Simulation Aids
(continued)
approximated as a solid dielectric. The default time step was
being used in
2.0964 picoseconds in the main grid and 0.420 picoseconds in
experiments. The
the subgrid. Each simulation ran for 9550 time steps.
parallel orientation,
on the other hand,
provides two orders
Validating the Model
of magnitude larger
SAR than when
To test the validity of the XFDTD model, the numerically
the filter is located
computed electric field (E) and magnetic flux density (B) within
at the B field
the waveguide, with the cell perfusion apparatus removed,
maximum. This is
were compared
because the E field
with well-known
is much stronger
waveguide theory
in this orientation
based on measured
and the E field is
values of forward and
Distribution of the Specific Absorption
coupled into the
reflected power. The
Rate in Watts/kg in the region containing
filter according
magnitudes of E and
the biological cells. Here the biological
to the tangential
B at their maxima
cells were assumed to be evenly
boundary
in the standing
distributed over the entire glass fiber
condition. In
wave pattern in
filter. Results are from XFDTD for an input
this orientation,
the waveguide at
power of 0.5W into the waveguide and
homogeneity
a frequency of 1
a frequency of 1 GHz, and are imported
within 30% is
GHz showed good
into SigmaPlot for plotting and analysis.
achieved over
agreement for
83% of the filter
forward powers in
area. The simulation demonstrated that this configuration
the range 0.5-5 W,
and this configuration alone provides the high and consistent
with a maximum
SAR needed to evaluate the exposure of chromaffin cells for
Numerical mesh of the cell perfusion
difference of 8.5%.
identifying RF
apparatus created by XFDTD.
This difference can
field effects on
likely be attributed
catecholamine
to the fact that the computations based on waveguide
release. The
theory utilized values of power measured by a wattmeter
simulation also
having a manufacturer specified accuracy of 5% and that the
provided detailed
waveguide theory computations did not take into account field
SAR values
disturbances caused by the probe launch and waveguide slots.
over the filter.
Knowing the
Determining the Optimal Cell
SAR distribution,
Perfusion Apparatus Position and
together with
Orientation
ability to
determine the
The next step was simulating the waveguide with the cell
location of cells
perfusion apparatus in order to determine a position and
on the glass fiber
orientation for the RF exposure of the cells. The researchers
filter at the end
Figure 5: Distribution of the Specific
first used XFDTD to predict SAR distribution with the cell
of the experiment
Absorption Rate in Watts/kg in the region
perfusion chamber located at the maximum in B. This
by staining the
containing the biological cells. Here the
position with the E field perpendicular to the plane of the
cells with a
same number of biological cells as used in
glass filter provided a very low SAR, on the order of 10-2 W/kg
dye , provides
generating the results shown in Figure 4 were
across the filter. The overall SAR on the filter is small because
the researchers
assumed to be evenly distributed over a small
of the low value of the E field at the maximum of B in the
with important
circular region of diameter 1 cm at the center
standing wave pattern and the E field, being normal to the
information to
of the glass fiber filter. Results are directly
plane of the filter, provides little coupling. Computation of
interpret their
plotted in XFDTD for an input power of 0.5W
the SAR distribution across the filter with the E field parallel
experimental
into the waveguide and a frequency of 1 GHz.
to the plane of the glass fiber showed higher SAR values but
results.
with relatively higher variation of SAR within the filter.
1. T. Hagan, I. Chatterjee, D. McPherson and G.L. Craviso, "A Novel
Researchers next changed the XFDTD model to position the
Waveguide-based Radio frequency/microwave Exposure System for
cell perfusion chamber at the E field maximum. When the
Studying Nonthermal Effects on Neurotransmitter Release ­ Finite-
cell perfusion apparatus was oriented so that the filter was
difference Time-domain Modeling," IEEE Transactions on Plasma Science,
perpendicular to E, the SAR distribution showed dramatic
Vol. 32, August 2004, pp. 1668-1676.
differences that also precluded this configuration from
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