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QinetiQ/D&TS/WPNS/PUB0701309
www.QinetiQ.com
April 2007
© Copyright QinetiQ limited 2007
QinetiQ Proprietary
Modelling the Ignition of Modular ChargesClive Woodley & Steve Fuller
A presentation to: 42nd Guns & Missiles Conference
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Contents
01 Background
02 Validation
03 Simulations
04 Conclusions & future work
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01Background
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01 Charge design – why UPCS?
Existing inventory replaced with 1 module
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01 Charge design – advantages of UPCS
• Current charges− Not fully IM compliant
− Not cleared for A1/C2 climatic conditions
− Wasteful – decremental system
− Costly & L10 can’t routinely be used for training
− Often remain in WMR until they ‘life out’
• With UPCS− Same charges are used in training as are deployed for war fighting
− Training simplified/more realistic
− Substantial cost savings can be achieved through incremental system
− Logistic burden reduced
− Autoloader compatible
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01 Modular charges – the problem being addressed
Safety & performance are important requirements – linked to ignition
• Pressure waves eliminated or minimised and consistent
• Simultaneous ignition along length of charge
• Combustible cartridge cases present barrier to flamespread along the propellant bed
• Modules act as projectiles!
-20
-10
0
10
20
30
0 5 10 15 20 25
Time (ms)
Pres
sure
diff
eren
ce (M
Pa)
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01 Modelling approach - QIMIBS
2D mortar code
• Developed initially with MOD funding
• Developed further using QinetiQ funding
• Details presented at 22nd
International Symposium on Ballistics
• Ability to represent internal solid boundaries
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02Validation
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02 Primer only – single module – initial geometry
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02 Primer only – single module
0.000.050.100.150.200.250.300.350.40
0 2 4 6 8 10
Time (ms)
Pre
ssur
e (M
Pa)
QIMIBS P1 QIMIBS P2Round 4 P1 Round 4 P2
0.00
0.05
0.10
0.15
0.20
0.25
0 2 4 6 8 10
Time (ms)
Pre
ssur
e (M
Pa)
QIMIBS P1 QIMIBS P2Round 1 P1 Round 1 P2
1.43g black powder
Max velocity measured: 1.5m/s
Max velocity predicted: 3.2m/s
1.25g NC
Max velocity measured: 2.0m/s
Max velocity predicted: 5.0m/s
Correct trend predicted for pressure and module velocity
Module velocities overpredicted but no account taken of sliding resistance
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02 5 modules - flamespread
0
1
2
3
4
5
6
0 0.2 0.4 0.6 0.8 1
Distance from breech (m)
Tim
e of
firs
t vis
ible
ligh
t (m
s)
Test 1Test 2Simulation
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03Simulations
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03 Simulations
• Single module− Igniter mass & location
− Flash tube diameter & vent hole size
• Three modules
• Five modules
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03 Single module – igniter mass (5g top, 15g bottom)0.5ms 1.0ms
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03 Single module – igniter mass (5g top, 15g bottom)1.5ms 2.0ms
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03 Single module – igniter mass (5g top, 15g bottom)2.5ms 3.0ms
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03 Single module – igniter mass (5g top, 15g bottom)3.5ms 4.0ms
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03 Single module – igniter mass (5g top, 15g bottom)4.5ms 5.0ms
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03 Single module – igniter mass (5g top, 15g bottom)5.5ms 6.0ms
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03 Single module – igniter mass (5g top, 15g bottom)6.5ms 7.0ms
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03 Single module – igniter mass
200
400
600
800
1000
1200
1400
1600
1800
0 5 10 15Time (ms)
Tem
pera
ture
(K)
5g P6 5g P5 5g P415g P6 15g P5 15g P4
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03 Single module – effect of igniter position
0200400
600800
1000
1200
140016001800
0 2 4 6 8 10 12 14 16
Time (ms)
Tem
pera
ture
(K)
Outside P6 Outside P5 Outside P4Inside P6 Inside P5 Inside P4
0200400
600800
1000
1200
140016001800
0 2 4 6 8 10 12 14
Time (ms)
Tem
pera
ture
(K)
Outside P6 Outside P5 Outside P4I/O P6 I/O P5 I/O P4
Outside = outside module but inside flash tube
Inside = inside module but outside flash tube
Modelling indicates better ignition if igniter material is both sides of the flash tube
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03 Single module – effect of flash tube diameter
Modelling indicates better ignition for 26mm flash tube diameter
200
400
600
800
1000
1200
1400
1600
0 2 4 6 8Time (ms)
Tem
pera
ture
(K)
52mm P6 52mm P5 52mm P426mm P6 26mm P5 26mm P4
200
400
600
800
1000
1200
1400
0 1 2 3 4 5 6 7 8
Time (ms)
Tem
pera
ture
(K)
20mm P6 20mm P5 20mm P426mm P6 26mm P5 26mm P4
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03 Single module – effect of flash tube hole size
Modelling indicates better ignition for 6mm flash tube holes
200
400
600
800
1000
1200
1400
0 2 4 6 8Time (ms)
Tem
pera
ture
(K)
14mm P6 14mm P5 14mm P410mm P6 10mm P5 10mm P4
200
400
600
800
1000
1200
1400
0 2 4 6 8Time (ms)
Tem
pera
ture
(K)
6mm P6 6mm P5 6mm P410mm P6 10mm P5 10mm P4
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03 Three modules – initial geometry
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03 Three modules – 10g black powder per module
Taking 600K as the propellant ignition temperature, propellant in 2nd & 3rd modules ignited 0.8ms & 1.7ms after the 1st module
Use another internal ballistics code to predict pressure waves
200
400
600
800
1000
1200
1400
1600
1800
0 2 4 6 8 10 12Time (ms)
Tem
pera
ture
(K)
P1 P2 P3P6 P5 P4
200
400
600
800
1000
1200
1400
1600
1800
0 2 4 6 8 10 12Time (ms)
Tem
pera
ture
(K)
P9 P8 P7P12 P11 P10
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03 Five modules – initial geometry
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03 Five – 10g black powder per module
Igniter in last module not ignited
Module 2 might ignite first
Taking 600K as the propellant ignition temperature, propellant in 2nd , 3rd & 4th
modules ignited 1ms, 2ms & 5ms after the 1st module – use another internal ballistics code for ΔP
200
400
600
800
1000
1200
1400
1600
1800
0 2 4 6 8 10 12 14
Time (ms)
Tem
pera
ture
(K)
P1 P2 P3P6 P5 P4
200
400
600
800
1000
1200
1400
1600
1800
0 2 4 6 8 10 12 14
Time (ms)
Tem
pera
ture
(K)
P9 P8 P7P12 P11 P10
200
400
600
800
1000
1200
1400
1600
0 2 4 6 8 10 12 14
Time (ms)
Tem
pera
ture
(K)
P15 P14 P13P18 P17 P16
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04Conclusions & future work
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04 Conclusions & further work
• QIMIBS has much of the functionality required to model MCS
• Validated for two primers for 1 & 5 modules
• Parameter studies showed
− 5g black powder per module not likely to ignite
− Best position of igniter is both sides of flash tube
− 26mm diameter flash tube better than 52mm and 20mm
− Reducing flash tube vent area predicted to produce better ignition
• Predictions for 5 modules show
− Primer and igniter insufficient to ignite (5th) module adjacent to the projectile
− Module 2 might ignite before module 1
− Possibility of significant ignition delay for 4th module
• 155mm gun firings planned & further modelling
• Conclusions likely to be very dependent on primers and geometries used in this study
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