Abstract
AbstractA three‐dimensional implementation of the lumped‐element by Crank‐Nicolson finite‐difference time‐domain (CN‐FDTD) algorithm has been presented in this article. Several examples of planar microwave circuits with lumped resistor, capacitor, and/or inductor are simulated and compared with traditional finite‐difference time‐domain method and measurements. The accuracy of CN‐FDTD implementation for lumped elements in this article has been verified. © 2008 Wiley Periodicals, Inc. Microwave Opt Technol Lett 51: 113–116, 2009; Published online in Wiley InterScience (www.interscience.wiley.com). DOI 10.1002/mop.23969
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