5/24/2018 mel341-2h
1/41
THE BIRTH OF JET PROPULSION
P M V Subbarao
Professor
Mechanical Engineering Department
Another Beak Through Idea by an Individual.
5/24/2018 mel341-2h
2/41
Working Principle of Propeller
aircraft
Vm
jet
Vm
5/24/2018 mel341-2h
3/41
Aerofoil Theory of Propeller
aircraftjetthrust VVmF
5/24/2018 mel341-2h
4/41
Anatomy of Propeller
5/24/2018 mel341-2h
5/41
Capacity of Propeller
aircraftjetthrust VVmF
5/24/2018 mel341-2h
6/41
Engines to drive propeller
5/24/2018 mel341-2h
7/41
Need for Alternative Propulsion Method
Dr. Hans von Ohain and Sir Frank Whittle are both
recognized as being the co-inventors of the jet engine. Each worked separately and knew nothing of the other's
work.
Hans von Ohain is considered the designer of the first
operational turbojet engine. Frank Whittle was the first to register a patent for the
turbojet engine in 1930.
Hans von Ohain was granted a patent for his turbojet
engine in 1936. However, Hans von Ohain's jet was the first to fly in
1939.
Frank Whittle's jet first flew in in 1941.
5/24/2018 mel341-2h
8/41
Parallel Invention
Doctor Hans Von Ohainwas a German airplane designerwho invented an operational jet engine.
Hans Von Ohain, started the investigating a new type of
aircraft engine that did not require a propeller.
Only twenty-two years old when he first conceived theidea of a continuous cycle combustion engine in 1933.
Hans Von Ohain patented a jet propulsion engine design
similar in concept to that of Sir Frank Whittle but different
in internal arrangement in 1934.
Hans Von Ohain joined Ernst Heinkel in 1936 and
continued with the development of his concepts of jet
propulsion.
5/24/2018 mel341-2h
9/41
A successful bench test of one of his engines wasaccomplished in September 1937.
A small aircraft was designed and constructed by Ernst
Heinkel to serve as a test bed for the new type of
propulsion system - the Heinkel He178.
The Heinkel He178 flew for the first time on August 27,
1939.
The pilot on this historic first flight of a jet-powered
airplane was Flight Captain Erich Warsitz.
5/24/2018 mel341-2h
10/41
Think Different.
A Royal Air Force officer.
His first attempts to join the RAF failed as aresult of his lack of height, but on his thirdattempt he was accepted as an apprentice in1923.
He qualified as a pilot officer in 1928.
As a cadet Whittle had written a thesisarguing that planes would need to fly at highaltitudes, where air resistance is much lower,in order to achieve long ranges and highspeeds.
5/24/2018 mel341-2h
11/41
Piston engines and propellers were unsuitable for this
purpose.
He concluded that rocket propulsion or gas turbinesdriving propellers would be required.
Jet propulsion was not in his thinking at this stage.
By October 1929, he had considered using a fan enclosed
in the fuselage to generate a fast flow of air to propel aplane at high altitude.
A piston engine would use too much fuel, so he thought of
using a gas turbine.
After the Air Ministry turned him down, he patented theidea himself.
5/24/2018 mel341-2h
12/41
In 1935, Whittle secured financial backing and, with Royal
Air Force approval, Power Jets Ltd was formed.
They began constructing a test engine in July 1936, but itproved inconclusive.
Whittle concluded that a complete rebuild was required,
but lacked the necessary finances.
Protracted negotiations with the Air Ministry followed andthe project was secured in 1940.
By April 1941, the engine was ready for tests. The first
flight was made on 15 May 1941.
By October the United States had heard of the project andasked for the details and an engine.
A Power Jets team and the engine were flown to
Washington to enable General Electric to examine it and
begin construction.
5/24/2018 mel341-2h
13/41
The Americans worked quickly and their XP-59A
Aircomet was airborne in October 1942, some time beforethe British Meteor, which became operational in 1944.
The jet engine proved to be a winner, particularly in
America where the technology was enthusiastically
embraced.
