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Page 1: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

1 Challenge the future

Introduction to Aerospace Engineering

Lecture slides

Page 2: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

18-9-2011

Challenge the future

DelftUniversity ofTechnology

Introduction to Aerospace EngineeringAE1101ab - Propulsion

Prof.dr.ir. Jacco Hoekstra

Page 3: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

18-9-2011

Challenge the future

DelftUniversity ofTechnology

Page 4: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

3AE1101 Introduction to Aerospace Engineering | xx

11Propulsion

We do not use Anderson’s ch 9 (too difficult for now), but these slides for 1101ab

Page 5: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

4AE1101 Introduction to Aerospace Engineering | xx

The propulsion perspective…

Gee Bee model ‘R’ Sportster

Page 6: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

5AE1101 Introduction to Aerospace Engineering | xx

Wright Flyer required an engine that did not exist

• Engine: Wright 4-cylinder 12 - 20 hp water-cooled inline• Weight 150 lbs, 200 lbs with fuel

Page 7: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

6AE1101 Introduction to Aerospace Engineering | xx

“Even considering the improvements possible …… the gas turbine could hardly be considered a feasible application to airplanes, mainly because of the difficulty with the stringent weight requirements.”Gas turbine committee, US National Academy of Sciences (1940)

Same statement is currently often heard for electrical propulsion!

Page 8: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

7AE1101 Introduction to Aerospace Engineering | xx

Theory

T

V0 (m/s)

L

D

W

aircraft- and rocket propulsion≡ reaction propulsion

Page 9: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

8AE1101 Introduction to Aerospace Engineering | xx

You can see this principle in the water rocket.

Page 10: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

9AE1101 Introduction to Aerospace Engineering | xx

Theory of air breathing engines

V0 (m/s) VJT

For rocket propulsion we use Tsjolkovski’s rocket equation (covered 1101cd)!

[ / ]m kg s

Page 11: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

10AE1101 Introduction to Aerospace Engineering | xx

Theory

0( )jT m V V→ = −

Momentum Equation:

V0 (m/s) VJ

T

dIFdt

=

I m V= ⋅ (En: linear momentum, NL: impuls)

(Newton's second law) [kg m/s2](=N)

[kg/s · m/s] (=N)

dVF m m adt

→ = ⋅ = ⋅

Page 12: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

11AE1101 Introduction to Aerospace Engineering | xx

What Flew or Is Flying Around?

Human Powered Electrical Engine Airbreathing Engine Rocket Engine

Propeller Propulsion Jet Propulsion

Piston Engine TurboProp TurboShaft

Propeller Propulsion

TurboFan TurboJet Ramjet Scramjet

Jet Propulsion

Page 13: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

12AE1101 Introduction to Aerospace Engineering | xx

Propeller Propulsion

Counter Rotating Rotating

Page 14: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

13AE1101 Introduction to Aerospace Engineering | xx

Propeller Propulsion

Counter Rotating Rotating

Fixed Pitch Variable Pitch Ducted Fan

Page 15: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

14AE1101 Introduction to Aerospace Engineering | xx

Propeller Theory

ω (rad/s)

r(m)

Vrot(m/s)

R(m)

rVrot Ω= ω·

Page 16: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

15AE1101 Introduction to Aerospace Engineering | xx

Propeller Theory: Blade is like a wing

ω (rad/s)

r(m)

SR(m)

T

Useful force: T Thrust (pointing at us)

Loss: S Side force (like drag for wing)

Page 17: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

16AE1101 Introduction to Aerospace Engineering | xx

Twisted for constant angle of attack

ω (rad/s)Large Twist Small Twist

Constant angle of attack!

Page 18: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

17AE1101 Introduction to Aerospace Engineering | xx

t

T

t+Δt

T

Δs

Available Power for thrust

Work Performed: W= T·Δs [Nm or J]

Available Power: Pa= = T·V [Nm/s, J/s or W]ΔtT·Δs

Page 19: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

18AE1101 Introduction to Aerospace Engineering | xx

tTt+ΔtT

Δs=VΔt

Available Power

Net available Power for thrust: Pa= T V

Brake (shaft) Power: Pbr

PbrPropulsive Efficiency: η= = T V

Pbr

Pa

Speed is V

Page 20: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

19AE1101 Introduction to Aerospace Engineering | xx

Airbreathing EnginesThey all work the same way..........in principleOnly the details differ.

