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Analytical study of ionizing blast waves in atomic hydrogen
The ionization effect on both the evolution and internal structure of a blast wave (BW) is determined in laboratory conditions. In a first step, the Rankine–Hugoniot equations describing the structure of the shock front together with the Saha equation modeling ionization are solved analytically in a...
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Published in: | Physics of plasmas 2023-04, Vol.30 (4) |
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Main Authors: | , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites |
Online Access: | Get full text |
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Summary: | The ionization effect on both the evolution and internal structure of a blast wave (BW) is determined in laboratory conditions. In a first step, the Rankine–Hugoniot equations describing the structure of the shock front together with the Saha equation modeling ionization are solved analytically in a consistent way for the conditions of a cold initial atomic hydrogen gas. In a second step, a simplified approach is used by introducing an effective adiabatic index
γ
* that takes into account ionization arising at the shock front. Finally,
γ
* is used as input data in the self-similar model derived formerly by Barenblatt to describe the structure and the dynamics of the ionizing BW. For the typical laboratory conditions of blast wave experiments, ionization achieves a hydrogen gas compression up to about 11 times at the shock front of the blast wave where a thin and dense shell forms. For such a compression, the value of the effective adiabatic index is
γ
*
≃
1.2 leading to a self-similar evolution of the BW where its radius R(t) varies according to
R
(
t
)
∝
t
α
* with
α
*
≃
0.33. This value of
α
* is lower than the adiabatic expansion stage
α
=
2
/
5, where the total energy of the BW is conserved. Thus, ionization is found to act as a cooling effect at the shock front where a fraction of kinetic energy is absorbed to ionize the gas. |
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ISSN: | 1070-664X 1089-7674 |
DOI: | 10.1063/5.0133470 |