Nonlinear evolution of the ablative Rayleigh-Taylor instability with preheating
W. H. Ye, X. T. He, W. Y. Zhang, and M. Y. Yu

TL;DR
This paper numerically investigates how preheating length influences the nonlinear evolution of the ablative Rayleigh-Taylor instability, revealing different behaviors for weak and strong preheating conditions.
Contribution
It provides new insights into the nonlinear evolution of the ablative Rayleigh-Taylor instability considering preheating effects, highlighting the dependence on preheating length.
Findings
Weak preheating causes a sharp maximum in growth rate and secondary spike-bubbles.
Strong preheating results in elongated jets without secondary spike-bubbles.
Interaction of harmonic modes explains the different evolution patterns.
Abstract
Evolution of the single-mode ablative Rayleigh-Taylor instability in the presence of preheating is investigated numerically. It is found that the instability evolution depends strongly on the preheating length in front of the ablation-front interface. For weak preheating (, where is the Spitzer-Harm length and is a critical value), the linear growth rate has a sharp maximum and a secondary spike-bubble structure is generated. Interaction of this growing structure with the master spike-bubble leads to rupture of the latter. However, for strong preheating (), the linear growth rate has no sharp maximum and no secondary spike-bubble is generated. Instead, the master spike-bubble evolves into an elongated jet. These results are interpreted in terms of the evolution and interaction of the instability-generated harmonic…
Peer Reviews
No public reviews on file for this paper yet. If you reviewed it on a platform where reviews are public (OpenReview, ICLR, NeurIPS, ICML), you can paste yours below so the community can read it here.
Videos
No videos yet. Explain this paper in a talk, walkthrough, or lecture? Add one.
Taxonomy
TopicsFluid Dynamics and Turbulent Flows · Laser-Plasma Interactions and Diagnostics · Plasma and Flow Control in Aerodynamics
