Discrete Sommerfeld diffraction problems on hexagonal lattice with a zigzag semi-infinite crack and rigid constraint

被引:0
作者
Basant Lal Sharma
机构
[1] Indian Institute of Technology Kanpur,Department of Mechanical Engineering
来源
Zeitschrift für angewandte Mathematik und Physik | 2015年 / 66卷
关键词
Sommerfeld diffraction; Lattice; Hexagonal; Honeycomb; Zigzag; Crack; Rigid ribbon; Wiener–Hopf; Primary 78A45; Secondary 39A14; 47B35;
D O I
暂无
中图分类号
学科分类号
摘要
Diffraction problems, associated with waves scattered by a semi-infinite crack and rigid constraint, in a hexagonal (honeycomb) lattice model, with nearest neighbor interactions, are solved exactly using the method of Wiener and Hopf. Asymptotic expressions for the scattered waves in far field are provided for both problems, by application of the method of stationary phase to corresponding diffraction integrals. Additionally, for the crack diffraction problem, bond lengths on the semi-infinite row complementing the crack, as well as the crack opening displacement, are provided in closed form except for the presence of concomitant Fourier coefficients of the Wiener–Hopf kernel. For the rigid constraint diffraction problem, the solution on the semi-infinite row complementing the constrained lattice sites, as well as that adjacent to the constrained row, are provided in similar closed form. The amplitude, as well as phase, of waves in far field is compared, through graphical plots, with that of a numerical solution on finite grid. Also, the analytical solution for few sites near the tip of each defect is compared with numerical solution. Both discrete Sommerfeld diffraction problems and their solutions are also relevant to numerical solution of the two-dimensional Helmholtz equation using a 4-point hexagonal grid, besides having applications inherent to the scattering of waves on a honeycomb structure.
引用
收藏
页码:3591 / 3625
页数:34
相关论文
共 48 条
[1]  
Ablowitz M.J.(2012)Nonlinear waves in shallow honeycomb lattices SIAM J. Appl. Math. 72 240-260
[2]  
Zhu Y.(1982)Lattice-dynamical model for graphite Phys. Rev. B 26 4514-4522
[3]  
Al-Jishi R.(1994)A perfectly matched layer for the absorption of electromagnetic waves J. Comput. Phys. 114 185-200
[4]  
Dresselhaus G.(2007)Conical diffraction: Hamilton’s diabolical point at the heart of crystal optics Prog Optics 50 13-50
[5]  
Berenger J.P.(2009)Truncation effects in a semi-infinite periodic array of thin strips: A discrete Wiener–Hopf formulation Radio. Sci. 44 RS2S91-396
[6]  
Berry M.V.(1963)The vibrations of three two-dimensional lattices Proc. Camb. Phil. Soc. 59 383-27
[7]  
Jeffrey M.R.(1955)Asymptotic representations of Fourier integrals and the method of stationary phase J. Soc. Ind. Appl. Math. 3 17-1220
[8]  
Capolino F.(2012)Honeycomb lattice potentials and Dirac points J. Am. Math. Soc. 25 1169-286
[9]  
Albani M.(2015)Wave packets in honeycomb structures and two-dimensional Dirac equations Commun. Math. Phys. 326 251-884
[10]  
Dean P.(1958)Diffraction of electromagnetic waves on a semi-infinite grating Radiotekhn i Elektron 3 882-95