Hostname: page-component-77c89778f8-7drxs Total loading time: 0 Render date: 2024-07-18T23:41:34.586Z Has data issue: false hasContentIssue false

Effect of the surface finish on the stability of targets imploded by thermal radiation

Published online by Cambridge University Press:  09 March 2009

A. Caruso
Affiliation:
Associazione EURATOM-ENEA sulla Fusione, C.E. Frascati, C.P. 65–00044 Frascati, Roma, Italia
V. A. Pais
Affiliation:
Associazione EURATOM-ENEA sulla Fusione, C.E. Frascati, C.P. 65–00044 Frascati, Roma, Italia

Abstract

The effect of surface finish on the evolution of ICF targets has been studied. As driver for the implosion has been used a temporally profiled thermal radiation pulse (25 ns in duration) as that expected for the case of a high-gain (cm sized) capsule enclosed in a cavity. 2-D numerical simulations have been performed on a planar analog to investigate the stability to perturbations having wavelengths in the interval 2.5–40 μm and initial amplitudes of 0.03 and 1 μm. The simulations show perturbation growing due to hydrodynamic instabilities. The distortion of the ablation front reaches such a level to strongly enhance the ablation rate because of the increase in the exposed area and in the power absorbed per unit area. Two different phenomena have been identified: one, preferentially occurring for small wavelengths, in which the motion behind the first shock wave becomes turbulent and the symmetry is lost; the other, appearing for long wavelengths, in which a thermal radiation wave penetrates into the fuel. This preheating phenomenon is related to the formation of holes in the thermal shield due to the enhanced ablation and to matter transverse piling up. All these effects may render useless the 1-D-based design of a high-gain capsule exposed to a given thermal bath. However, it has been also observed that, for the longer wavelength (40 μm) and a smaller initial perturbation amplitude (e.g. 0.01 μm), during the temperature pulse the preheating does not occur and most of the fuel can be accelerated as a whole to speeds of the order of 2 × 107 cm/s or greater without a substantial onset of transverse velocities, even in the presence of the ablator piling up.

Type
Research Article
Copyright
Copyright © Cambridge University Press 1993

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

References

REFERENCES

Caruso, A. 1989 In Proceedings of the Varenna Course and Workshop on Inertial Confinement Fusion, Casa Editrice Compositori, Bologna, Italy, p. 139.Google Scholar
Caruso, A. & Pais, V.A. 1989 In Proceedings of the Varenna Course and Workshop on Inertial Confinement Fusion, Casa Editrice Compositori, Bologna, Italy, p. 163.Google Scholar
Pais, V.A. & Caruso, A. 1990 Comp. Phys. Comm. 58, 55.CrossRefGoogle Scholar