Frequency-Dependent MNL-FDTD Scheme for Wideband Analysis of Printed Circuit Boards With Debye Dispersive Media

A semiimplicit and frequency-dependent 3-D finite-difference time-domain (FDTD) scheme with relaxed numerical stability was presented for wideband analysis of multilayer printed circuit boards (PCBs) with thin conductive and dielectric layers. This new scheme is formulated by directionally and magnetically introducing the Newmark-beta method into the conventional FDTD explicit scheme based on the recursive convolution (RC) approach for the so-called extended Debye model with an effective dc conductivity. No dependence of mesh step in the normal direction to the PCB layers is included in its stable condition. Interestingly, the presented semiimplicit scheme can be reduced to the RC-based explicit FDTD when the Newmark parameter is chosen as zero. The scheme was carefully verified in applications to rectangular power-bus structures, an irregular power-bus structure with decoupling capacitors and multilayer PCBs with planar electromagnetic bandgap structures. It was demonstrated in these test problems that the calculation time was reduced by a factor of 1/4–1/30 in comparison with the explicit scheme, while maintaining the same level of accuracy.

[1]  Juan Chen,et al.  Numerical Simulation Using HIE-FDTD Method to Estimate Various Antennas With Fine Scale Structures , 2007, IEEE Transactions on Antennas and Propagation.

[2]  Cylindrical FDTD with improved time step size based on hybrid Newmark-Beta discretization , 2013, 2013 International Symposium on Electromagnetic Theory.

[3]  A Partially Implicit FDTD Method for the Wideband Analysis of Spoof Localized Surface Plasmons , 2015, IEEE Photonics Technology Letters.

[4]  R. B. Standler,et al.  A frequency-dependent finite-difference time-domain formulation for dispersive materials , 1990 .

[5]  Raymond J. Luebbers Lossy dielectrics in FDTD , 1993 .

[6]  T. Namiki 3-D ADI-FDTD method-unconditionally stable time-domain algorithm for solving full vector Maxwell's equations , 2000 .

[7]  Kazuhiro Fujita MNL-FDTD/SPICE Method for Fast Analysis of Short-Gap ESD in Complex Systems , 2016, IEEE Transactions on Electromagnetic Compatibility.

[8]  Amelia Rubio Bretones,et al.  Extension of the ADI-FDTD method to Debye media , 2003 .

[9]  K. Fujita Hybrid Newmark-Conformal FDTD Method for Multiphysics Modeling of Short Spark Gaps With Curved Metallic Surfaces , 2017 .

[10]  M. A. Stuchly,et al.  Simple treatment of multi-term dispersion in FDTD , 1997 .

[11]  Om P. Gandhi,et al.  A frequency-dependent finite-difference time-domain formulation for general dispersive media , 1993 .

[12]  A Taflove,et al.  Direct time integration of Maxwell's equations in linear dispersive media with absorption for scattering and propagation of femtosecond electromagnetic pulses. , 1991, Optics letters.

[13]  K. Yee Numerical solution of initial boundary value problems involving maxwell's equations in isotropic media , 1966 .

[14]  P. Pinho,et al.  Interpolating Wavelets and Adaptive Finite Difference Schemes for Solving Maxwell's Equations: The Effects of Gridding , 2007, IEEE Transactions on Magnetics.

[15]  Yansheng Jiang,et al.  A hybrid implicit‐explicit FDTD scheme with weakly conditional stability , 2003 .

[16]  Bernard Jecko,et al.  Modelling of dielectric losses in microstrip patch antennas: application of FDTD method , 1992 .

[17]  Gaofeng Wang,et al.  PLRC-WCS FDTD Method for Dispersive Media , 2009, IEEE Microwave and Wireless Components Letters.

[18]  Ichiro Fukai,et al.  A treatment by the FD‐TD method of the dispersive characteristics associated with electronic polarization , 1990 .

