THREE DIMENSIONAL FLAME PROPAGATION ABOVE LIQUID FUEL POOLS
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1 THREE DIMENSIONAL FLAME PROPAGATION ABOVE LIQUID FUEL POOLS By Jinsheng Cai, Feng Liu, and William A. Sirignano Mechanical and Aerospace Engineering University of California, Irvine Supported by NASA Microgravity Program and Coordinated with NASA Glenn experimental work of H.D. Ross and F.J. Miller
2 OBJECTIVES
3 CONFIGURATION 3-D Liquid Fuel Pool in wind tunnel floor. Igniter modelled as a hot gas pocket with a linear temperature increase to 1700 K in 0.01s.
4 ASSUMPTIONS & CONDITIONS
5 DIFFUSION MODELS
6 NUMERICAL METHOD
7 CASES INVESTIGATED 3D, 0-g, Hot Tunnel Floor (Insulated) 3D, 1-g, Hot Tunnel Floor (Insulated) 3D, 0-g, Cold Tunnel Floor (Heat Sink) 3D, 1-g, Cold Tunnel Floor (Heat Sink) 2D, 0-g 2D, 1-g Other Parameters: Propanol Fuel, Opposed air velocity = 30cm/s; Pool depth = 2mm; Initial Fuel Temperature = 11 to 19 o C.
8 EFFECT OF DIFFUSION MODEL 30 cm/s opposed flow. Flame speed and frequency increase with pool temperature. Pulsations occur at both 1-g and 0-g. Fast oxygen diffusion accounts for increased flame speed.
9 3D VS. 2D COMPARISON Hot Tunnel Floor, 0-g, 30cm/s Flame speed and frequency increase with pool temperature.
10 FLAME POSITION VS. TIME Hot Tunnel Floor, 0-g, 30cm/s Flame speed and frequency increase with pool temperature.
11 FLAME POSITION VS. TIME Hot Tunnel Floor, 1-g, 30cm/s Flame speed and frequency increase with pool temperature. Pulsations occur at both 1-g and 0-g.
12 FLAME POSITION VS. TIME Cold Tunnel Floor, 0-g and 1-g 30 cm/s opposed flow. Flame speed and frequency increase with pool temperature. Pulsations occur at both 1-g and 0-g.
13 FLAME POSITION VS. TIME Hot Floor, Cold Floor, and 2D
14 Top View Fuel Consumption Rate Slow phase, t=2s Fast phase, t=1.8s 13 o C, pulsating case, 1-g, y=1mm. Cold Tunnel Floor. Flame tails lie along pool edge.
15 13 o C, pulsating case, 1-g, t=1.8s. Cold tunnel floor. Cross View Fuel Consumption Rate x/l =.69 x/l =.75
16 Temperature Contours & Velocity Vectors Slow Flame Phase 1g, t=2.0s, z=0. Recirculation zone forms allowing fuel vapor accumulation.
17 Temperature Contours & Velocity Vectors Fast Flame Phase 1g, t=1.8s, z=0. Less recirculation, more hot gas expansion.
18 Cross View - Velocity Vectors & Temperature Contours Slow Phase 13 o C, 1g, t=2s. Cold floor. x/l= 0.68, recirculation.
19 Cross View - Velocity Vectors & Temperature Contours Fast Phase 13 o C, 1g, t=1.8s. Cold Floor. x/l= 0.69; expansion near flame front. x/l=.75, recirculation.
20 Liquid Velocity t=1.8s, fast phase t=2s, slow phase 13 o C, 1g, t=1.8s. Cold floor. Surface tension plus buoyancy causes recirculation.
21 Velocity & Temperature in Symmetry Plane 13 o C, 0-g, t=2.3s, slow phase. Forced convection together with surface tension causes recirculation.
22 Cross View - Velocity Vectors & Temperature Contours Slow Phase 13 o C, 0g, t=2.3s. Cold floor. x/l= No side recirculation without buoyancy.
23 CONCLUSIONS Pulsations are found at both 0-g and 1-g with forced convection. Recirculation zone is key to mechanism for pulsation. Fuel vapor concentration increases during slow phase. Flammability limits are extended. Flame speed and pulsation frequency increase with initial fuel temperature. Improved diffusion model predicts faster propagation and uniform-rate spread / pulsating spread boundary moves to lower initial temperature.
24 CONCLUSIONS (continued) Three-dimensional spread rate exceeds twodimensional spread rate due to increased influx of oxygen. Increase in side heat losses reduces pulsating flame spread rate but has minor effect on uniform spread rates Flame front curves around pool edge extending along and setting over the pool edge. In 1-g case, buoyancy causes side vortices to form in pulsating spread.
25 Top View Fuel Consumption Rate 13 o C, pulsating case, 0-g, t=1.74s, y=1mm. Cold Tunnel Floor. Flame tails along pool edge are short.
26 Cross View, Behind Flame Fuel Consumption Rate 13 o C, pulsating case, 0-g, t=1.74s, x/l=.73. Cold Tunnel Floor.
27 Fuel Consumption Rate in Symmetry Plane 13 o C, 0-g, t=1.74s, Cold Floor
28 Velocity & Temperature in Symmetry Plane 13 o C, 0-g, t=1.74s. Flame remains close to surface in absence of buoyancy.
29 Cross View - Velocity Vectors & Temperature Contours 13 o C, 1-g, t=1.7s, x/l=.725. Cold floor. Vortex on side.
30 Cross View, Behind Flame Fuel Consumption Rate 13 o C, pulsating case, 0-g, t=1.74s, x/l=.80. Cold tunnel floor.
31 FLAME POSITION VS. TIME Symmetry Plane Hot floor, 30cm/s, 1-g, 13 o C
32 FLAME POSITION VS. TIME Edge of Pool Hot floor, 30cm/s, 1-g, 13 o C
33 3D 0, 1g
34 Cross View - Velocity Vectors & Temperature Contours 13 o C, 0-g, t=1.74s, x/l=.73. Cold floor. No vortex on side in absence of buoyancy.
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