Laser pulse heating and vapor front generation

被引:5
作者
Yilbas, B. S. [1 ]
Bin Mansoor, S. [1 ]
Shuja, S. Z. [1 ]
Abualhamayel, H. [1 ]
机构
[1] King Fahd Univ Petr & Minerals, Dept Engn Mech, Dhahran 31261, Saudi Arabia
关键词
laser; pulse; heating; phase change; cavity; vapor;
D O I
10.1002/aic.11411
中图分类号
TQ [化学工业];
学科分类号
0817 ;
摘要
Laser nonconduction limited heating situation results in cavity formation and vapor front development above the cavity. As laser heating progresses, cavity wall recesses towards the solid bulk while the vapor front expands into its ambient due to recoil pressure generated at liquid-vapor interface in the cavity. To obtain velocity, temperature, and pressure fields in the evaporating front become challenging, since the process involves with transient evaporation of the surface during the absorption of the laser energy by the solid substrate. In the present study, phase change processes taking place in the substrate material during a laser heating process are modeled using an energy method and evaporating front behavior is modeled using the transient flow equations. Since the problem is involved with the multi-physics, the numerical technique is introduced to solve the resulting governing equations. The water ambient is assumed around the cavity in order to resemble the laser processing situation, particularly for laser shock processing. It is found that for nanosecond pulses with high intensity, the recession velocity of the surface reaches about 100 m/s at the symmetry axis and the recoil pressure of in the order of 10 GPa is generated in the cavity as a result of rapid evaporation. (c) 2008 American Institute of Chemical Engineers.
引用
收藏
页码:627 / 638
页数:12
相关论文
共 18 条
[1]   Entrainment characteristics of transient gas jets [J].
Abraham, J .
NUMERICAL HEAT TRANSFER PART A-APPLICATIONS, 1996, 30 (04) :347-364
[2]  
[Anonymous], 1980, SERIES COMPUTATIONAL, DOI [DOI 10.1201/9781482234213, 10.1201/9781482234213]
[3]   The effect of plasma formation on beam focusing in deep penetration welding with CO2 lasers [J].
Beck, M ;
Berger, P ;
Hugel, H .
JOURNAL OF PHYSICS D-APPLIED PHYSICS, 1995, 28 (12) :2430-2442
[4]   TEMPERATURE PROFILE IN SEMI-INFINITE BODY WITH EXPONENTIAL SOURCE AND CONVECTIVE BOUNDARY-CONDITION [J].
BLACKWELL, BF .
JOURNAL OF HEAT TRANSFER-TRANSACTIONS OF THE ASME, 1990, 112 (03) :567-571
[5]   HIGH-INTENSITY LASER-INDUCED VAPORIZATION AND EXPLOSION OF SOLID MATERIAL [J].
DABBY, FW ;
PAEK, U .
IEEE JOURNAL OF QUANTUM ELECTRONICS, 1972, QE 8 (02) :106-&
[6]   Two-dimensional gas-dynamic model of laser ablation in an ambient gas [J].
Gusarov, AV ;
Gnedovets, AG ;
Smurov, I .
APPLIED SURFACE SCIENCE, 2000, 154 :66-72
[7]   Analytical solution for laser evaporative heating process: time exponentially decaying pulse case [J].
Kalyon, M ;
Yilbas, BS .
JOURNAL OF PHYSICS D-APPLIED PHYSICS, 2001, 34 (22) :3303-3311
[8]   SPREADING RATE OF AN UNSTEADY TURBULENT JET [J].
KOUROS, H ;
MEDINA, R ;
JOHARI, H .
AIAA JOURNAL, 1993, 31 (08) :1524-1526
[9]   Spectroscopic characterization of laser-induced plasma created during welding with a pulsed Nd:YAG laser [J].
Lacroix, D ;
Jeandel, G .
JOURNAL OF APPLIED PHYSICS, 1997, 81 (10) :6599-6606
[10]   Computational modeling of physical processes during laser ablation [J].
Liu, CL ;
Leboeuf, JN ;
Wood, RF ;
Geobegan, DB ;
Donato, JM ;
Chen, KR ;
Puretzky, AA .
MATERIALS SCIENCE AND ENGINEERING B-SOLID STATE MATERIALS FOR ADVANCED TECHNOLOGY, 1997, 47 (01) :70-77