Three-dimensional thermal simulation of nanosecond laser ablation for semitransparent material
Introduction
When laser is irradiated onto the free surface of a material, it is partially reflected and partially absorbed. The reflected portion of the incident laser beam has not always been considered in the calculation of the laser energy transfer in laser material processing simulations. This is acceptable when the reflected laser beam does not contact the free surface again or the reflectance of the material is sufficiently low. However, in laser material processing, a deep keyhole is typically formed, requiring the reflections inside the keyhole to be carefully considered. It is clear that the effect of reflections is significantly more important for highly reflective materials. However, the Fresnel reflection theory predicts that even a “nonreflecting” material will reflect almost 100% of an incident laser beam at grazing incidence. Ray tracing techniques have been implemented to calculate the effect of reflections [1], [2], [3], [4], [5], [6]. In these techniques, a laser beam consists of a number of rays. Each ray is traced in the simulation domain, and consequently, the total absorbed energy is summed over the entire domain to obtain the energy redistribution of the laser beam.
The refracted portion of the incident laser beam is transmitted into the material and eventually absorbed. If the material can be assumed to be perfectly opaque, it is not transmitted into the material and fully absorbed at the free surface. In this case, it is considered as the surface energy flux boundary condition at the free surface. Although a real material is partially transparent to some degree, the assumption is valid when the penetration depth of the laser beam into the material is sufficiently small. Metals usually satisfy this assumption. However, the absorption of the laser beam energy is not limited to the free surface and volumetric absorption occurs inside a semitransparent material such as polymer. Although a few numerical models describing volumetric absorption in polymer could be found in the literature [7], [8], the authors used predefined volumetric absorption models that do not correctly consider the time-varying shape of the laser-processed region.
Ray tracing highly depends on the geometry of a free surface. Several methods are available for the reconstruction of the free surface in numerical simulations. The level set (LS) method and the volume-of-fluid (VOF) method are the most prominent. The prime advantage of the VOF method over the LS method is its accuracy of the mass calculation, which is important to estimate the amount of material removal in the numerical simulation of laser material processing. The LS method gives smoother representation of the free surface, which is indispensable for the calculation of the reflected/refracted ray direction. Because the VOF and the LS methods are complementary to each other, some methods that couple them have been suggested [9], [10], [11], [12]. However, they are complicated because both the LS advection equation and VOF advection equation need to be solved together. Sun and Tao [13] suggested a simpler method in which only the VOF advection equation needs to be solved. The LS function which is needed for the free surface reconstruction is calculated by geometric operation of the volume fraction data of VOF.
It is difficult to find an integrated 3D simulation model including both the reflection and the volumetric absorption of the transmitted laser beam. Only one of the two is considered in most simulation models. Despite the frequent use of ray tracing in laser energy transfer models, an in-depth discussion of the ray tracing method itself is rarely given. In this study, an integrated model was established for the numerical simulation of laser material processing of a semitransparent material. Both the reflection and the volumetric absorption are considered by means of a ray tracing technique. The discretized signed distance function, a kind of LS function, is applied for ray/surface intersection detection and calculation of the reflected/refracted directions of rays.
Section snippets
Free surface representation
There are several methods to represent a free surface shape in a VOF method such as the simple line interface calculation (SLIC) [14], the piecewise linear interface construction (PLIC) [15], and the flux line-segment model for advection and interface calculation (FLAIR) [16]. The PLIC method is generally used to represent a free surface shape in a VOF method among these methods. In the PLIC, the free surface in a cell is represented as a straight line segment (in 2D) or a plane segment (in 3D)
Ray tracing in the simulation domain
Despite the frequent application of ray tracing to the energy transfer models of laser beams, it is difficult to find detailed descriptions of the specific ray tracing algorithms being applied. They are briefly given in a few previous studies [3], [5], [6]. However, the given ray tracing algorithm requires extensive search operations to identify the cell in which the ray intersects the free surface. The drawback of such algorithm is that all the simulation cells are accessed whenever the
Numerical simulation
Numerical simulations were carried out to validate whether the proposed model well describes the effect of reflection and transmission in 3D simulations. The simulations are designed to observe the effects of various initial surface shapes and the varying aspect of laser energy transfer during surface deformation by ablation. Since a semitransparent material such as polymer is suitable for this purpose, polyimide is selected as the target material of the present study.
Conclusion
In 3D simulations of laser material processing based on the VOF method, both reflection and refraction were considered by the proposed ray tracing model. Fresnel equations were implemented in the calculations of reflection and refraction. The problem of a ray branching into reflected and refracted rays was resolved by a stochastic treatment of the ray/surface intersection event.
The applied free surface reconstruction method was a contributing factor for improved ray tracing, particularly for
Acknowledgment
This work was supported by the Technology Innovation Program (Industrial Strategic Technology Development Program, 10033829) funded by the Ministry of Trade, Industry & Energy (MOTIE) and the National Research Foundation funded by the Ministry of Science, ICT & Future Planning (MSIP).
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