They all have 4 stages:1. Intake 2. Compression3. Work4. Exhaust

Page 21: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

20AE1101 Introduction to Aerospace Engineering | xx

Piston Engines

What is used in Aviation ?• 2 Stroke Engine• 4 Stroke Engine• Wankel Engine• Diesel Engine

ObsoleteCommon‘New’Expected

Page 22: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

21AE1101 Introduction to Aerospace Engineering | xx

Combustion Cycle (Otto Cycle)

.dW F ds p A ds= = Δ ⋅ ⋅

Quasi-static !!

( )upper lowerdW p p dV= −max

min

( )V

upper lowerV

W p p dV= −∫

T1

T2

Page 23: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

22AE1101 Introduction to Aerospace Engineering | xx

Working Cycle (4 stroke engine)

p

V

RTpV =INTAKE COMPRESSION

WORK EXHAUST

Page 24: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

23AE1101 Introduction to Aerospace Engineering | xx

Working Cycle (4 stroke engine)INTAKE COMPRESSION WORK EXHAUSTp

V

Work [J]

Page 25: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

24AE1101 Introduction to Aerospace Engineering | xx

Throttle control

Page 26: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

25AE1101 Introduction to Aerospace Engineering | xx

Piston Engines: In-Line

Page 27: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

26AE1101 Introduction to Aerospace Engineering | xx

Piston Engines: Boxer

Page 28: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

27AE1101 Introduction to Aerospace Engineering | xx

Piston Engines

In-Line

Radial

V Boxer

Page 29: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

28AE1101 Introduction to Aerospace Engineering | xx

Continuous Combustion

Airbreathing EnginesPropeller Propulsion Jet Propulsion

Piston Engines TurboPropTurboShaft

TurboFan TurboJet RamJet

TurboCompound

Engine

TurboEngine

With Propfan

By-PassEngine

Turbo-RamJet RamRocket

ScramJet

AftFan

Page 30: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

29AE1101 Introduction to Aerospace Engineering | xx

Continuous CombustionINTAKE COMPRESSION WORK EXHAUST

Page 31: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

30AE1101 Introduction to Aerospace Engineering | xx

Continuous CombustionINTAKE COMPRESSION WORK EXHAUST

Page 32: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

31AE1101 Introduction to Aerospace Engineering | xx

Ramjet

Page 33: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

32AE1101 Introduction to Aerospace Engineering | xx

Pure Jet Engine

Page 34: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

33AE1101 Introduction to Aerospace Engineering | xx

Jet Engine With Afterburner

Page 35: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

34AE1101 Introduction to Aerospace Engineering | xx

Trading Exhaust Power for Shaft Power

INTAKE COMPRESSION WORK EXHAUST

Page 36: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

35AE1101 Introduction to Aerospace Engineering | xx

TurboProp/TurboShaft

Page 37: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

36AE1101 Introduction to Aerospace Engineering | xx

Turboprop

Page 38: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

37AE1101 Introduction to Aerospace Engineering | xx

Turboshaft

Page 39: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

38AE1101 Introduction to Aerospace Engineering | xx

Trading Exhaust Power for Shaft PowerINTAKE COMPRESSION WORK EXHAUST

Page 40: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

39AE1101 Introduction to Aerospace Engineering | xx

TurboFan

Page 41: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

40AE1101 Introduction to Aerospace Engineering | xx

This is quite a large duct fan (high bypass flow) Why?

Page 42: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

41AE1101 Introduction to Aerospace Engineering | xx

Engine development 1950-1980

Higher Bypass-ratio

Bypass airflow (Cold) Core airflow (Hot)

More air, less velocity

Higher propulsive efficiency

c

h

mBm

=.

.

Can you explain why?

Page 43: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

42AE1101 Introduction to Aerospace Engineering | xx

Jet efficiency

( )2 2102j jP m V V= −

( )( )( )

0 0

10 02

j

j j

m V V V

m V V V V

−=

+ −

V0 (m/s) Vj

m (kg/s).

