2013
DOI: 10.1134/s002189441302020x
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Effect of shielding of a part of the casing of a technological explosion chamber on its stress state

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Cited by 3 publications
(3 citation statements)
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“…In a real EC, the distances from the side wall and cupola to the charge center may be different, so the stress-strain state of the shell may differ significantly from the uniform one. The strain-stress measurements performed in the explosive chamber KV-2M, KVG-16 described below showed that the real maximal stresses in the EC shell could differ by 1.5 -2 times from the averaged values calculated by the formulas (6-8) [5,6]. This effect is caused by the fact that, during shell oscillations, flexural waves converge in the cupola center, their amplitudes are added, and stresses are concentrated.…”
Section: Basic Calculations Of Explosion Chambersmentioning
confidence: 93%
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“…In a real EC, the distances from the side wall and cupola to the charge center may be different, so the stress-strain state of the shell may differ significantly from the uniform one. The strain-stress measurements performed in the explosive chamber KV-2M, KVG-16 described below showed that the real maximal stresses in the EC shell could differ by 1.5 -2 times from the averaged values calculated by the formulas (6-8) [5,6]. This effect is caused by the fact that, during shell oscillations, flexural waves converge in the cupola center, their amplitudes are added, and stresses are concentrated.…”
Section: Basic Calculations Of Explosion Chambersmentioning
confidence: 93%
“…The formulas (1,2,5) give an important relation for the evaluation of the EC shell mass needed to localize the explosion of the specific mass M e 2 2 In this formula σ a means an allowable stress in the shell. For example, taking σ a = 200 MPa for a steel shell, we have M/M e = 1.2 10 3 .…”
Section: Basic Calculations Of Explosion Chambersmentioning
confidence: 99%
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