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.

1.
A.
Kar
and
J.
Mazumder
A Mathematical Model for Nanoscale Particles Formed During Laser Ablation
,”
Phys. Rev. E
49
,
410
419
(
1994
).
2.
M. F.
Kanevsky
,
L. A.
Bolshov
,
S. Yu.
Chernov
and
V. A.
Vorobjev
, “
Computer Modeling of Unsteady Gasdynamical and Optical Phenomena in Low Temperature Plasmas
,”
SPIE
Vol.
1440
(
1990
), and related papers.
3.
S. I.
Braginskii
, “Transport Processes in a Plasma,” in
Reviews of Plasma Physics
,
M. A.
Leontovich
(ed.),
Consultants Bureau
,
NY
,
1965
, Vol.
I
.
4.
P. J.
Roache
,
Computational Fluid Dynamics
,
Hermosa Publishers
,
Albuquerque
,
1972
.
5.
Ya. B.
Zel’dovich
and
Yu. P.
Raizer
,
Physics of Shock Waves and High-Temperature Hydrodynamic Phenomena
,
Academic Press
,
1966
.
6.
S. I.
Anisimov
, “
Vaporization of Metal Absorbing Laser Radiation
,”
Sov. Phys. JETP
27
,
182
183
(
1968
)
C. J.
Knight
, “
Theoretical Modeling of Rapid Surface Vaporization with Back Pressure
,”
AIAA J.
17
,
519
523
(
1979
).
7.
Data taken at LLNL by
L. V.
Berzins
(low intensities) and by
E. P.
Dragon
(high intensities).
8.
A. C.
Hindmarsh
, “ODEPACK, a Systematized Collection of ODE Solvers,” in
Scientific Computing
,
R. S.
Stepleman
et al. (eds.),
North-Holland, Amsterdam
,
1983
(Vol. I of IMACS Transactions on Scientific Computing), pp.
55
64
.
9.
M. B.
Carver
, “
Pseudo Characteristic Method of Lines Solution of the Conservation Equations
,”
J. Comp. Phys.
35
,
57
76
(
1980
)
Y.-Z.
Wang
and
S. H.
Johnson
, “
Pseudocharacteristic Method of Lines Simulation of Single- and Two-Phase One-Dimensional Flow Transients
,”
Proc. IMACS 11th World Congress
, Vol.
2
, pp
201
204
,
Oslo
,
1985
.
10.
A.
Nesmeyanov
Vapor Pressure of the Chemical Elements
,
Elsevier Publishing Co.
,
1963
.
11.
K.
Hornung
Liquid Metal Coexistence Properties from Corresponding States and Third Law
,”
J. Appl. Phys.
46
,
2548
(
1975
).
12.
Y. S.
Touloukian
et al,
Thermophysical Properties of Matter, Vol. I, Thermal Conductivity — Metallic Elements and Alloys
,
IFI/Plenum
,
1970
.
13.
A.
Ng
. et al, “
Reflectivity of Intense Femtosecond Laser Pulses from a Simple Metal
,”
Phys. Rev. Letters
72
,
3351
(
1994
).
This content is only available via PDF.
You do not currently have access to this content.