mme.modares.ac.ir
*1
2
- 1 - 2
* 11155-1639
18 :
1395
: 05 1395
: 16 1395
.
76.
101. .
. .
.
1.2
.
0.8.
0.5.
2.
.
Numerical study of a detonation wave structure in annular chamber
Mohammad Farahani
*, Mohammad Badrgoltapeh
Department of Aerospace Engineering, Sharif University of Technology, Tehran, Iran
* P.O.B. 11155-1639 Tehran, Iran, [email protected]
A RTICLE I NFORMATION A BSTRACT
Original Research Paper Received 06 April 2016 Accepted 25 June 2016 Available Online 06 August 2016
Detonation engines are expected to be used as propulsion system in aerospace applications in the future.
Several types of detonation engines are currently under examination, including the rotating detonation engine (RDE). In this work, the feasibility study for design of a laboratory sample RDE which has an annular geometry with diameter of 76 mm has been performed. In this sample, hydrogen and standard air are separately injected into the combustion chamber of detonation engine. First, numerical studies are validated comparing the FLUENT results with the experimental ones. Then, the geometry and equivalence ratio of injection mixture are investigated parametrically. Considering the negligible variations of thermodynamics parameters in the radial direction of flow field to reduce the computational costs, also a 2D model is used for numerical simulations. Three different equivalence ratios were employed. Results show for the case with the equivalence ratio of 1.2, detonation speed, pressure, and temperature behind detonation front is more than the equivalence ratio of 0.8. Also, maximum detonation speed and pressure behind detonation take place in stoichiometric conditions. The parametric study of the chamber length effects was also conducted using a length 0.5 and 2 times of the main chamber. Because the chamber outflow is subsonic at some regions, chamber length change has a significant effect on the engine performance and flow field. The results point out that increasing the chamber length in low injection pressure and high injection pressure leads to increasing and decreasing the height of detonation front, respectively.
Keywords:
Rotating Detonation Engine
Rotating Detonation Combustion Modeling Geometry Design of RDE
2D simulation of RDE
-1 .
.
( )
.
[ Downloaded from mme.modares.ac.ir on 2023-12-10 ]
.
. :
]
1[ 1 . .
.
) .
2
] [ 2,1 .
)
. ( 5-0
.
( )
. .
)
3
(
.
4
.
5) .(
. .
. .
.
] [ 3 .
1Standing Detonation Engine (SDE)
2Pulse detonation engine (PDE)
3Deflagration To Detonation Transition (DDT)
4Rotating Detonation Engine (RDE)
5Continuous Detonation Engine (CDE)
] [ 5,4 .
.
] [ 8-6 .
] [. 7
6
- .
- 95
] [. 9
.
- .
.
.
7
-2
6 Chapman-Jougeaut Velocity (Vcj)
7 Computational Fluid Dynamics (CFD++)
[ Downloaded from mme.modares.ac.ir on 2023-12-10 ]
] [ 10
- .
.
] [. 9 ] [ 11
. )
1
-
2
- ] [ 12 ( .
25-1000
3
- .
- 300 .
25
- . .
-
. - .
.
- . .
. .
1 Richtmyer-Meshkov Instabilities (RMI)
2 Kelvin-Helmholtz Instabilities (KHI)
3 Half-Reaction Zone Length (HRL)
-
] 15-13 [ .
. - -
- -
. .
] [ 16 .
] [ 17 . .
4
] [ 18 .
.
5 6
7
-
.
8
.
. .
4 Large-Eddy Simulation (LES)
5 Vorticity
6 Dissipation
7 Small-Scale Structures
8 Sub-Grid Scales (SGSs)
[ Downloaded from mme.modares.ac.ir on 2023-12-10 ]
. .
. - 600
-
.
. .
-
] [ 19 .
] [ 20 ]
[ 21 ]
[ 22
)
( 1
) ( 1
+ [ ] =
W F G ) S
( 2
=
…
… , =
…
… , =
( )
… ( ) ( … )
0
+
, =
…
… 0 0 0 0 0
) ( 2 )
( G=0
) ( 3
) ( 3
+ =
) ( 4 ) ( 5
) ( 4
=
) ( 5
= )
( 6
) ( 6
=
) ( 7
) ( 7
=
,+
°( ) + | |
2 ) ( 8
) ( 8
= exp( )
k
] [ 19 .
