|
Excitation of a Hertzian dipole field
|
Excitation of a Hertzian dipole field into an FDTD region using the total-field/scattered-field formulation
This research is aimed towards the development of improved methods for
time-domain simulations of EM propagation through inhomogeneous media
such as human body tissue. A new time-domain method has been developed
and implemented. The advantages of which include: 1) high accuracy, 2)
high efficiency, 3) isotropic numerical dispersion error, 4) increased
stability allowing larger time steps, and 5) straightforward implementation
of PML absorbing boundary conditions.
Excitation of a Hertzian dipole field
This is novel because it allows a dipole excitation for an arbitrarily
oriented dipole without incurring errors due to staircasing. Also,
any number of dipoles may be excited via superposition.
SAR distributions for the sagittal slice (scale is in dB)
SAR distributions for the frontal slice (scale is in dB)
SAR distributions for the coronal slice (scale is in dB)
A method of moments code was used to solve for the currents on a
center-fed half wavelength wire antenna operating at 900 MHz. The
resulting current elements are treated as a string of dipoles and were
excited into the FDTD region using the Hertzian dipole excitation of
the first Figure (excitation of a Hertzian dipole field).
The above figures are specific absorption rate (SAR) distributions for
the center-fed half-wavelength antenna next to a
human head.
The Figures show the comparison of the numerical dispersion error 1-w/kc as
a function of propagation direction at 10 cells/wavelength for the Yee
algorithm and the present algorithm.
![]() Yee algorithm dispersion error ![]() Present algorithm dispersion error
These figures come from a novel time-domain method that was developed in
Eric Forgy's M.S. thesis. The title is
"A Time-Domain Method for Computational Electromagnetics with
Isotropic Numerical Dispersion on an Overlapped Lattice."
The following Figures show the total and scattered fields for a plane
wave at 10 cells/wavelength with the optimized algorithm, the combined
algorithm, and the Yee algorithm.
Total and scattered fields for the optimized algorithm
Total and scattered fields for the combined algorithm
Total and scattered fields for the Yee algorithm
The optimized and combined algorithms are from Eric Forgy's thesis. The
bleeding of the fields from the total-field to the scattered-field
region is a result of phase error as the wave propagates from front
to back. The optimized algorithm has essentially no error, the
combined algorithm has phase error but is a great improvement over
the Yee algorithm.
The above work is a collaboration between Eric Forgy and Prof. Weng Cho Chew. Please send suggestions, comments, and inquiries to: forgy@students.uiuc.edu.
|
Electrical and Computer Engineering Department
webmaster@ccem.uiuc.edu
Copyright © 1998-2002