221

oVm 221

jVm

What is efficiency of jet?

aj

j

PP

η =

Jet efficiency

( )0

2 2102 j

TVm V V

=−

0

2

1j

jVV

η =+

0( )jT m V V= − Pa= T V0

What is effect onengines of previous slide?

Page 44: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

43AE1101 Introduction to Aerospace Engineering | xx

Example of this effect0

2

1j

jVV

η =+

In words: by lowering exhaust speed, the efficiencygoes from 31% to 54% (amount of energy used for propulsion)

Page 45: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

44AE1101 Introduction to Aerospace Engineering | xx

And also less noise due to lower Vj

Page 46: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

45AE1101 Introduction to Aerospace Engineering | xx

Engine Development

Very big

Page 47: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

46AE1101 Introduction to Aerospace Engineering | xx

Engine Applications• Single engine training aircraft:

• Low subsonic passenger aircraft:

• Concorde (Supersonic):

• Helicopter:

• Piston engine

• Turboprop

• Pure (straight) jet

• Turboshaft or piston

Page 48: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

47AE1101 Introduction to Aerospace Engineering | xx

Two or Four Engines? ETOPS• Extended Twin OPerationS

• Engines Turning Or Passengers Swimming

• Twin engined airliners restricted to a maximum diversion time (120 to 207 minutes) dependant on strict maintenance and aircraft type.

• Crossing some parts of the atlantic and pacific ocean and bothpoles is (currently) restricted to four engined airliners.

Page 49: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

48AE1101 Introduction to Aerospace Engineering | xx

Future air breathing EnginesPropeller Propulsion Jet Propulsion

Piston Engines TurboPropTurboShaft

TurboFan TurboJet RamJet

TurboEngine

With Propfan

Turbo-RamJet RamRocket

ScramJet

AftFan

By-PassEngine

TurboCompound

Engine

Page 50: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

49AE1101 Introduction to Aerospace Engineering | xx

Engines

• Pratt & Whitney – PW127B• Turboprop• Aircraft: Fokker 50• Power: 2750 SHP (x2)

2050 kW (x2)

Page 51: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

50AE1101 Introduction to Aerospace Engineering | xx

Engines

• Rolls Royce - Tay 650• Low bypass Turbofan• Aircraft: Fokker 100• Thrust: 67 kN (x2)• Fan Diameter: 1.14 m• Length: 2.4 m• Bypass Ratio: 3.07

Page 52: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

51AE1101 Introduction to Aerospace Engineering | xx

Engines

• General Electric – GE90-115B• High bypass turbofan• Aircraft: Boeing 777• Thrust: 512 kN (x2)• Fan Diameter: 2.95 m• Length: 4.55 m• Bypass Ratio: 9

Largest and highest thrust engine in the world!

Page 53: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

52AE1101 Introduction to Aerospace Engineering | xx

Engines

• Rolls Royce – Trent 900• High bypass turbofan• Aircraft: Airbus 380• Thrust: 311 kN (x4)• Fan Diameter: 2.95 m• Length: 4.55 m• Bypass Ratio: 8.5

Page 54: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

53AE1101 Introduction to Aerospace Engineering | xx

Engines

• Rolls Royce / SnecmaOlympus 593

• Pure Turbojet• Aircraft: Concorde• Thrust: 170 kN* (x4)

*Using afterburner (take-off and transonic)

Page 55: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

54AE1101 Introduction to Aerospace Engineering | xx

Links

• www.howstuffworks.com• www.rollsroyce.com• www.ge.com

Page 56: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

55AE1101 Introduction to Aerospace Engineering | xx

Beechcraft Super King Air 200

Page 57: Introduction to Aerospace Engineering - TU Delft OCW Introduction to Aerospace Engineering 3 | xx 11 Propulsion We do not use Anderson’s ch 9 (too difficult for now), but these slides

56AE1101 Introduction to Aerospace Engineering | xx

Pratt & Whitney PT6A-41

• Per engine: 850 Shaft horse power, Pbr=634 kW

• Maximum speed at sea level: