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Objectives of the present work. Develop a methodology to study multidimensional effects of wave rotors and apply to NASA four-port pressure exchanger using commercial CFD code Predict the fuel-air mixing in an internal combustion wave rotor (ICWR)Determine key parameters that affect the fuel-air d
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1. Prediction And Design Of Fuel-Air Mixing in a Combustion Wave Rotor Using Two-Dimensional Unsteady Moving Mesh Flow Computation Arnab Banerjee
Mechanical Engineering
IUPUI
MSME Thesis Presentation
Advisor: Prof. Razi Nalim
November 27, 2005
2. Objectives of the present work Develop a methodology to study multidimensional effects of wave rotors and apply to NASA four-port pressure exchanger using commercial CFD code
Predict the fuel-air mixing in an internal combustion wave rotor (ICWR)
Determine key parameters that affect the fuel-air distribution in a wave rotor and improve understanding to obtain desired fuel distribution
3. Introduction Wave Rotor: A device for energy exchange efficiently within fluids of differing densities by utilizing unsteady wave motion
Two configurations studied here
NASA four-port pressure exchanger
Internal combustion wave rotor (ICWR)
4. NASA four-port pressure exchanger Turbine inlet pressure is 15% -20% more than compressor exit pressure ideally
Increased overall engine thermal efficiency and specific work
5. Internal Combustion Wave Rotor (ICWR)
6. 2D & 3D view of wave rotor
7. Pre- and Post- Processing Package Developed in-house by Khalid (2004-05)
Hexagonal unstructured grid
Parametric geometry and grid
Grid and geometry stored in small portable files
Variable port/rotor channel counts and shape
Tailored grid clustering
Imports and exports STAR-CD files
3D and “unwrapped” simultaneous view
Runs easily on laptops (windows)
8. Results of two grid packages
9. Past 1-D simulations
10. Past 2-D simulations
11. Solution Methodology Arbitrary Sliding Interface
MARS (Monotone Advection Reconstruction Scheme) – 2nd order accurate
PISO predictor-corrector algorithm
Corrector stages below specified limit (20) indicates convergence reached for specified residual tolerance
12. Arbitrary Sliding Interface
13. Estimating Artificial Diffusivity Use shock tube with different grid resolutions representing the range of CFD simulations carried out
Calculated artificial diffusion from known equation
Compared these values with physical diffusivity in simulations
15. Hardware Resources AVIDD Linux Cluster
Huge Scratch space
Batch Scheduling
Accessible from outside of network (SSH)
Dual CPU PC
Quick turnaround
Debugging
Manual decomposition
16. Methodology Development Welch (1997) simulated NASA 4-port configuration using code validated against experiment
2D unsteady, laminar, compressible, ideal gas, adiabatic walls, no leakage
IUPUI simulation
Same as above and also included passage to passage leakage
17. Grid Resolution
19. Computed instantaneous total temperature
21. Computed instantaneous static temperature contours showing close up view of passage gradual opening process and 2D flow features
22. Fuel-Air Mixing in an Internal Combustion Wave Rotor (ICWR) Include multidimensional effects
Include turbulence modeling (k-epsilon with wall functions)
Include species transport equations
Include property dependence on mixture composition and temperature
Examine the effect of fuel-air distribution on combustion
23. Boundary Conditions - from Alparslan, Nalim and Synder (2004)
Inlet was specified as total conditions
Total pressure at inlet segments ? 109 KPa
Total temperature at inlet segments ? 291 K
Exit port was specified as static conditions
Static pressure at ? 72 KPa
Hot gas injection port
Static temperature ? 600 K
Combustion using one-step reaction combined time scale model
C3H8 + 5O2 ? 3CO2 + 4H2O
the reaction time scale is the sum of the dissipation and chemical kinetics time scales.
24. ICWR geometry
25. Grid Resolution
27. Non-Combustion Pressure waves for time converged solution
29. Shape of fuel-air interface Fuel-air interface at the middle of the inlet has expected skew (tangential non-uniformity) due to passage opening to fuel over time
Fuel-air interface forming at the beginning of the inlet is less skew
The skew of interface maybe something useful to control
30. Close-up view of first inlet segment opening to rotor passage“tufts indicate flow vectors relative to rotor”
31. Developing more uniform fuel-air interface All the inlet port segments have the same total pressures
First inlet segment has higher static pressure than other segments due to higher pressure from rotor passage
Thus absolute velocity in the first inlet segment is lower than other segments
Non-axial relative velocity forces more fuel into the trailing side of the passage
32. Reduced total pressure at first inlet segment
33. Increased total pressure at first inlet segment
34. Results of varying total pressure at first inlet segment Decreasing total pressure at first inlet segment has backflow ? not helping in the fuel distribution shape in other passages
The fuel-air interface is skewed similar to fuel air interaction in middle of inlet ports
Increasing total pressure at first inlet segment causes no backflow
The fuel-air interface is skewed too
35. Adding air-buffer as first inlet segment
36. Results from air buffer case The non-axial relative velocity in the first inlet segment which doesn’t have fuel ? doesn’t influence the filling of fuel in passage
The fuel-air surface is skewed similar to the fuel-air surface in the middle of the inlet port
38. Setup - combustion case Boundary conditions obtained from 1-D detonation model.
The present case is studied for deflagration and 2-D ? incompatible with 1-D BCs
Modified BCs to velocity ? high flow causing choke exhaust
Used case to study general effect of fuel-air distribution on combustion
41. Results of combustion case Premature ignition when fuel-air mixture from first three inlet segments due to hot products from previous cycle
Presence of air buffer as first inlet segment prevents premature combustion
42. Skewness (tangential non-uniformity)
43. Comparison of penetration of fuel for both configurations
44. Conclusions Developed methodology for 2-D wave rotor simulation
Compared with published 2-D simulation results by Welch (1997)
Used commercial solver for CFD simulations
Applied methodology to ICWR
Studied multidimensional factors affecting fuel-air distribution on few configurations
With no air buffer – skew can be affected by timing, total inlet conditions
Premature ignition can be prevented by air-buffer
To do a higher fidelity simulation, of a given wave rotor configuration, include a finer grid based on NASA 4-port wave rotor and geometry and boundary conditions obtained from one-dimensional deflagration.