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Combustion Team
Faculty Advisors:
Dr. GuillaumeDr. GuillaumeDr. Wu Dr. Wu Dr. BoussalisDr. BoussalisDr. LiuDr. Liu
Sara Esparza
Cesar Olmedo
Student Researchers:
1NASA Grant URC NCC NNX08BA44A
Agenda
Background, Theory & Input Parameters
Supersonic Combustion
Mach Number & Operational Envelope
Engine Design & Optimization
Design Components
Design Component Analysis
Numerical Analysis and Subsequent Design Modification
Future Work
Timeline
2NASA Grant URC NCC NNX08BA44A
Governing Equations:Motion of Fluid Substances
• Conservation of Mass
fTpDt
Dv
0 vDt
D
pRT
WdUQ
SJxumxMt
)(
1
)(
1
)(
1
• Conservation of Momentum
• State Equation – Ideal Gas Law
• Conservation of Species
• Conservation of Energy
3NASA Grant URC NCC NNX08BA44A
Combustion
Combustion stoichiometryIdeal fuel/ air ratio
Recommended fuels for scramjetsHydrogen - most common EthyleneKerosene
Only oxidizer is airIn scramjets, combustion is often unstableEquivalence ratio
Should range from 0.2 - 2.0 for combustion to occur with a useful time scale Lean mixture ratio below 1.0Rich mixture ratio above 1.0
tricstoichiome
actual
AF
AF
4NASA Grant URC NCC NNX08BA44A
Equivalence and Swirl Ratios:Specific to Combustion Projects
0H2
yN
476.3xCO3.76NO
4HC 22222yx
yx
yx
• Equivalence Ratio, φ
axial
tagential
G
GS
• Swirl Number, S
5NASA Grant URC NCC NNX08BA44A
Supersonic Combustion
6NASA Grant URC NCC NNX08BA44A
Supersonic CombustionResearch & Product Description
Design, fabricate and test supersonic combustion ramjet in supersonic wind tunnel
Research and improve upon high speed flow, mixing, and combustion stability
7NASA Grant URC NCC NNX08BA44A
Speed of Sound
TRa
γ = adiabatic index R = gas constant T = air temperature
At sea level a=768 mi/hr or 343m/s
The rate of travel of a sound wave through air under specified conditions
8NASA Grant URC NCC NNX08BA44A
Mach Number & Operational Regimes – Subsonic, Transonic, Supersonic & Hypersonic Flight
SubsonicBoeing 747
0<Ma<1Ma =.85
SupersonicF15 Fighter Plane
1.0<Ma<3.0Ma =1.5
HypersonicSpace Shuttle
Ma>3Ma =25
9NASA Grant URC NCC NNX08BA44A
Reversed Alligator Inlet Design Chosen
Multiple Inward Turning Scoop Reversed Inlet Design Chosen
10NASA Grant URC NCC NNX08BA44A
CompressorTurn Angle 18deg
Variable CowlMach decrease from heat input
DiffuserExit angle12.29 deg
Integrated Scramjet Vehicle
11NASA Grant URC NCC NNX08BA44A
Exit Mach Number One Dimensional Flow
12NASA Grant URC NCC NNX08BA44A
Shockwaves Traverse through Engine Two-Dimensional Flow
13NASA Grant URC NCC NNX08BA44A
Shock and Turn Angles
14NASA Grant URC NCC NNX08BA44A
Prandtl Meyer Expansion Waves
15NASA Grant URC NCC NNX08BA44A
Integrated Scramjet Vehicle
M∞ = 4.5
M = 2.6
M = 2.1
M = 4.2
16NASA Grant URC NCC NNX08BA44A
Supersonic mixing
Ignition and flame holding are a first order issue for supersonic combustion
17NASA Grant URC NCC NNX08BA44A
Supersonic Combustion – Mixing & Stability
Supersonic Mixing
Development of mixing length
Development of injector location
Development of ignition location
Development of flame holder
18NASA Grant URC NCC NNX08BA44A
CombustionTurbulent Shear Mixing
19NASA Grant URC NCC NNX08BA44A
Turbulent mixing at supersonics speeds
Micro-mixing
20NASA Grant URC NCC NNX08BA44A
CombustionTurbulent Shear Mixing
• Mean velocity profile combines– Prandtl’s number
– Turbulent kinematic viscosity
– Time average characteristics of turbulent shear
3
431
11
yy
r
r
U
U
c
Micro-mixingFuel vortexFuel wave
21NASA Grant URC NCC NNX08BA44A
CombustionTurbulent Shear Mixing
Shear layer width – Two methods
m
m
lB
xr
rB
1
16 2
Local shear layer width for turbulent shear mixing
xr
rCm
1
1
Recent researchCδ is a experimental constant
22NASA Grant URC NCC NNX08BA44A
CombustionTurbulent Shear Mixing
• Density effects on shear layer growth – compressible flow
• Based on constant but different densities
• A density ratio, s, is derived
• s can be calculated once stagnation pressure and stream velocities are known
2
1
2
12
1
21
22
11
2222
2111
2
1
2
1
2
1
UU
UU
U
Us
PP
UUU
UUU
uPuP
s
c
c
c
c
23NASA Grant URC NCC NNX08BA44A
CombustionTurbulent Shear Mixing
• Convective velocity for the vortex structures
• With compressible flow using isentropic stagnation density equation changes to
2
22
1
11
1222
212
11
2/12
2/11
2
1
1
2
11
2
11
1
a
UUM
a
UUM
MM
s
UsUU
cC
cC
CC
c
24NASA Grant URC NCC NNX08BA44A
CombustionTurbulent Shear Mixing
• Density correct expression for shear layer growth including compressibility effects
213
1
2/1
2/1
2/1
2/11
8.2.)(
1129.1
1
11
12
1
1
1)(49.
