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Simulation of the Effects of an Air Blast Wave - ELSA - Europa

Simulation of the Effects of an Air Blast Wave - ELSA - Europa

Simulation of the Effects of an Air Blast Wave - ELSA - Europa

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250200Impulse from KingeryImpulse with b from KinneyImpulse with b from BakerImpulse with b by using pminImpulse [Pa sec]1501005000 2 4 6 8 10 12 14 16 18 20Scaled dist<strong>an</strong>ce Z [m/kg 1/3 ]Figure 7: Decay parameter b – resulting impulse in comparison with <strong>the</strong> impulse from KingeryTherefore, <strong>the</strong> parameter b is next calculated using <strong>the</strong> impulse <strong>of</strong> <strong>the</strong> positive phase. Then, <strong>the</strong>resulting curve <strong>of</strong> b is similar to <strong>the</strong> curves <strong>of</strong> Kinney <strong>an</strong>d Baker. The exponential trend line givenby Excel has <strong>the</strong> following equationb1.1975= 5.2777⋅ Z −(11)The pressure time curve that is built with this b doesn’t fulfil <strong>the</strong> minimal pressure in <strong>the</strong> negativephase. Sometimes <strong>the</strong> pressure p is smaller th<strong>an</strong> <strong>the</strong> atmospheric pressure. This results in <strong>an</strong>impossible state <strong>of</strong> <strong>the</strong> air. Therefore, <strong>the</strong> approximation <strong>of</strong> <strong>the</strong> negative phase is done with abilinear curve shown in equation (12) <strong>an</strong>d Figure 8 by using <strong>the</strong> values <strong>of</strong> <strong>the</strong> negative phase shownin section 2.2.4.⎛tt ⎞ dp= p0 + pmax⎜1 − ⎟ for t < td⎝ td⎠2 pntnp= p0− ( t− td) for t > td ∧ t < td+t22 pntnp = p0− ( t + t − t) for t > t + ∧ t < t + tt2p= p for t > t + t0nnbt−d n d d ndn(12)15

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