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Noise mitigation measures to be used for the explosive cladding in ...

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<strong>Noise</strong> <strong>mitigation</strong> <strong>measures</strong> <strong>to</strong> <strong>be</strong> <strong>used</strong> <strong>for</strong><strong>the</strong> <strong>explosive</strong> <strong>cladd<strong>in</strong>g</strong> <strong>in</strong> open airErik Car<strong>to</strong>nFrank van den BergFrits van der Eerden1 Mei 2012


Mitigation Open Air Explosions 1Simulation of <strong>the</strong> blast wave shapeØ 2 m plate of de<strong>to</strong>nat<strong>in</strong>g TNT (0.1 m thick)


Mitigation Open Air Explosions 2Video images of de<strong>to</strong>nation of 50 kg <strong>cladd<strong>in</strong>g</strong> <strong>explosive</strong>without (left) and with water foamFoam:• Reduction <strong>in</strong> peak pressure 28%• Reduction <strong>in</strong> impulse 22%


Mitigation Open Air Explosions 3Overview of presentationObjectiveNumerical techniques & ValidationMuzzle blast <strong>mitigation</strong> (M<strong>in</strong>istry of Defense)Mitigations of open air explosionsConclusions


Mitigation Open Air Explosions 4Objective: Reduction of blast noise from<strong>explosive</strong> <strong>cladd<strong>in</strong>g</strong> <strong>in</strong> open airOpen air explosions burden <strong>for</strong>people <strong>in</strong> <strong>the</strong> surround<strong>in</strong>gsComparable with problems militarytra<strong>in</strong><strong>in</strong>g areaCommon approach not applicable:Shield<strong>in</strong>g <strong>measures</strong> (like <strong>for</strong> traffic) do notworkSound propagation different due <strong>to</strong> highnoise levels (non-l<strong>in</strong>ear effects)


Mitigation Open Air Explosions 5Background: Reduction of “blast” noiseInitialized by:- US-Army- <strong>the</strong> Ne<strong>the</strong>rlands M<strong>in</strong>istry of DefenseObjective: Mitigation of blast noise from large weapons (armor, artillary)- Propagation over large distances- By means of barriers and sound absorb<strong>in</strong>g material- Close <strong>to</strong> <strong>the</strong> source (non-l<strong>in</strong>ear acoustics)gabion or Hesco’s


Mitigation Open Air Explosions 6Numerical hybrid model: FCT – NPE – PEFCT: “Flux-Corrected Transport technique” strong shock waveNPE: “Non-l<strong>in</strong>ear progressive wave equation” weak shock wavePE: “Parabolic Equation” l<strong>in</strong>ear acoustic


Mitigation Open Air Explosions 7Validated at A<strong>be</strong>rdeen Test Centre, MD, USAA large pile of gravel 15x15 m2, 1.5m high, coarse gravel (3cm)Three source locations, C-4 bricks (0.57 kg) 32 … 63 Hz3m1m1.5m-5m+2m


Mitigation Open Air Explosions 8Numerical FCT results (compared <strong>to</strong> measurements)


Mitigation Open Air Explosions 9Case study: Shield<strong>in</strong>g Howitzer blast noise


Mitigation Open Air Explosions 10Case study: Barrier with absorption addedGravel filled gabions/bastions (1 m 3 ):- absorb shock wave energy- suppress ground reflection (<strong>be</strong>h<strong>in</strong>d barrier)


Mitigation Open Air Explosions 11Case study: Barrier with absorption addedTwo movies: blast <strong>mitigation</strong> <strong>be</strong>h<strong>in</strong>d barrier


Mitigation Open Air Explosions 12Calculation results <strong>for</strong> different configurations


Mitigation Open Air Explosions 13A balcony construction <strong>for</strong> <strong>in</strong>creased reduction


Mitigation Open Air Explosions 14Numerical results (sound exposure level, <strong>in</strong> dB)With balcony


Mitigation Open Air Explosions 15Study <strong>to</strong> reduce open airexplosions from <strong>cladd<strong>in</strong>g</strong>“Absorb<strong>in</strong>g” material(broken s<strong>to</strong>nes)


Mitigation Open Air Explosions 16Simulations: 8 variants (500 kg source)Variant 0 = slope without gabionsVariant 1a, 1b = slope with 1m high gabionsVariant 2a,2b,2c = slope with 2m or 3m high gabionsVariant 3a,3b = barrier <strong>in</strong> front of slopeVariant 4, comb<strong>in</strong>ation 3b & 2cvariant2bmicrophones at 80mslope


Mitigation Open Air Explosions 17Levels at end of slope (at 80m, 1/5/10/20m high)Variant0: 12000 PaVariant2b: 6000 PaResult: 6 dB (20log2)Measurement at 90m: 174 dBSimulation at 80m: 176 dB


Mitigation Open Air Explosions 18Levels at 300m (<strong>be</strong>yond slope)Small effects <strong>for</strong> all variants! No noticable effect of <strong>mitigation</strong> <strong>measures</strong>


Mitigation Open Air Explosions 19Explanationvariant2bAt 80m: variant0 12000 Pa, variant2b 6000 PaAt 90m: variant0 6000 Pa, variant2b 5000 Pa propagation <strong>in</strong><strong>to</strong> “shadow zone”, easy <strong>for</strong> low frequenciesshadowvariant2b, already smooth wave with low-frequency content (higher freq’s are damped)variant0, only low-frequencies propagate <strong>in</strong><strong>to</strong> shadow zoneVariant0Variant2b


Mitigation Open Air Explosions 20Balcony results: <strong>in</strong>creased screen<strong>in</strong>g


Mitigation Open Air Explosions 21Balcony results: <strong>in</strong>creased screen<strong>in</strong>g


Balcony results at 300 mMitigation Open Air Explosions 22


Mitigation Open Air Explosions 23ConclusionsHybrid FCT-NPE-PE method presented <strong>for</strong> shock wave propagation non-l<strong>in</strong>ear <strong>in</strong>teraction with barrier / absorb<strong>in</strong>g material;Standard barrier has limited effect <strong>for</strong> explosions;Add<strong>in</strong>g absorb<strong>in</strong>g material <strong>in</strong>creases shield<strong>in</strong>g effect;For strong explosions special constructions (balcony) are needed <strong>to</strong><strong>in</strong>crease barrier effect significantly.

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