Bulletin of the American Physical Society
65th Annual Meeting of the APS Division of Plasma Physics
Monday–Friday, October 30–November 3 2023; Denver, Colorado
Session UP11: Poster Session VIII:
HED:High Energy Density Plasma Science
MFE: Superconducting Tokamaks; Self-organized configurations II: FRC, RFP, Spheromak; Machine learning techniques in MFE
ICF: Machine learning techniques in ICF
2:00 PM - 5:00 PM
Thursday, November 2, 2023
Room: Plaza ABC
Abstract: UP11.00036 : Shock Structure and Radiative Cooling Effects on Reverse Shock Experiments at MAGPIE*
Presenter:
Stefano Merlini
(Imperial College London)
Authors:
Stefano Merlini
(Imperial College London)
Jack D Hare
(MIT PSFC)
Guy C Burdiak
(First Light Fusion Ltd)
Jack W Halliday
(University of Oxford)
Andrea Ciardi
(Sorbonne Université, Observatoire de Paris)
Jeremy P Chittenden
(Imperial College London)
Aidan C Crilly
(Imperial College London)
Katherine Marrow
(Imperial College London)
Danny Russell
(Technische Universitaet Muenchen)
Lee G Suttle
(Imperial College London)
Eleanor R Tubman
(Imperial College London)
Vicente Valenzuela-Villaseca
(Princeton University)
Thomas Varnish
(Massachusetts Institute of Technology)
Sergey V Lebedev
(Imperial College London)
Despite similar upstream flow velocities and mass densities, we observe striking variations in the reverse shock structure depending on the wire material used. Specifically, when aluminium wire arrays are employed, we observe a well-defined, sharp shock that aligns with magneto-hydrodynamic theory. However, in the case of tungsten wires, we do not observe a distinct stand-off shock; instead, we observe a broad region characterized by density fluctuations spanning a wide range of spatial scales.
These two contrasting interactions are diagnosed by using interferometry, Thomson scattering, shadowgraphy, and a newly developed imaging refractometer [3]. The refractometer enables to characterise the small-scale density perturbations by detecting subtle deflections of the probing laser. Our findings suggest that the differences in shock structure are most likely due to radiative cooling instabilities which give rise to density perturbations elongated along magnetic field lines. In aluminium plasma, these instabilities grow more slowly and are mitigated by thermal conduction.
[1] J. H. Hunter, Jr., “Generalized Thermal Stability and its Application to the Interstellar Gas”, ApJ, (1970).
[2] F. Suzuki-Vidal, et. al. “Bow Shock Fragmentation Driven by a Thermal Instability in Laboratory Astrophysics Experiments”, ApJ, (2015).
[3] Hare, J. D. et. al. “An Imaging Refractometer for Density Fluctuation Measurements in High Energy Density Plasmas”, RSI, (2020).
[4] S. Merlini, J. D. Hare, G. C. Burdiak, et. al. "Radiative Cooling Effects on Reverse Shocks Formed by Magnetised Supersonic Plasma Flows", AIP PoP, (2023) [arXiv preprint].
*This work was supported by the Engineering and Physical Sciences Research Council (EPSRC) Grant No. EP/N013379/1 and the US Department of Energy (DOE), including Awards No. DE-NA0003764 and No. DESC0020434.
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