gas dynamics of variable area ducts

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Gas Dynamics of Variable Area Ducts P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Development of Efficient and Compact Passive Devices….

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Gas Dynamics of Variable Area Ducts. P M V Subbarao Professor Mechanical Engineering Department I I T Delhi. Development of Efficient and Compact Passive Devices…. System of Equaions. Combine conservation, state equations– can algebraically show. - PowerPoint PPT Presentation

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Page 1: Gas Dynamics of Variable Area Ducts

Gas Dynamics of Variable Area Ducts

P M V Subbarao

Professor

Mechanical Engineering Department

I I T Delhi

Development of Efficient and Compact Passive Devices….

Page 2: Gas Dynamics of Variable Area Ducts

0A

dA

V

dV

ρ

0V

dVM

2p

dp

D

fdxM

2 2

22

h

2 γγ

0

V

dV

2

M1

T

dT

TC

q2

22

p

'''

γδ

0T

dT

ρ

p

dp

0V

dV

M

dM

T

dT2

2

2

2

System of Equaions

Page 3: Gas Dynamics of Variable Area Ducts

Combine conservation, state equations– can algebraically show

2

0p

'''

h

22

2

2

2

M1TC

q

A

dA2

D

fdxM

M1

M2

11

M

dMγ

δγ

γ

So we have three ways to change Mach number of a flow

– area change (dA):

– friction: f > 0, same effect as –dA

– heat transfer: heating, q’’’ > 0, like –dA cooling, q’’’ < 0, like +dA

Page 4: Gas Dynamics of Variable Area Ducts

Effect of Shape of duct on Flow

2

0p

'''

h

22

2

2

2

M1TC

q

A

dA2

D

fdxM

M1

M2

11

M

dMγ

δγ

γ

Pure shape effects :

A

dA2

M1

M2

11

M

dM2

2

2

A

dA

1M

M12

M

dM2

2

2

2 γ

A

dA

1M2

M12

M

dM2

1M2

M12M

dM

A

dA

2

2

γ

Page 5: Gas Dynamics of Variable Area Ducts

Pure Shape Effects …..

Page 6: Gas Dynamics of Variable Area Ducts

p

dp1

u

duM2

γ

p

dp1

A

dA

M1

M2

2

γ

ρ

p

dpγ

Subsonic Nozzle Subsonic Diffuser

dA < 0 & M <1So, du > 0 & dp <0

dA > 0 & M <1So, du < 0 & dp>0

A

dA

1M

1

u

du2

T

dT

A

dA

M1

M12

2

γ

Page 7: Gas Dynamics of Variable Area Ducts

Supersonic Diffuser Supersonic Nozzle

dA < 0 & M >1So, du < 0 & dp >0

dA > 0 & M >1So, du >0 & dp<0

p

dp1

u

duM2

γ

p

dp1

A

dA

1M

M2

2

γ

A

dA

1M

1

u

du2

ρ

p

dpγ

ρ

A

dA

1M

M2

2

T

dT

A

dA

1M

M12

2

γ

Page 8: Gas Dynamics of Variable Area Ducts

Generation of High Pressure from Supersonic velocity

p

dpM

u

du 2

γ

p

dp1

M

M1

A

dA2

2

γ

p

dp1

ρ

γ

p

dp1

T

dT

γ

γ

A

dA

1M

1

u

du2

Page 9: Gas Dynamics of Variable Area Ducts

Generation of Supersonic Velocity from Rest

p

dpM

u

du 2

γ

p

dp1

M

M1

A

dA2

2

γ

p

dp1

ρ

γ

p

dp1

T

dT

γ

γ Rocket Nozzle

Page 10: Gas Dynamics of Variable Area Ducts

X – 15 : Hypersonic Research at the Edge of Space

The X-15 was air launched from a B-52 aircraft at about 45,000 ft and speeds upward of 500 mph. The airplane first set speed records in the Mach 4-6 range with Mach 4.43 on March 7, 1961; Mach 5.27 on June 23, 1961; Mach 6.04 on November 9, 1961; and Mach 6.7 on October 3, 1967. It also set an altitude record of 354,200 feet (67 miles) on August 22, 1963, and provided an enormous wealth of data on hypersonic air flow.Aerodynamic heating, control and stability at hypersonic speeds, reaction controls for flight above the atmosphere, piloting techniques for reentry, human factors, and flight instrumentation.

Page 11: Gas Dynamics of Variable Area Ducts

Intake at Design Altitude

p1

p2pthroat

p

p2

p*

p1

Page 12: Gas Dynamics of Variable Area Ducts

0p

dp1

M

M1

A

dA2

2

γAt M=1

Minimum Area = A* : Also called throat

*** AcρρuA

u

RT

ρ

ρ

u

c

ρ

ρ

A

A **

γ

Page 13: Gas Dynamics of Variable Area Ducts
Page 14: Gas Dynamics of Variable Area Ducts

Frictional Adiabatic Flow in A Variable Area Duct

2

0p

'''

h

22

2

2

2

M1TC

q

A

dA2

D

fdxM

M1

M2

11

M

dMγ

δγ

γ0

A

dA2

D

fdxM

M1

M2

11

M

dM

h

22

2

2

2

γ

γ

Constant Mach number frictional flow

h

2

2D

fMA

dx

dA γ