5/24/2018 mel341-2h
14/41
The biggest aircraft
An-225 Cossack 1,322,750 lb L: 275'7";S: 290'
The An-225 Cossack is the largest airplane in the world.
Powerplant:6 ZMKB Progress
D-18 turbofans, 229.5 kN each
5/24/2018 mel341-2h
15/41
The popular Biggest Aircrafts in the World
# Plane Max. Weight Dimensions
1. Hindenburg * 484,400 lb L: 804';D: 135'
2.An-225 Cossack 1,322,750 lb L: 275'7";S: 290'
The An-225 Cossack is the largest airplane in the world.
3.HK-1 Spruce Goose 400,000 lb L: 218'6";S: 320'The HK-1 Spruce Goose has the largest wingspan of all aircraft.
4.Airbus A380F 1,305,000 lb L: 239'3";S: 261'8"
The Airbus A380F is the largest passenger airliner in the world.
5. KM Caspian Sea Monster 1,080,000 lb L: 348';S: 131'
6. An-124 Condor 892,872 lb L: 226'8.5";S:240'5.75"
7. C-5 Galaxy 840,000 lb L: 247'10";S: 222'9"
8. Boeing 777-300ER 775,000 lb L: 242'4";S: 212'7"
9. Airbus A340-600 807,400 lb L: 246'11";S: 208'2"
10. Boeing 747 875,000 lb L: 231'10";S: 211'5"
5/24/2018 mel341-2h
16/41
The world's largest aircraft engine, the GE90-115B
Max. Thrust: 569kN
5/24/2018 mel341-2h
17/41
The fastest Aircraft
X-15 is having a 4,520 mph world speed record.
Fastest manned aircraft.
Not only is the North American X-15 the fastest piloted
aircraft ever, it is the highest flying.
Thrust was obtained from one engine that produced 313kNat maximum altitude.
The North American X-15 was produced to explore the
limits of sub-orbital supersonic flight.
Three were produced. They flew a total of 199 times. The X-15 first took to the sky on June 8, 1959. The last
flight took place on Oct. 24, 1968. A 200th flight was
never made, even after several attempts.
5/24/2018 mel341-2h
18/41
Course Overview
This undergraduate level course teaches theprinciples of jet propulsion.
The primary focus of the course is on the teachingof thermodynamics and Gas dynamics in aircraft
engines. The course provides information that will enable
the engineering analysis of
ramjets and turbine engines and
its separate components including inlets, nozzles,combustion chambers, compressors, and turbines.
5/24/2018 mel341-2h
19/41
Course Objectives
Students successfully completing MEL 341 will get:
A basic understanding of thermodynamic cycles of jetengines.
A basic understanding of the rational behind several typesof jet engines.
A basic understanding of the compressible fluid flow ininlets and compressors and turbines.
A basic understanding of the combustion physics incombustion chambers.
The ability to analyze jet engines; determine propulsionefficiency and design inlets and nozzles.
5/24/2018 mel341-2h
20/41
Course Contents
UNIT- I: PROPULSION
Aircraft Propulsionintroduction -- Early aircraft engines --
Types of aircraft engines -- Reciprocating internal combustion
engines -- Gas turbine engines -- Turbo jet engine -- Turbo fan
engine -- Turbo-prop engine
Aircraft propulsion theory: thrust, thrust power, propulsive and
overall efficiencies -- Problems.
UNIT- II: THERMODYNAMIC ANALYSIS OF IDEAL
PROPULSION CYCLES
Thermodynamic analysis of turbojet engineStudy of subsonic
and supersonic engine models -- Identification and Selection of
optimal operational parameters. Need for further development
Analysis of Turbojet with after burner.
5/24/2018 mel341-2h
21/41
Thermodynamic analysis of turbofan engineStudy ofsubsonic and supersonic systems -- Identification and
selection of optimal operational parameters. Design of fuel
efficient enginesMixed flow turbo fan engineAnalysis
of Turbofan with after burner. Thermodynamic analysis of turbo-prop engine
Identification and selection of optimal operational
parameters.
