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CreatorTitleDescriptionSubjectDate
1 Furse, Cynthia M.Design of implantable microstrip antenna for communication with medical implantsThe objective of this paper is to design a microstrip patch antenna for communication with medical implants in the 402-405-MHz Medical Implant Communications Services band. Microstrip antenna design parameters are evaluated using the finite-difference time-domain method, and are compared to measure...Biocompatible antenna; Medical Implant Communications Services; MICS; Pacemaker antenna; Medical implants2004-08
2 Furse, Cynthia M.; Gandhi, Om P.; Lazzi, GianlucaElectromagnetic absorption in the human head and neck for mobile telephones at 835 and 1900 MHzWe have used the finite-difference time-domain method and a new millimeter-resolution anatomically based model of the human to study electromagnetic energy coupled to the head due to mobile telephones at 835 and 1900 MHz. Assuming reduced dimensions characteristic of today's mobile telephones, we h...Electromagnetic absorption; FDTD; Finite-difference time-domain; Specific absorption rates; SAR1996-01-01
3 Christensen, Douglas A.Extending the two-dimensional FDTD method to hybrid electromagnetic systems with active and passive lumped elementsThis paper extends the finite-difference time-domain (FDTD) method to include distributed electromagnetic systems with lumped elements (a hybrid system) and voltage and current sources. FDTD equations that include nonlinear elements like diodes and transistors are derived. Calculation of driving-p...Finite-difference time-domain method; Lumped elements1992-04
4 Furse, Cynthia M.; Gandhi, Om P.Improvements to the finite-difference time-domain method for calculating radar cross section of a perfectly conducting targetAbstract -The finite-difference time-domain (FDTD) method has been used extensively to calculate scattering and absorption from both dielectric objects and perfectly conducting objects. Several improvements to the FDTD method for calculating the radar cross section (RCS) of a perfectly conducting ta...Finite-difference time-domain method; FDTD; RCS; Perfectly conducting target1990-07
5 Furse, Cynthia M.; Gandhi, Om P.Improvements to the finite-difference time-domain method for calculating the radar cross section of a perfectly conducing targetThe finite-difference time-domain (FDTD) method has been used extensively to calculate scattering and absorption from both dielectric objects and perfectly conducting objects. Several improvements to the FDTD method for calculating the radar cross section (RCS) of a perfectly conducting target are p...Finite-difference time-domain; FDTD1990-01-01
6 Christensen, Douglas A.Modeling sources in the FDTD formulation and their use in quantifying source and boundary condition errorsThe modeling of voltage and current sources as either added or replaced sources in FDTD simulations is described and their differences discussed in terms of a transmission line analogy. An infinitesimal current element (ICE) is used to illustrate the validation of added source modeling and to study...Finite-difference time-domain method; Infinitesimal current element1995-04
7 Furse, Cynthia M.; Gandhi, Om P.Simple convolution procedure for calculating currents induced in the human body for exposure to electromagnetic pulsesThe finite-difference time-domain (FDTD) and frequency dependent finite difference time-domain (FD)2TD methods have been previously used to calculate internal electric (E) fields and induced currents for exposure of the anatomically based model of the human body to electromagnetic pulses (EMPs) and...Frequency dependent finite difference time-domain; Finite-difference time-domain; FDTD; Electric fields; Induced current; Electromagnetic pulses; Continuous wave sinusoids1994-07
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