= 1.29
= 368.9 [ J/kg. K]
= 7.5 × 10 [s ]
= 4.794 × 10 [ J/kg]
. .
-3
100
90 . 75
90 0.8
. 60 . 0.4
"
" 1 .
7.7 265
] [. 9
. 0.5
) 0.25
) (
(
. 1
0.25 × 0.5
Fig. 1 Injection schematic and detailed geometry[9]
]
1[
9 CombustionChamber Fuel Injection Manifold
Air Injection Manifold
Injection Section
D
outD
inL
totL
c[ Downloaded from mme.modares.ac.ir on 2023-12-10 ]
1
Table1Comparison of one-dimensional detonation properties at different grid scales
(m/s) (mm) TStatic (K)
PStatic (bar)
0.5 × 1 1110
2904 18.01
0.25 × 0.5 1250
3271 20.29
0.125 × 0.25 1252
3276 20.32
0.0625 × 0.125 1255
3284 20.37
-4 .
"
" 2
-5
1
. 11
] [ 9 .
( )
.
"
" 3 .
.
2
. .
"
" 4
Fig. 2 Conversion of three-dimensional to two-dimensional geometry 2
1pressure outlet
2User Defined Functions (UDF) Fig. 3 Computational domain boundary conditions
3
- 1-5 )
( , , )
(
.
) ( 9
= 0
- 2-5 )
( , , )
(
=
( , , )) ( 10
) ( 10
= 2
1 [1 ( ) ]
- 3-5 )
( , , )
(
) = ( 11
) ( 11
= 2
+ 1
) ( 12
Fig. 4 Different injection conditions based on the local combustion chamber pressure on inlet boundary
4 Detonation Wave
In je ct o r
InjectorIn je ct o r
Fuel / Oxidizer P0P0
P0
P
wP
wP
wInjector
Wall Injector
Wall Detonation Wave Detonation Wave
1) No Injection:
Pw P0
2) Subsonic Injection:
P0 > Pw Pcr
3) Sonic Injection:
Pw Pcr
F u el / O x id iz er
Fuel / OxidizerCombustion Products Outlet
75 (mm) Wall Changed to
Periodic Wall Changed to
Periodic
(H2 + Air) Inlet 95 (mm)
Exhaust
Outer wall
Exhaust
Inlet Inner wall
Outer wall Inner
wall
a a
a
b b
b
[ Downloaded from mme.modares.ac.ir on 2023-12-10 ]
) ( 12
= ( 2 - + 1)
1.7 300
. .
= 1.4074918
= 397.6951729
-6
1 20
.
"
" 5 2
.
( )
-7 -
) ( 13
) ( 13 H + 0.5(O + 3.76N ) H O + 0.5(3.76)N
-8
] [ 9 .
.
] [ 9
2
Table 2 Different region propertise for the initial conditions (K) (bar)
1 3000 10
%100
2 300
%100 1
3 300
%100 1
Fig. 5 Initiation strategy for 2D case
5
.
. .
15 30
. .
"
" 6 ] [ 9
"
" 6 .
4.5 .
) t
pp(
) U
det(
) ( 14
= Combustion Chamber Circumference Time Between Pressure Peaks = .
) ( 14 )
( 15
t
ppU
det. 0.3
. 0.6
"
" 6 .
-9
"
" 7
"
" 8 .
1
. 4
4
1 .
. .
1Rotating Detonation Combustion (RDC)
) ( 15
Error = ±
Combustion Products Outlet
20 (mm)
Product @ 25 (bar) & 3000 (K)
Reactant @1 (bar) & 298 (K) Product @ 1(bar) & 298 (K)
(H2 + Air) Inlet 1 (mm)
[ Downloaded from mme.modares.ac.ir on 2023-12-10 ]
Fig.6Comparison of experimental [9] and numerical results for pressure variations at the outer side wall 15 mm from the inlet boundary
6
] [
9 15Fig.7 Static temperature contour at different times
7 Fig.8 Static pressure contour at different times
8
2
2 3 1
3 .
] [ 23 -
. .
4
) .
"
" 9 .
. .
-
"
" 10
"
" 11 .
.
Time (ms)
P re ss u re (M P a )
2.5 3 3.5 4
0 0.5 1 1.5 2 2.5 3
Time (ms)
P re ss u re (M P a)
2.4 2.6 2.8 3
0 1 2
3 Experimental Data [9]
Present Work (Air - H
2)
[ Downloaded from mme.modares.ac.ir on 2023-12-10 ]
.
.
-10
"
" 12
. 76
. 101
Fig. 9 Detonation-shock combined wave
-
9Fig. 10 Streamlines
10
Fig.11Velocity Vector
11 Fig. 12 Designed RDE geometry
12 RDE
- -11
:
H + 0.5(O + 3.76N ) H O + (O ) + 0.5(3.76)N ) ( 16
= 1.2 :
) ( 17 H + 0.5(O + 3.76N )
H O + (1 )(H ) + 0.5(3.76)N
-12 )
( 18
) ( 18
= × . × 1
( )
) ( 19
) ( 19
= +
2 ) ( 20
3
) ( 20
= 0.03439892946
-13 0.8
1 1.2
.
3
Table 3 Injection pressure and injected mixture properties in numerical simulation for various equivalence ratio
(kg/s)
(kg/s)
(bar)
1 0.39 65.64
1.4075 397.69
1.48143
0.8 1.4073
376.29 1.44105
1.2 1.4076
418.85 1.52029
[ Downloaded from mme.modares.ac.ir on 2023-12-10 ]
.
. 1.2
0.8
.
. 4
-14 0.5
2
. .
50.75 203
.
" 5
" 13
-15
.
. 4
- .
) .
.
. -
4
Table 4 Detonation wave parameters for different equivalence ratios (m/s)
TStatic (K) PStatic (bar)
1 1250
3271 20.29044
0.8 1132
2960 18.93272
1.2 1210
3232 19.53543
Fig.13 Static temperature contour for different lengths of chamber 13
5
Table 5 Detonation parameters for different chamber length
(mm) (mm)
(m/s) TStatic
(K) PStatic
(bar)
50.75 19.142
1168 3185 19.62631
101.5 19.741
1250 3271 20.29044
203 21.667
1420 3465 21.58263
.
0.8 1 . 1.2
1.2 0.8
. . .
0.5
. 2 .
[ Downloaded from mme.modares.ac.ir on 2023-12-10 ]
50.75 . 203
- 16
CDE k
DDT
) ( bar
PDE
RDC RDE
) ( K x
V y
k z
k
) kgm
-1s
-1(
) kgm
-3(
air (x, 0, t) = w C k
mix react ref 0
-17
[1] K. Kailasanath, Review of propulsion applications of detonation waves, AIAA Journal, Vol. 38, No. 9, pp. 1698-1708, 2000.
[2] T. Chao, E. Winterberger, J. Shepherd, On the design of pulse detonation engines, GALCIT Report FM 00-7, 2001.
[3] J. Kindracki, P. Wola ski, Z. Gut, Experimental research on the rotating detonation in gaseous fuels–oxygen mixtures, Shock Waves, Vol. 21, No. 2, pp. 75-84, 2011.
[4] B. Voitsekhovskii, V. Mitrofanov, M. Topchian, Investigation of the structure of detonation waves in gases, Proceedings of The Combustion Institute, Elsevier, Vol. 12, No. 1, pp. 829-837, 1969.
[5] B. Voitsekhovskii, V. V. Mitrofanov, M. Topchiyan, Structure of the detonation front in gases (survey), Combustion, Explosion, and Shock Waves, Vol. 5, No. 3, pp. 267-273, 1969.
[6] D. M. Davidenko, I. Gokalp, A. N. Kudryavtsev, Numerical study of the continuous detonation wave rocket engine, Proceedings of The 15th International Space Planes and Hypersonic Systems and Technologies Conference, Dayton, Ohio, 28 April – 1 May, 2008.
[7] M. Hishida, T. Fujiwara, P. Wolanski, Fundamentals of rotating detonations, Shock waves, Vol. 19, No. 1, pp. 1-10, 2009.
[8] D. A. Schwer, K. Kailasanath, Feedback into mixture plenums in rotating detonation engines, Proceeding of The 50th AIAA Aerospace Sciences Meeting including The New Horizons Forum and Aerospace Exposition, Nashville, Tennessee, January 9-12, 2012.
[9] S.-J. Liu, Z.-Y. Lin, W.-D. Liu, W. Lin, M.-B. Sun, Experimental and three- dimensional numerical investigations on H2/air continuous rotating detonation wave, Proceedings of The Institution of Mechanical Engineers, Part G: Journal of Aerospace Engineering, Vol. 227, No. 2, pp. 326-341, 2013.
[10] S. Zhdan, F. Bykovskii, E. Vedernikov, Mathematical modeling of a rotating detonation wave in a hydrogen-oxygen mixture, Combustion, Explosion, and Shock Waves, Vol. 43, No. 4, pp. 449-459, 2007.
[11] K. Mazaheri, Y. Mahmoudi, M. I. Radulescu, Diffusion and hydrodynamic instabilities in gaseous detonations, Combustion and Flame, Vol. 159, No. 6, pp. 2138-2154, 2012.
[12] Y. Mahmoudi, K. Mazaheri, S. Parvar, Hydrodynamic instabilities and transverse waves in propagation mechanism of gaseous detonations, Acta Astronautica, Vol. 91, pp. 263-282, 2013.
[13] Y. Mahmoudi, K. Mazaheri, Triple point collision and hot spots in detonations with regular structure, Combustion Science and Technology, Vol.
184, Nos. 7-8, pp. 1135-1151, 2012.
[14] K. Mazaheri, Y. Mahmoudi, M. Sabzpooshani, M. I. Radulescu, Experimental and numerical investigation of propagation mechanism of gaseous detonations in channels with porous walls, Combustion and Flame, Vol. 162, No. 6, pp. 2638-2659, 2015.
[15] Y. Mahmoudi, K. Mazaheri, High resolution numerical simulation of triple point collision and origin of unburned gas pockets in turbulent detonations, Acta Astronautica, Vol. 115, pp. 40-51, 2015.
[16] M. Arienti, J. E. Shepherd, The role of diffusion in irregular detonations, Proceedings of The 4th Joint Meeting of The US Sections of The Combustion Institute, Philadelphia, Pennsylvania, 2005.
[17] S. Singh, J. M. Powers, S. Paolucci, Multidimensional Detonation Solutions from Reactive Navier-Stokes Equations, Proceedings of The 37th AIAA Aerospace Sciences Meeting and Exhibit, Reno, Nevada, January 11-14, 1999.
[18] Y. Mahmoudi, N. Karimi, R. Deiterding, S. Emami, Hydrodynamic instabilities in gaseous detonations: comparison of Euler, Navier–Stokes, and large-eddy simulation, Journal of Propulsion and Power, Vol. 30, No. 2, pp.
384-396, 2014.
[19] F. Ma, J.-Y. Choi, V. Yang, Thrust chamber dynamics and propulsive performance of single-tube pulse detonation engines, Journal of Propulsion and Power, Vol. 21, No. 3, pp. 512-526, 2005.
[20] T.-H. Yi, J. Lou, C. Turangan, B. C. Khoo, P. Wolanski, Effect of nozzle shapes on the performance of continuously rotating detonation engine, Proceedings of The 48th AIAA Aerospace Sciences Meeting Including the New Horizons Forum and Aerospace Exposition, Orlando, Florida, January 4-7, 2010.
[21] S. Ye-Tao, W. Jian-Ping, Change in continuous detonation wave propagation mode from rotating detonation to standing detonation, Chinese Physics Letters, Vol. 27, No. 3, p. 034705, 2010.
[22] L. Shi-Jie, L. Zhi-Yong, S. Ming-Bo, L. Wei-Dong, Thrust vectoring of a continuous rotating detonation engine by changing the local injection pressure, Chinese Physics Letters, Vol. 28, No. 9, p. 094704, 2011.
[23] T. Fujiwara, S.-i. Tsuge, Quasi-onedimensional analysis of gaseous free detonations, Journal of the Physical Society of Japan, Vol. 33, No. 1, pp.
237-241, 1972.
[ Downloaded from mme.modares.ac.ir on 2023-12-10 ]