Bulletin of the American Physical Society
23rd Biennial Conference of the APS Topical Group on Shock Compression of Condensed Matter
Volume 68, Number 8
Monday–Friday, June 19–23, 2023; Chicago, Illinois
Session DD06: Perturbation Growth and Ejecta: Experiments
9:15 AM–10:15 AM,
Friday, June 23, 2023
Sheraton Grand Chicago Riverwalk
Room: Chicago 8
Chair: Jonathan Lind, Lawrence Livermore National Laboratory
Abstract: DD06.00004 : Calculation and measurement of the velocity of a jet from a triangular groove
10:00 AM–10:15 AM
Presenter:
Laurent Soulard
(CEA, DAM, DIF, F-91297 Arpajon, France)
Authors:
Laurent Soulard
(CEA, DAM, DIF, F-91297 Arpajon, France)
Olivier Durand
(CEA, DAM, DIF)
Jean-René Burie
(CEA, DAM, DIF)
Sébastien Eveillard
(CEA, DAM, DIF, F-91297 Arpajon, France)
Louis-Pierre Terzulli
(CEA, DAM, GRAMAT, F-46500 Gramat, France)
In micro-jetting modeling, it is important to know the velocity and density of the jet. This is particularly the case for the development of jet fragmentation models, such as the FZP model proposed a few years ago in the literature [J. Appl. Phys., 117,165903 (2015)]. An extension of the Birkhoff's model, called BMPT-2, has recently been proposed. This model allows the calculation of the speed of the jet and its density provided that the solution is known. BMPT-2 leads to a satisfactory agreement with the results of classical molecular dynamics simulations. In order to go further, a series of plates impact experiments were done in which the velocities of jets from triangular grooves of tin targets were accurately measured by PDV. The comparison of BMPT-2 with these experimental results is very satisfactory and the agreement is much better than with the original Birkhoff’ model, or with a model derived from the Richtmyer-Meshkov instabilities theory. In addition to the jet velocity, BMPT-2 provides its density. The calculation shows that it is much lower than the density of the material at rest.
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