2020
DOI: 10.1039/d0ra04730a
|View full text |Cite
|
Sign up to set email alerts
|

A coupled model of electromagnetic and heat on nanosecond-laser ablation of impurity-containing aluminum alloy

Abstract: Nanosecond laser ablation is the theoretical revealed by a coupled model of electromagnetic and heat.

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1

Citation Types

0
3
0

Year Published

2021
2021
2024
2024

Publication Types

Select...
4
1

Relationship

1
4

Authors

Journals

citations
Cited by 5 publications
(3 citation statements)
references
References 39 publications
0
3
0
Order By: Relevance
“…This equation is commonly expressed as a function of the incident electric field and the imaginary part of the permittivity function, 𝑞 = 𝜀𝜔 0 Im(𝜀 𝑚 )|𝐄(𝑟)| 2 , where ω is the angular frequency and Δ m is the permittivity of the materials. 34 Stray light on the Al-based functional gradient films did not imply large laser fluences. 35 Hence, Ohm's law was used to calculate the heat source density,𝑞 = |𝐉| 2 ∕𝜎, where σ is the electrical conductivity of the materials.…”
Section: Simulation Proceduresmentioning
confidence: 97%
See 1 more Smart Citation
“…This equation is commonly expressed as a function of the incident electric field and the imaginary part of the permittivity function, 𝑞 = 𝜀𝜔 0 Im(𝜀 𝑚 )|𝐄(𝑟)| 2 , where ω is the angular frequency and Δ m is the permittivity of the materials. 34 Stray light on the Al-based functional gradient films did not imply large laser fluences. 35 Hence, Ohm's law was used to calculate the heat source density,𝑞 = |𝐉| 2 ∕𝜎, where σ is the electrical conductivity of the materials.…”
Section: Simulation Proceduresmentioning
confidence: 97%
“…The heat source density ( q [W/m 3 ]) given byq=boldE·boldJ$q = {\bf{E}} \cdot {\bf{J}}$, where E is the electric field and J is the current density. This equation is commonly expressed as a function of the incident electric field and the imaginary part of the permittivity function, q=Δω0Im(Δm)false|E(r)false|2$q = \varepsilon {\omega _0}{\mathop{\rm Im}\nolimits} ({\varepsilon _m}){| {{\bf{E}}(r)} |^2}$, where ω is the angular frequency and Δ m is the permittivity of the materials 34 . Stray light on the Al‐based functional gradient films did not imply large laser fluences 35 .…”
Section: Simulation and Experimental Proceduresmentioning
confidence: 99%
“…Several methods have been used for LIDT simulation, such as the finite element method (FEM) and the finite difference time domain (FDTD) 30 – 32 The order of LIDT magnitude in simulation can be consistent with that in experiments currently. However, the mechanisms and performance of laser-induced damage in materials have not been clearly investigated yet.…”
Section: Introductionmentioning
confidence: 95%