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mme.modares.ac.ir

*1

2

- 1 - 2

* 11155-1639

[email protected]

18 :

1395

: 05 1395

: 16 1395

.

76

.

101

. .

. .

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1.2

.

0.8

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0.5

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2

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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

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.

[ Downloaded from mme.modares.ac.ir on 2023-12-10 ]

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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

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- 95

] [. 9

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6 Chapman-Jougeaut Velocity (Vcj)

7 Computational Fluid Dynamics (CFD++)

[ Downloaded from mme.modares.ac.ir on 2023-12-10 ]

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] [ 10

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] [. 9 ] [ 11

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1

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25-1000

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- 300 .

25

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. - .

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- . .

. .

1 Richtmyer-Meshkov Instabilities (RMI)

2 Kelvin-Helmholtz Instabilities (KHI)

3 Half-Reaction Zone Length (HRL)

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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 ]

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= 1.29

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= 7.5 × 10 [s ]

= 4.794 × 10 [ J/kg]

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Fig. 1 Injection schematic and detailed geometry[9]

]

1

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9 Combustion

Chamber Fuel Injection Manifold

Air Injection Manifold

Injection Section

D

out

D

in

L

tot

L

c

[ Downloaded from mme.modares.ac.ir on 2023-12-10 ]

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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

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Fig. 2 Conversion of three-dimensional to two-dimensional geometry 2

1pressure outlet

2User Defined Functions (UDF) Fig. 3 Computational domain boundary conditions

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=

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= 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

Injector

In je ct o r

Fuel / Oxidizer P0

P0

P0

P

w

P

w

P

w

Injector

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 / Oxidizer

Combustion 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 ]

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) ( 12

= ( 2 - + 1)

1.7 300

. .

= 1.4074918

= 397.6951729

-6

1 20

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( )

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) ( 13

) ( 13 H + 0.5(O + 3.76N ) H O + 0.5(3.76)N

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] [ 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

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15 30

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"

" 6 ] [ 9

"

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4.5 .

) t

pp

(

) U

det

(

) ( 14

= Combustion Chamber Circumference Time Between Pressure Peaks = .

) ( 14 )

( 15

t

pp

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1

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4

1 .

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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)

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Fig.6Comparison of experimental [9] and numerical results for pressure variations at the outer side wall 15 mm from the inlet boundary

6

] [

9 15

Fig.7 Static temperature contour at different times

7 Fig.8 Static pressure contour at different times

8

2

2 3 1

3 .

] [ 23 -

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4

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"

" 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

)

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.

.

-10

"

" 12

. 76

. 101

Fig. 9 Detonation-shock combined wave

-

9

Fig. 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 ]

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.

. 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 ]

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50.75 . 203

- 16

CDE k

DDT

) ( bar

PDE

RDC RDE

) ( K x

V y

k z

k

) kgm

-1

s

-1

(

) kgm

-3

(

air (x, 0, t) = w C k

mix react ref 0

-17

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