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2/3/2015 1 Gas Turbine and Jet Propulsion Xin Zhang Room: 2577C. Telephone: (852) 3469-2220 Email: [email protected] 1.1. Introduction to propulsion

1.1 Introduction to Propulsion

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  • 2/3/2015

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    Gas Turbine and Jet Propulsion

    Xin ZhangRoom: 2577C. Telephone: (852) 3469-2220Email: [email protected]

    1.1. Introduction to propulsion

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    Why propulsion Aircraft is a feasible alternative for long distance travel (>3 hrs)

    Aircraft is a good option for high-speed travel (>300km/h)

    What is propulsion To push forward or drive an object forward

    Thrust is generated through the application of Newton's ? law of action and reaction.

    In an aircraft engine a working fluid is accelerated and the reaction to this acceleration produces a thrust force on the engine

    Net force on CV = Momentum flux out Momentum flux in

    Thrust is produced if there is an increase in momentum of the working fluid

    Momentum

    Control Volume (CV)

    Momentum in Momentum out

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    The environmental impact of air transport

    Environmental noise a local nuisance near airports*, a major constraint on the growth of air transport

    NOx emissions a threat to local air quality and public health

    Carbon emissions (fuel burn) a contributor to global warming .. currently 3% of global carbon emissions + contrails

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    * En route noise may be an issue with new propulsion systems

    WHO guidelines for community noise

    Noise-induced hearing impairment

    Interference with speech communication

    Sleep disturbance

    Cardiovascular and physiological effects

    Mental health effects

    effects of noise on performance

    effects of noise on residential behaviour and annoyance

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    Newtons laws of motion

    First law

    Second law

    Third law

    When viewed in an inertial reference frame, an object either remains at rest or continues to move at a constant velocity, unless acted upon by an external force.

    The vector sum of the forces on an object is equal to the mass m of that object multiplied by the acceleration vector of the object

    When one body exerts a force on a second body, the second body simultaneously exerts a force equal in magnitude and opposite in direction on the first body

    = 0 = 0= =

    Lateral and longitudinal accelerations

    Longitudinal acceleration:

    Lateral acceleration:

    sV

    tVa

    =

    =211

    RVa

    22=

    R

    V1

    V2

    s

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    Classification of gas turbine engines

    There are four main types of aerospace propulsive devices:

    Piston engine Gas turbine engines Airbreathing Ramjets Rockets

    The list is given in ascending order of vehicle flight speed.

    Method of thrust generation

    Engine type Working fluid

    Cycle Thrust generation

    Piston Air Intermittent Propeller, rotor

    Gas turbine Air Continuous Jet, fan, propeller, rotor

    Ramjet Air Continuous Jet

    Rocket Various Continuous Jet

    In addition to thermodynamic cycle, the method of thrust generation can differ for each of these engines

    Newtons 2nd law of motion

    Force = rate of change of momentum

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    Variants and hybrids

    Obvious examples Turbine powered

    Turbojet Turbofan Turboprop and turboshaft Propfan

    Non-continuous combustion Less obvious hybrids

    Turboramjet

    Turborocket

    Ram-rocket

    Liquid air cycle engines (LACE)

    Q. What dictates choice of engine types?

    A1: Vehicle mission vs. engine capability

    The vehicle must operate within a flight corridor which is governed by Lift limit (loss of lift at high altitude and/or low speed) Aerodynamic force limit (excessive structural loading at high speed and

    low altitude) Temperature limit (excessive aerodynamic heating at high speed)

    Engine capability is determined by

    Ability to provide sufficient thrust Ability to operate with adequate fuel economy, as indicated by, for

    example, the engines specific impulse:

    = where FN is the thrust, is the total mass flowrate of stored propellant

    (fuel+oxidiser), and is the Earths gravitational constant at sea level.

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    Q. What dictates choice of engine types?

    A2: Economics Development cost Purchase cost Operation cost

    A3: Reliability and safety Mean time between overhaul (MTBO) Mean time between failure (MTBF)

    A4: Technology and legislation Aerothermodynamics Materials Emissions Others (fuels, lubrication, cooling).

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    Rocket propulsion

    O2

    Fuel

    Combustionchamber

    Propelling nozzle

    Rocket propulsion

    O2

    Fuel

    Combustionchamber

    Propelling nozzle

    Working fluid is the exhaust products (no momentum in)

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    Propeller propulsion

    Air

    Propeller propulsion

    Air

    Working fluid is Air (momentum inflow from incoming air)

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    Lorins concept for jet propulsion (1913)

    Air Fuel Exhaust

    Combustionchamber Propelling nozzle

    Lorins concept for jet propulsion (1913)

    Air Fuel Exhaust

    Combustionchamber Propelling nozzle

    Working fluid is Air & Exhaust gases

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    Lorins concept for jet propulsion (1913)

    Air Fuel Exhaust

    Combustionchamber Propelling nozzle

    No rotating parts ~ Ramjet principle

    Requires high speed flight velocity

    Vin

    Combustionchamber

    Compressor

    Exhaust

    Turbine Propelling nozzle

    Vjet

    Whittles turbo-jet 1930(Co-inventor Ohain 1936)

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    Vin

    Combustionchamber

    Compressor

    Exhaust

    Turbine Propelling nozzle

    Vjet

    Whittles turbo-jet 1930(Co-inventor Ohain 1936)

    The compressor and the turbine are turbomachines: Machines which transfer energy from or to working fluid through the fluid-dynamic action of rotating blade-rows

    Vin

    Combustionchamber

    Compressor

    Exhaust

    Turbine Propelling nozzle

    Thrust ~ mass flow x (Vjet Vin)

    Vjet

    Whittles turbo-jet 1930(Co-inventor Ohain 1936)

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    Gas turbine cycle

    P3

    P2

    2

    4

    5

    3

    Entropy

    Turbine entry temperature

    2 3 45

    Work input to actual compressor is greater than work input for the ideal one!Actual turbine produces less work than the reversible, adiabatic one!

    =

    Gas turbine cycle

    P3

    P2

    Entropy

    Turbine entry temperature

    = WorkoutHeatin = Heatin HeatoutHeatin

    Heat in

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    Gas turbine cycle

    P3

    P2

    Entropy

    Turbine entry temperature

    = WorkoutHeatin = Heatin HeatoutHeatin

    Heat out

    Gas turbine cycle

    P3

    P2

    Entropy

    Turbine entry temperature

    = WorkoutHeatin = Heatin HeatoutHeatin

    Useful work+Lost work

    Lost work

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    Gas turbine cycle

    P3

    P2

    Entropy

    Turbine entry temperature

    = WorkoutHeatin = Heatin HeatoutHeatin

    Useful work+Lost work

    Lost work

    Gas turbine cycle

    Entropy

    Turbine entry temperature

    = WorkoutHeatin = Heatin HeatoutHeatin

    Useful work+Lost work

    Lost work

    As turbine entry temperature (TET) and pressure ratio rises useful work to heat input rises

    Higher efficiency

    Higher specific work ~ thrust : weight

    Pressure ratio