5/24/2018 mel341-2h
22/41
UNITIII: GAS DYNAMICS OF PASSIVE
COMPONENTS OF TURBO ENGINES
FUNDAMENTALS OF GAS DYNAMICS : Energy equation for a
non-flow process -- Energy equation for a flow process -- Theadiabatic energy equation -- Momentum Equation --Moment of
Momentum equation -- Stagnation Velocity of Sound --Stagnation
Pressure -- Stagnation Density -- Stagnation State -- Velocity of
sound -- Critical states -- Mach number -- Critical Mach number --Various regions of flow.
ANALYSIS OF DIFFUSERS AND NOZZLES: Introduction
study of intakes for subsonic and supersonic engines -- Comparison
of isentropic and adiabatic processes -- Mach number variation --
Area ratio as function of Mach numbers -- Impulse function -- Mass
flow rates -- Flow through nozzles -- Flow through diffusers
Effect of friction -- Analysis of intakes for supersonic engines
intakes with normal shockoblique shocks Study of special
supersonic nozzles and diffusers.
5/24/2018 mel341-2h
23/41
UNITIV: STUDY OF COMPRESSORS
Design and Analysis of compressorsClassificationanalysis of centrifugal compressorsvelocity triangles
design of impellers and diffusersanalysis of axial flow
compressoranalysis of stagecharacterization of stage
design of multistage axial flow compressorPerformances
analysis of centrifugal and axial flow compressors.
5/24/2018 mel341-2h
24/41
UNITV: GAS DYNAMICS OF COMBUSTORS
Stoichimetry of combustioncalculation air-fuel ratio
gas dynamics of combustorsthermal loading factors
design and selection of combustors.
UNITVI: STUDY OF TURBINES
Concept of gas turbineanalysis of turbine stage
velocity triangles and characterization of blades and stages
Design of multistage axial flow turbinePerformance
analysis of turbines.
UNITVI: ADDITIONAL TOPICS
Thermodynamic analysis real turbo engine cycles
performance analysis and thermodynamic optimization.
Introduction to ramjetsstudy of rocket enginesstudy
of missile engines.
5/24/2018 mel341-2h
25/41
Books & References
Jet Propulsion:
Flack, R.D.., Fundamentals of Jet Propulsion,Cambridge University Press,2005.
Baskharone, E.A., Principles of Turbomachinery in Air-Breathing Engines,Cambridge University Press, 2006.
Kerrebrock J.L., Aircraft Engines and Gas Turbines,MIT Press, 1992.
Mattingly, J.D., Elements of Gas Turbine Propulsion,McGraw-Hill Inc.,
1996. Gas Dynamics:
Anderson, J.D., Modern Compressible Flow: With Historical Perspective,McGrawHill, 2002.
Zuker, R.D., and Biblarz, O.,Fundamentals of Gas Dynamics, John Wiley& Sons Inc., 2002.
Thompson, P. A. Compressible Fluid Dynamics.Maple Press Company, 1984. Saad, M.A.,Compressible Fluid Flow,Prentice-Hall, 1993.
Liepmann, H., and A. Roshko.Elements of Gas Dynamics.John WileyPublishers, 1957.
5/24/2018 mel341-2h
26/41
Propulsion - Overview
What is propulsion?
The word is derived from two Latin words:
promeaning before or forwards and
pelleremeaning to drive.
Propulsionmeans to push forward or drive an object forward.
A propulsion system is a machine that produces thrustto push anobject forward.
On airplanes, thrust is usually generated through some application ofNewton's third law of action and reaction.
A gas, or working fluid, is accelerated by a machine, and the reactionto this acceleration produces a force on the engine.
5/24/2018 mel341-2h
27/41
Classification of Propulsion Systems
5/24/2018 mel341-2h
28/41
Jet Propulsion
Operating principle based on Newtons laws of motion. 2nd law - rate of change of momentum is proportional to
applied thrust (i.e.F = m a)
3rd law - every action has an equal and opposite reaction.
5/24/2018 mel341-2h
29/41
Classification of Systems
Only the practical thermo-chemicalcategory will be consideredfurther in this Course.
This may be split into two main sub-categories:
Rockets (Solid or Liquid Propellant);Air Breathers (Ramjet, Turbojet , Turbofan & Turboprop);
along with a Hybrid Ram rocket.
The fundamental operating principle common in all these cases
is , that ofjetor reaction propulsion, i.e. by generating high-
velocity exhaust gases.
5/24/2018 mel341-2h
30/41
Jet Characteristics
Quantities defining a jet are:
cross-sectional area;
composition;
velocity.
Of these, only the velocityis a truly characteristic feature and
is of considerable quantitative significance.
5/24/2018 mel341-2h
31/41
Jet Characteristics of Practical Propulsion Systems
System Jet Velocity (m/s)
Turbofan 200 - 600
Turbojet (sea-level, static) 350 - 600
Turbojet (Mach 2 at 36000 ft) 900 - 1200
Ramjet (Mach 2 at 36000 ft) 900 - 1200
Ramjet (Mach 4 at 36000 ft) 1800 - 2400
Solid Rocket 15002600
Liquid Rocket 20003500
I d i R k
5/24/2018 mel341-2h
32/41
Introduction to Rockets
5/24/2018 mel341-2h
33/41
Solid Propellant Rocket - Basic Operating Features
Four basic components:
motor case, nozzle, solid propellant charge, igniter.
Propellant charge comprises combined fuel & oxidizer.
Gaseous combustion products fill void at high pressure(70 bar typically) and sustains combustion.
Hot gases vent through convergent-divergent nozzle to
provide high-speed (supersonic) propulsion jet.
Gases generated and escape at fixed rate for steady
operation by maintaining constant burning surface area.
5/24/2018 mel341-2h
34/41
Solid Propellant Rocket for GW
Jet velocity: 1500-2600m/s
Most widely used in GW
Short, medium range (< 50 km)
Simple, reliable, easy storage,
high T/W
Rapier
5/24/2018 mel341-2h
35/41
Solid Rocket Features
High propellant density (volume-limited designs).
Long-lasting chemical stability.
Readily available, tried and trusted, proven in service.
No field servicing equipment & straightforward handling.
Cheap, reliable, easy firing and simple electrical circuits.
But
Lower specific impulses (compared with liquid rockets).
Difficult to vary thrust on demand. Smokey exhausts (especially with composite propellants).
Performance affected by ambient temperature.
5/24/2018 mel341-2h
36/41
Liquid Propellant Rocket - Basic Operating Features
Fueland oxidanttanked separately and delivered tocombustion chamber at specific rates and pressures.
Propellant flowrates (and hence thrust) variable upondemand.
Disadvantages compared with solid propellant rockets: increased complication;
Storage problems (usually LOX & LH2 which must bemaintained at very low temperatures);
more costly; reduced reliability.
5/24/2018 mel341-2h
37/41
Liquid Propellant Rocket - Space
Jet velocity: 2000 - 3500m/s.Highest thrust, can be throttled.
Long sustained flight (5mins+).Ariane 5
5/24/2018 mel341-2h
38/41
Space Transportation System(STS)
Travel Cycle of Modern Spacecrafts
5/24/2018 mel341-2h
39/41
Travel Cycle of Modern Spacecrafts
5/24/2018 mel341-2h
40/41
Rentering Space Craft
5/24/2018 mel341-2h
41/41
Major Knowledge Gains Through Gas Dynamics
Simple principles of Gas Dynamics, it was showed thatthe heat load experienced by an entry vehicle was inversely
proportional to the drag coefficient.
The greater the drag, the less the heat load.
Through making the reentry vehicle blunt, the shock waveand heated shock layer were pushed forward, away fromthe vehicle's outer wall.
Since most of the hot gases were not in direct contact withthe vehicle, the heat energy would stay in the shocked gas
and simply move around the vehicle to later dissipate intothe atmosphere.