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UNIVERSITY OF WEST BOHEMIA FACULTY OF MECHANICAL ENGINEERING DEPARTMENT OF POWER SYSTEM ENGINEERING Ratkovská Katarína
32

Ratkovská Katarína

Feb 23, 2016

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UNIVERSITY OF WEST BOHEMIA FACULTY OF MECHANICAL ENGINEERING DEPARTMENT OF POWER SYSTEM ENGINEERING. Ratkovská Katarína. JET ENGINES. HISTORY. 17.12.1903 Orvill Wright and Wilburom Wright - first controlled flight. 1935 Frank Whitley - patented principle of jet engines - PowerPoint PPT Presentation
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Page 1: Ratkovská Katarína

UNIVERSITY OF WEST BOHEMIAFACULTY OF MECHANICAL ENGINEERING

DEPARTMENT OF POWER SYSTEM ENGINEERING

Ratkovská Katarína

Page 2: Ratkovská Katarína

JET ENGINES

Page 3: Ratkovská Katarína

HISTORY• 17.12.1903 Orvill Wright and Wilburom Wright

- first controlled flight

Page 4: Ratkovská Katarína

• 1935 Frank Whitley- patented principle of jet engines

• 27.8.1939 Hans von Ohain- HeS – 3B jet engine

W - 1

Page 5: Ratkovská Katarína

He - 178

Page 6: Ratkovská Katarína

TYPICAL ENGINE CUTS

0 – 1 engine intake1 – 2 compressor2 – 3 main combustion chamber3 – 4 gas turbine4 – 5 exhaust system

Page 7: Ratkovská Katarína

VK 1 engine with radial

compressor

Page 8: Ratkovská Katarína

RD 33

Page 9: Ratkovská Katarína

MiG-29

Page 10: Ratkovská Katarína

BASIC PARAMETERS

• Engine thrust [N]- It's more important parameter, which is

characterized a jet engines with direct reaction

[N ]Where:- mass flow rate []- – output gas velocity []- – air speed []

Page 11: Ratkovská Katarína

• Engine thrust [N]

mass flow rate - gas [] mass flow rate - air [] – output gas velocity [] – air speed []

Page 12: Ratkovská Katarína

• Engine performance P[W] turbo-prop engines

- – propeller thrust [N]- – air speed- – propeller efficiency [1]

Page 13: Ratkovská Katarína

Turboprop engine TP 100

Page 14: Ratkovská Katarína

TS - 21

- Turboshaft engine with free gas turbine.- It is starter of R-27F2M-300 engines.

Page 15: Ratkovská Katarína

Mig 23 - FLOGGER

Page 16: Ratkovská Katarína

• Air mass flow rate[] - Quantity of air that flows through the engine

in second.

=

• m – air mass [kg]• t – time [s]

Page 17: Ratkovská Katarína

• Specific engine thrust Fm []

• Hour fuel consumption [kg.]

- Fuel flow rate.

Page 18: Ratkovská Katarína

• Total compressor pressure ratio - Define ratio between total pressure on compressor

output to total pressure on compressor input.

– total air pressure on compressor input [Pa] – total air pressure on compressor output [Pa]

Page 19: Ratkovská Katarína

COMPRESSOR TYPESCentrifugal flow compressors

Page 20: Ratkovská Katarína

AXIAL FLOW COMPRESSORS

Page 21: Ratkovská Katarína

• Total absolute temperature before turbine stage [K]

- is the temperature value on combustion chamber output before turbine stage.

T3T = t3T+273,15 [K]

• Total absolute temperature behind turbine stage [K]

T4T = t4T+273,15 [K]

Page 22: Ratkovská Katarína

THERMAL CYCLE

• Jet engines are reactive engines witch works with atmospheric air. Purpose of air in this case is:

- Basic component of working media in thermodynamic cycle- Oxygen included in air is used during chemical reaction of burning- Accelerated air (in case of engines with direct reaction) create trust

Page 23: Ratkovská Katarína

SfJE - Ideal thermal cycle

Page 24: Ratkovská Katarína

SfJE with afterburner – ideal thermal cycle

Page 25: Ratkovská Katarína

WORK OF IDEAL THERMAL CYCLE

Page 26: Ratkovská Katarína

• In p-V diagram

• In T-s diagram

1,,. . kgJWWW adkomadexid

121. . kgJqqWid

WORK OF IDEAL THERMAL CYCLE

Page 27: Ratkovská Katarína

Ideal expansion work of gas:

1013

3

5353,

.11...11..

1..

kgJe

TcTc

TTTcTTcW

pp

ppadex

Page 28: Ratkovská Katarína

EFFICIENCY OF IDEAL CYCLE - SfTJE

• Quality of transformation of input heat “” to work “” is described by thermodynamic efficiency “”

111111..

1.1..

10

0

1

ee

eeTce

eTc

qW

p

pi

t

Page 29: Ratkovská Katarína

DEPENDENCE OF “” BY “”

Page 30: Ratkovská Katarína

WORK OF IDEAL THERMAL CYCLE - SfTJE

0

3

.

1

. TTe

opt

opt

0dedWi

1.2

0

31.2.

TT

opt

Page 31: Ratkovská Katarína

CONCLUSION

• Work of ideal cycle in thermodynamics is characterized by efficiency .

• Thermal efficiency of cycle depend by pressure ratio π and temperature ration /

Page 32: Ratkovská Katarína

DISCUSSION

QUESTIONS