Upload
vanquynh
View
218
Download
3
Embed Size (px)
Citation preview
Development of Shock Diffuser for Pulse Detonation Turbine Engines
K. Yoshinaga, T. Ofuka, A. OchiT. Yatsufusa, T. Endo, and S. Taki (Hiroshima univ., Japan)
S. Aoki, and Y. Umeda (Toho Gas Co., Ltd., Japan)
20th International Colloquium on the Dynamics of Explosions and Reactive Systems
McGill University, Montreal, CanadaAugust 1-5, 2005
1
Pulse Detonation Turbine Engine(PDTE)
• A pulse detonation turbine engine (PDTE) is a PDE which drives a turbine for power generation.
• For high turbine efficiency and safety, the pressure history at the turbine inlet should be smoothed enough.
2
shock smoothing
Multi-tube system
Thermal efficiency of an ideal PDTE is higher than that of a conventional gas turbine engine
pinlet
p1
One of the key issues is development of a shock-smoothing device, which should be installed between the combustor and turbine
C3H8-air mixture
3
Function of shock diffuser• Shock diffuser deforms a strong shock wave into a
series of weaker shock waves, or a gradually-rising compression wave in the mean time.
• Because the sound speed becomes higher when the pressure becomes higher, a compression wave deforms into a shock wave as it propagates.
4
The effect of the shock diffuse is intrinsically transient.
Principle of shock diffuser
• A shock wave is divided into several small-wave-front shock waves.
• These shock waves are weakened by wave-front expansion, and merged together with different phases.
5
Shock diffuser (prototype)
• The shock diffuser we developed consisted of the confinement chamber, the diffuser tube, and the multi-step reflector.
6
(Dimensions are in mm)
Diffuser tube
• The V-slit diffuser tube is installed inside the confinement chamber, and the direction of the V-slit is variable relative to the outlet.
‘0’ ‘π/2’ ‘π’
outlet
P3
Confinement chamber
7
Principle of diffuser tube
time
Pres
sure
• A shock wave is weakened by the geometrical expansion of its wave front.
• A shock wave coming out through a narrower portion of the slit is weakened more than that coming out through a wider portion of the slit.
8
At the outlet
Multi-step reflector
各段で長さ変更可能
71 87 100
1x
1x 1x 2x
• The cross-sectional area of each step, which reflects the corresponding portion of a shock wave, is the same.
• The lengths, and , are variable.
9
2x
1x
Before reflection
After reflection
w/o multi-step reflector w/ multi-step reflector
Principle of multi-step reflector
Before reflection
After reflection
A series of weaker shock waves
A strong shock wave
10
Detonation tube for shock diffuser experiments
• The flame speed is measured by the ionization probes I1 and I2.
• The pressure transducer P2 is located in the air-filled portion, where the inert shock wave propagates.
11
(Dimensions are in mm)
Experimental apparatus
Detonation tube Shock Diffuser
outlet
PTPT
PT: Pressure transducer
12
Experimental conditions
• We confirmed detonation propagation in all experiments
13
Mixture White gasoline-airEquivalence ratio 1.1Initial pressure 1atmC-J velocity 1820m/s
Measureddetonation speed 1670±100m/s
Effects of the confinement chamber • Pressure histories at P2 and P3
in the case of confinement chamber only.
14
Effects of the diffuser tube• Pressure histories at P3 in the case of no multi-step reflector.
The first shock wave was diffused
‘0’ ‘π/2’ ‘π’
outlet
P3
15
Effects of the length • Pressure histories at P3 in the case of confinement
chamber, diffuser tube and multi-step reflector.
Reflector lengths:X1=30,60,90mmand X2=130mm
The reflected shock wave was diffused
161x
17
• Pressure histories at P3 in the case of confinement chamber, diffuser tube and multi-step reflector.
Reflector lengths: X1=90mm and X2=130,195,260mm
The best parameters in our experiments were
mmxandmmx
26090,2/
2
1
18Effects of the length 2x
19
• We developed the prototype of a shock diffuser which deforms a strong shock wave into a series of weaker shock waves.
• The shock diffuse was tested by using a simplified pulse detonation engine in a single pulse operation.
• The shock diffuser worked.
Conclusions 20
衝撃波の減衰
体積比約2.2倍PDE本体の後ろにPDEと同じ内径で長さが2.14mの管を継ぎ足したようなもの
2.14m
PDE 体積比約2.2倍
PDE Shock diffuser
1m
ホワイトガソリン特性
化学式
CnHn+2(n=6~9) :83% C5H10, C6H12:12% C6H5(CH3) . C6H4(CH3)2 :5%
沸点 60℃~140℃ 発火点 272℃
爆発限界 1~7(V%)
沸点・発火点が低いためPDEに適している
イオンプローブを設置したところの当量比は約1.1
38.51820 CJCJ MDAISTJANにより計算
衝撃波前後の圧力差 p 11.6 pp2.1,4.1 21 として計算すると
実際の実験では 2.5~6.4)/(1001670 CJCJ MsmD
1)6.5~3.4( pp
ホワイトガソリン特性
2
2 1
2
22
1
22
1
2
22
1111 2
112
)1(CJ
CJCJAA M
MMpp