A model of drilling by high radiance pulsed lasers is described. The model involves a one-dimensional description of heat transport below the bottom of the hole, hydrodynamic expansion of the vapor and compressed air, and light propagation through the vapor. The pressure and energy of the vapor are taken from a separate Saha equilibrium code. The boundary conditions at the vaporization surface include the formation of a transition layer within which macroscopic fluid conditions are reached. The absorption mechanisms are photoionization and inverse bremsstrahlung. The model has been applied to the case of drilling in stainless steel with green copper laser light, for peak input intensities ranging from 108 to 4 × 1010 W/cm2. Below 3 × 108 W/cm2, there is negligible absorption in the vapor and ablation increases rapidly with intensity. After decreasing for a short interval beyond this point, the ablation rate then increases steadily with power because of a growing electron thermal conduction to the surface. The experimental ablation rate exhibits a somewhat faster overall growth. It appears comparable to the model at low power but is about five times greater at the highest power.
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ICALEO '94: Proceedings of the Laser Materials Processing Conference
October 17–20, 1994
Orlando, Florida, USA
ISBN:
978-0-912035-52-9
PROCEEDINGS PAPER
Computational model of drilling with high radiance pulsed lasers Available to Purchase
C. D. Boley;
C. D. Boley
University of California, Lawrence Livermore National Laboratory
, Livermore, CA 94550 USA
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J. T. Early
J. T. Early
University of California, Lawrence Livermore National Laboratory
, Livermore, CA 94550 USA
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Published Online:
October 01 1994
Citation
C. D. Boley, J. T. Early; October 17–20, 1994. "Computational model of drilling with high radiance pulsed lasers." Proceedings of the ICALEO '94: Proceedings of the Laser Materials Processing Conference. ICALEO '94: Proceedings of the Laser Materials Processing Conference. Orlando, Florida, USA. (pp. pp. 499-508). ASME. https://doi.org/10.2351/1.5058828
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