1999
DOI: 10.1002/(sici)1099-1204(199901/04)12:1/2<157::aid-jnm323>3.0.co;2-v
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Incorporating non-linear lumped elements in FDTD: the equivalent source method

Abstract: A new approach is presented for modelling three‐dimensional lumped elements in the finite‐difference time‐domain (FDTD) solution of Maxwell's equations. The finite‐difference equations for the lumped element's circuit behaviour are derived to produce discrete relationships between the device's terminal currents and voltages. These difference equations are then implemented in the FDTD grid with equivalent voltage and current sources based on static field approximations. The method can be used for a wide range o… Show more

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Cited by 9 publications
(5 citation statements)
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“…To the best of the authors' knowledge, the implementation of dependent sources using FDTD has not been adequately addressed before. In addition, in most of the previous work the implementation of nonlinear devices such as transistors has been handled using FDTD-SPICE models or by importing the S-parameters from another technique to the FDTD simulation [2]- [7]. In this work the implementation of the VCCS in FDTD will be used to simulate a MOSFET with its equivalent model without the use of external tools, the entire simulation can be done using the FDTD.…”
Section: Introductionmentioning
confidence: 77%
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“…To the best of the authors' knowledge, the implementation of dependent sources using FDTD has not been adequately addressed before. In addition, in most of the previous work the implementation of nonlinear devices such as transistors has been handled using FDTD-SPICE models or by importing the S-parameters from another technique to the FDTD simulation [2]- [7]. In this work the implementation of the VCCS in FDTD will be used to simulate a MOSFET with its equivalent model without the use of external tools, the entire simulation can be done using the FDTD.…”
Section: Introductionmentioning
confidence: 77%
“…4. The values of the equivalent circuit parameters according to [7] are as follows: C gd = 0.06pF, C gs = 0.96pF, C ds = 0.26pF, g m =10 mS and R ds = 197 Ω. The FDTD grid cell size is ∆x = ∆y = ∆z = 0.25 mm, the circuit is simulated with 5×1×2 in x, y and z-directions respectively, 1000 time steps are used, CPML is used as the absorbing boundaries of the computational domain with 5 cells air buffer in every direction.…”
Section: B Test Case 2 (Mosfet Circuit)mentioning
confidence: 99%
“…In general, lumped elements can be incorporated into the FIT by formally adding a supplementary current j L due to the lumped element in Ampère's circuital law (3.16) [62,63]:…”
Section: Lumped Elementsmentioning
confidence: 99%
“…In order to derive the iteration procedure, at each time step we relate Gummel's method to direct UMFPACK method which is well known to converge quadratically [7]. The Equations (10), (11) and (12) are solved in a decoupled manner. Poisson equation is solved at all grid points, followed by electron continuity equation, and then by hole continuity one.…”
Section: Numerical Wholementioning
confidence: 99%
“…These equations are first-order linear the field vectors at any point in the space at any time. The current density distribution is obtained from the solution of the driftdiffusion model [11,12].…”
Section: Electromagnetic Wave Approximationmentioning
confidence: 99%