[19]  U. Navsariwala,et al.  An unconditionally stable finite element time-domain solution of the vector wave equation , 1995 .

[20]  Kazuhiro Fujita Complex-Frequency Shifted PML Formulation for the 3-D MNL-FDTD Method , 2016, IEEE Microwave and Wireless Components Letters.

[21]  3-D MNL-FDTD Formulation in General Orthogonal Grids , 2016, IEEE Antennas and Wireless Propagation Letters.

[22]  R. J. Luebbers,et al.  Piecewise linear recursive convolution for dispersive media using FDTD , 1996 .

[23]  Yoichi Kochibe,et al.  Poynting の活用事例 Application Examples of Electromagnetic Wave Simulation Software “ Poynting ” in Manufacturing Industry , 2013 .

[24]  Eng Leong Tan,et al.  Corrected Impulse Invariance Method in Z-Transform Theory for Frequency-Dependent FDTD Methods , 2009, IEEE Transactions on Antennas and Propagation.

[25]  A Frequency-Dependent Weakly Conditionally Stable Finite-Difference Time-Domain Method for Dispersive Materials , 2010 .

[26]  Raymond J. Luebbers,et al.  FDTD for Nth-order dispersive media , 1992 .

[27]  Dennis M. Sullivan,et al.  Z-transform theory and the FDTD method , 1996 .

[28]  Nathan M. Newmark,et al.  A Method of Computation for Structural Dynamics , 1959 .

[29]  K. Fujita Multiscale Modeling of a Short Relativistic Electron Bunch Interacting With Long Resistive Structures at Cryogenic Temperatures , 2016, IEEE Journal on Multiscale and Multiphysics Computational Techniques.

[30]  M. Stumpf,et al.  Efficient 2-D Integral Equation Approach for the Analysis of Power Bus Structures With Arbitrary Shape , 2009, IEEE Transactions on Electromagnetic Compatibility.

[31]  Zhizhang Chen,et al.  Numerical dispersion analysis of the unconditionally stable 3-D ADI-FDTD method , 2001 .

[32]  Joe LoVetri,et al.  Efficient Evaluation of Convolution Integrals Arising in Fdtd Formulations of Electromagnetic Dispersive Media , 1997 .

[33]  Juan Chen,et al.  Comparison between HIE‐FDTD method and ADI‐FDTD method , 2007 .

[34]  Extension of the magnetically mixed Newmark-Leapfrog finite-difference time-domain method to Debye dispersive media , 2017, 2017 IEEE International Conference on Computational Electromagnetics (ICCEM).

[35]  Dennis M. Sullivan,et al.  Frequency-dependent FDTD methods using Z transforms , 1992 .

[36]  Baruch Levush,et al.  A leapfrog formulation of the 3-D ADI-FDTD algorithm , 2009 .

[37]  D. Pommerenke,et al.  Wide-band Lorentzian media in the FDTD algorithm , 2005, IEEE Transactions on Electromagnetic Compatibility.

[38]  Susan C. Hagness,et al.  Errata to "On the accuracy of the ADI-FDTD method" , 2002 .

[39]  M. Leone The radiation of a rectangular power-bus structure at multiple cavity-mode resonances , 2003 .

[40]  Eng Leong Tan,et al.  Fundamental Schemes for Efficient Unconditionally Stable Implicit Finite-Difference Time-Domain Methods , 2008, IEEE Transactions on Antennas and Propagation.

[41]  T. Sarkar,et al.  Wideband frequency-domain characterization of FR-4 and time-domain causality , 2001, IEEE Transactions on Electromagnetic Compatibility.

[42]  B. Levush,et al.  A Leapfrog Formulation of the 3D ADI-FDTD Algorithm , 2007, 2007 Workshop on Computational Electromagnetics in Time-Domain.

[43]  K. Fujita Nonlinear MNL-FDTD scheme for short-gap electrostatic discharge simulation , 2016 .