cMc
cm
eMf
rr
rsrs
rs
rs
rCMf
x
25NASA Grant URC NCC NNX08BA44A
CombustionTurbulent Shear Mixing
26NASA Grant URC NCC NNX08BA44A
Supersonic Mixing Efficiency
• Mixing Efficiency
1,179.0 072.1 0 eC
b
Lmm
F
1,333.3 0204.1 0 eC
b
Lmm
A
27NASA Grant URC NCC NNX08BA44A
Fuel
• Hydrogen – Has four times the energy of aviation fluid, less polluting emissions
– Safety
• Silane– SiH4 is a pyrophoric that can be added to hydrogen to decrease ignition
delay time of the fuel
– Concentrations are between 5-20% by volume
– Useful when the combustion chamber is short or combustion chamber temperature is low
– Safety Concerns : is highly explosive easily ignites with air and 9.6k ppm is very lethal in just a four hour exposure
• JP–10 Fuel– Liquid Fuel used in First air-breathing Scramjet
28NASA Grant URC NCC NNX08BA44A
Combustion Stability
Flame velocity
Flame length
Recirculation
Detonation
Auto-ignition
Back pressure
29NASA Grant URC NCC NNX08BA44A
Design Approaches
Mach 2
Simple
Mutable
Flexible
Rapid prototype
ZPrinter powder, high temperature inner shell
Cheap
MFDCLab sufficient
Mach 4.5
Complex
Fixed shape
Not flexible
Machining
Stainless steel, high nickel steel, copper, aluminum
Expensive
Needs supersonic wind tunnel
30NASA Grant URC NCC NNX08BA44A
Combustion Performance & Design
Detonation – shockwave induced combustion
Flame holder – use back pressure to control flame stability
COSMOSWorks Flame Holder Inlet Mach 4.5Velocity contours shows recirculation zones
31NASA Grant URC NCC NNX08BA44A
Injector Pressure Profile
32NASA Grant URC NCC NNX08BA44A
Fuel Injector Holds the Flame
33NASA Grant URC NCC NNX08BA44A
Size Coolant Delivery Mechanism according to
Pressure and Temperature
Pc Mechanism
700 tubes
1310 tubes
1378 channels/tubes
1486 channels/ablative
2994 channels/tubes
34NASA Grant URC NCC NNX08BA44A
Proof of Concept
• Test supersonic leading edges
• Develop and simulate computational fluid dynamics run of overall design and individual components
• Compare and analyze test data
• Achieve supersonic combustion throughout the engine
35NASA Grant URC NCC NNX08BA44A
Conclusion
Sustain supersonic combustion
Increase fuel and air mixing time
Vary input parameters to create knowledge and testing base
Key components
Multiple combustion chambers
Cavities
Flameholders
Development of a doctoral dissertation
36NASA Grant URC NCC NNX08BA44A
Textbook References
Anderson, J. “Compressible Flow.”
Anderson, J. “Hypersonic & High Temperature Gas Dynamics”
Curran, E. T. & S. N. B. Murthy, “Scramjet Propulsion”
AIAA Educational Series,
Fogler, H.S. “Elements of Chemical Reaction Engineering” Prentice Hall International Studies. 3rd ed. 1999.
Heiser, W.H. & D. T. Pratt “Hypersonic Airbreathing Propulsion”
AIAA Educational Searies.
Olfe, D. B. & V. Zakkay “Supersonic Flow, Chemical Processes, & Radiative Transfer”
Perry, R. H. & D. W. Green “Perry’s Chemical Engineers’ Handbook”
McGraw-Hill
Turns, S.R. “An Introduction to Combustion”
White, E.B. “Fluid Mechanics”.
