity for a higher propulsive efficiency, which increases overall efficiency.
Use the parametric cycle analysis to derive equations for the specific thrust of an ideal ramjet by using the following steps.
i) Apply the thrust equation to the ramjet
ii) Express the velocity ratio V9/a0 in terms of Mach numbers and
temperatures
iii) Find the exit Mach number
iv) Find the temperature ratio T9/T0
v) Apply the first law of thermodynamics to the combustor
vi) Evaluate the specific thrust
vii) Evaluate the thrust specific fuel consumption
Look at 2017 answers, Q2a
Calculate the specific thrust, thrust specific fuel consumption at the following Mach numbers M0 = 1;3;5
T0 = 217k
gamma = 1.4
Cp = 1.004
hpr = 42800J/kg
Tt4 = 2000k
tR = 1.8 (tau R)
Look at 2017, Q2b
Describe and explain the operational envelope of an ideal ramjet
With higher specific thrust, less fuel is used. Max flight mach number will appear where thrust specific fuel consumption is infinitely close to zero
What is the difference between static and stagnation enthalpy
Static Enthalpy: Represents potential energy of fluid stream per unit mass which doesn’t include kinetic energy. If kinetic energy = 0. The stagnation enthalpy = static enthalpy
Stagnation Enthalpy: Represents total energy of a flowing fluid per unit mass which remains constant in an adiabatic condidtion
On an enthalpy-entropy diagram, how does the actual stagnation state differ from the isentropic stagnation state?
Stagnation fluid is the same for both cases. However, the actual stagnation pressure is lower than the isentropic stagnation pressure since entropy increases due to fluid friction
Explain the principle of a converging-diverging nozzle
When air enters a converging nozzle, Pressure, Temperature and Velocity decrease whilst Mach number increases and density decreases. Pressure reaches critical pressure at the throat.
Assume that air enters the above nozzle at negligible velocity at a pressure, p, of
0.2MPa and temperature, T, of 350K. Assuming isentropic flow, determine the
temperature and pressure of the air at the exit plane before the shock wave that results
in a Mach number, Mx = 2, and also the temperature, pressure, Mach number and
stagnation pressure after the shock wave (Assume P0y/P0x = 0.7209 across a shock
wave)
If the air in part b) had entered with a velocity of 200m/s, what would the temperature
and pressure at the exit plane, before the shock wave have been that resulted in a
Mach number, Mx of 2 (assume Cp = 1005Jkg-1K-1)
Look at 2017 Q3d and e
Discuss the reasons why the thrust power generated by a piston engine propeller combination will be significantly lower than the indicated power derived from the analysis of the otto cycle
TP = npnmncnbIP
These are propulsive, mechanical, cooling and combustion efficiency. These inefficiencies, in addition to the piston pump work being finite leads to thrust power being less than the indicated power
What methods have traditionally been applied to increase piston engine output and what are the associated problems?
Piston engine output can be increased by supercharging
Evaporative cooling: Evaporative cooling of the intake charge by using excess fuel and or water injection. This raises the density, and charge mass fuel flow, and hence power output
increase engine speed - Power output is directly proportional to engine speed. The penalty is increased piston speed and therefore engine wear.
Increasing engine compression ratio - Power output raises in direct relation to bmep. Increased mechanical loading of the engine may degrade its service life.
improve volumetric efficiency - Obtained with multiple valves and manifolds, these designs breathe easier.
Increase number of cylinders - Increases power output and has gone as high as 28 cylinders, however, it becomes very complex and reduces reliability
Describe how propellor pitch angle is determined in relation to angle of attack. What is the advantage to variable pitch propellors?
TA is a function of B, and Ta relies on alpha.
A variable pitch propellor can be continuously varied to maintain maximum efficiency at all flight velocities.
Derive an equation for thrust based on the Rankline-Froude actuator disk model
a = (V2-V1)/V1 V1 = a(V2-V1) V2 = V1(1+a)
b = (V3-V1)/V1 V1 = b(V3-V1) V3 = V1(1+b)
m = rhoV2A = rhoAV1(1+a)
T = m(V3-V1)
T = m(V1(1+b)-V1)
T = rhoAV1(1+a)(V1(1+b)-V1)
T = rhoaV1^2(1+a)b
T = 0.5ArhoV1((1-b^2)-1)
(1+a)b = 0.5((1+b)^2-1)
(1+a)b = 0.5(1+2b+b^2-1)
(1+a)b - 0.5(b^2+2b)
(1+a) = 0.5(2+b)
a = 0.5b
T = rhoAV1^2(1+a)2a
or
T = rhoAV1^2(1+b/2)b
Describe why a ramjet travelling at supersonic velocities may use a diffuser prior to the combustion process
A ramjet without a compressor is a logical evolution of the gas turbine for supersonic flight speeds as the compressor efficiency drops dramatically due to shock wave and boundary layer seperation lesses when the blade tips are near supersonic speeds.
The removal of the gas turbine rotors simplifies the engine mechanically, which eliminates mechanical losses that appear in the gas turbine engine. It also prevents swirling, as in purely axial flow, there are no radial components of the airstream velocity. The tangential velocity would be much larger, which directly contributes to larger thrust generation.
Either graphically or by description, indicate how the following quantities vary through all points from the diffuser to the entry of the conbustion chamber, pressure, temperature, velocity, stagnation pressure, stagnation temperature and density.
The inlet or diffuser slows the air velocity relative to the engine from the flight velocity V0 to a smaller value V3.
This decrease in velocity increases both the static pressure P3 and static temperature T3.
However, the stagnation pressure and temperature remain unchanged for an ideal ramjet engine as the process is assumed isentropic.
Sketch how the geometry of ramjets and scramjets may be used to control the combustion Mach Number
2016 Q1C.
Each have 4 sections.
Scramjet converges 1-2. diverges slightly 2-3, diverges greatly 3-4/
State and describe the function of the four main components of a solid rocket motor
Combustion Chamber - Stores and contains propellant during high pressure burning
igniter - Starts the propellant burning
Solid propellant - Burns and produces gases for propulsion
Nozzle - Expands the combustion product gases to high velocity, thus generating thrust.