29th International Symposium on Shock Waves 1 2015
DOI: 10.1007/978-3-319-16835-7_11
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Shock Tube Simulation of Low Mach Number Blast Waves

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“…One source is the growth of the boundary layer in the test slug and driver gas, which serves to attenuate the shock by entraining mass from the core flow [1,4]. The motion of the contact surface, the interface between the expanded driver gas and test gas, also produces waves which affect the shock speed [5]. The behaviour of the contact surface is itself dependent on many factors including the driver technology employed, the driver condition chosen for the experiment, and the primary diaphragm rupture behaviour [6].…”
Section: Introductionmentioning
confidence: 99%
“…One source is the growth of the boundary layer in the test slug and driver gas, which serves to attenuate the shock by entraining mass from the core flow [1,4]. The motion of the contact surface, the interface between the expanded driver gas and test gas, also produces waves which affect the shock speed [5]. The behaviour of the contact surface is itself dependent on many factors including the driver technology employed, the driver condition chosen for the experiment, and the primary diaphragm rupture behaviour [6].…”
Section: Introductionmentioning
confidence: 99%
“…The driver also causes further waves to reach the shock. This is due to having a finite driver section length, change in volume if a free piston driver is used or transient heating processes if a deflagration, detonation or arc heating driver are used [2]. Additionally, the diaphragm rupture is not an instantaneous process and can introduce a rapid acceleration of the shock and subsequent deceleration, substantially influencing shock tube performance [3,4].…”
Section: Introductionmentioning
confidence: 99%