37NASA Grant URC NCC NNX08BA44A
Journal References
Allen, W., P. I. King, M. R. Gruber, C. D. Carter, K. Y Hsu, “Fuel-Air Injection Effects on Combustion in Cavity-Based Flameholders in a Supersonic Flow”. 41st AIAA Joint Propulsal. 2005-4105.
Billig, F. S. “Combustion Processes in Supersonic Flow”. Journal of Propulsion, Vol. 4, No. 3, May-June 1988
Da Riva, Ignacio, Amable Linan, & Enrique Fraga “Some Results in Supersonic Combustion” 4 th Congress, Paris, France, 64-579, Aug 1964
Esparza, S. “Supersonic Combustion” CSULA Symposium, May 2008.
Grishin, A. M. & E. E. Zelenskii, “Diffusional-Thermal Instability of the Normal Combustion of a Three-Component Gas Mixture,” Plenum Publishing Corporation. 1988.
Ilbas, M., “The Effect of Thermal Radiation and Radiation Models on Hydrogen-Hydrocarbon Combustion Modeling” International Journal of Hydrogen Energy. Vol 30, Pgs. 1113-1126. 2005.
Qin, J, W. Bao, W. Zhou, & D. Yu. “Performance Cycle Analysis of an Open Cooling Cycle for a Scramjet” IMechE, Vol. 223, Part G, 2009.
Mathur, T., M. Gruber, K. Jackson, J. Donbar, W. Donaldson, T. Jackson, F. Billig. “Supersonic Combustion Experiements with a Cavity-Based Fuel Injection”. AFRL-PR-WP-TP-2006-271. Nov 2001
McGuire, J. R., R. R. Boyce, & N. R. Mudford. Journal of Propulsion & Power, Vol. 24, No. 6, Nov-Dec 2008
Mirmirani, M., C. Wu, A. Clark, S, Choi, & B. Fidam, “Airbreathing Hypersonic Flight Vehicle Modeling and Control, Review, Challenges, and a CFD-Based Example”
Neely, A. J., I. Stotz, S. O’Byrne, R. R. Boyce, N. R. Mudford, “Flow Studies on a Hydrogen-Fueled Cavity Flame-Holder Scramjet. AIAA 2005-3358, 2005.
Tetlow, M. R. & C. J. Doolan. “Comparison of Hydrogen and Hydrocarbon-Fueld Scramjet Engines for Orbital Insertion” Journal of Spacecraft and Rockets, Vol 44., No. 2., Mar-Apr 2007.
38NASA Grant URC NCC NNX08BA44A
Acknowledgements
Thanks to the faculty advisors:
Dr. D. Guillaume
Dr. C. Wu
And SPACE Center faculty:
Dr. H. Boussalis
Dr. C. Liu
SPACE Center Students
Combustion Team
Sheila Blaise
Rebecca Winfield
39NASA Grant URC NCC NNX08BA44A
Timeline2009 - 2010
40NASA Grant URC NCC NNX08BA44A
Timeline2010 - 2011
2011 Timeline Excel
Supersonic Combustion Team Timeline: March 2010 - February 2011
2010 2011Student Name MAR APR MAY JUN JUL AUG SEP OCT NOV DEC JAN FEB
Sara Esparza
Duel cavity flame
holder is selected
Engineering Drawing of
Flame Holder
Material Selection for flame
holder (Copper)
CFD analysis of Flame holder
Presentation
Fabrication of Flame Holder
Integration of SECETA and Flame
Holder
Application of Sensors on SECETA
Fabricate Fuel line to Wind
tunnel
Supersonic Wind tunnel
Testing
Set up
fuel lines
in wind tunn
el
Attempt Supersonic
Combustion
Gather Data
Attempt Multiple
combustion Chamber
Determine thrust of engine
Determine Combustion
time
Developed cost to
determined Budget
First cavity is adjustableDetermined if Budget can be
obtained
Cesar Olmedo
Duel cavity flame
holder is selected
Engineering Drawing of
Flame Holder
Material Selection for flame
holder (Copper)
CFD analysis of Flame holder
Presentation
Fabrication of Flame Holder
Integration of SECETA and Flame
Holder
Application of Sensors on SECETA
Fabricate Fuel line to Wind
tunnel
Supersonic Wind tunnel
Testing
Set up
fuel lines
in wind tunn
el
Attempt Supersonic
Combustion
Gather Data
Attempt Multiple
combustion Chamber
Determine thrust of engine
Determine Combustion
time
Developed cost to
determined Budget
First cavity is adjustableDetermined if Budget can be
obtained
Alonzo Perez Engineering Drawing of Flame Holde
Attempt Supersonic
Combustion
Gather Data
Attempt Multiple
combustion Chamber
Determine thrust of engine
Determine Combustion
time
41NASA Grant URC NCC NNX08BA44A