HAGAN et al.: NOVEL WAVEGUIDE-BASED RF/MW EXPOSURE SYSTEM FOR STUDYING NONTHERMAL EFFECTS
1675
IV. CONCLUSION
A novel system for the in vitro exposure of chromaffin cells
for identifying RF/MW field effects on neurotransmitter release
has been designed. The combination of a standard waveguide
and a cell perfusion apparatus constructed of nonmetallic mate-
rials allows online monitoring of catecholamine release during
RF/MW exposure. A detailed characterization of this exposure
system using the FDTD method has allowed estimation of the
optimal design of exposure procedures that will provide the
most homogeneous SAR over the region containing the cells.
field max-
Positioning the cell perfusion chamber at the
imum provides a higher SAR than that which can be achieved
at the maximum of for a given net input power into the wave-
guide. However, acceptable homogeneity is achieved only when
the field is parallel to the plane of the glass fiber filter. These
modeling results clearly indicate that the orientations of the
plane of the glass fiber filter and the narrow BSS channel with
respect to the field direction in the waveguide are strong fac-
tors in determining not only the magnitude of the SAR but also
its distribution in the region of the glass fiber filter.
In actual experiments, it will not be possible to control the
distribution of the cells on the glass fiber filter. However, the
FDTD results enable precise determinations of where field en-
hancements (electrical hot spots) occur. Knowing their locations
is important for two reasons. First, steps can be taken to mini-
mize them. For example, hot spots in SAR created by the exis-
tence of sharp corners and edges in the BSS flow channel in the
vicinity of the glass fiber filter can perhaps be greatly minimized
by modifying the geometry of the junction of the flow channel
in this region. Second, interpreting the outcomes of experiments
using the predicted knowledge of SAR distributions over the
filter will be facilitated. Because the location of the cells on the
glass fiber filter can be determined at the end of an experiment
by staining the cells with the dye neutral red, the magnitude of
Fig. 8. (a) Contour and (b) surface plot of the SAR distribution across the
any changes in catecholamine release can be correlated with the
glass fiber filter (location of chromaffin cells) computed by XFDTD for the
density of cells in regions of high SAR.
parallel orientation. Cell perfusion apparatus is at the
field maximum.
Forward power
W, frequency
GHz.
ACKNOWLEDGMENT
The authors would like to thank M. Trakas, R. Dopf, and
fairly uniform (except for a very small region at the center) in
D. Bhakta for assistance in characterizing the different compo-
a large part of the filter (Fig. 8). The two electrical hot spots
nents of the cell perfusion apparatus. They also acknowledge
adjacent to the central region once again coincide with the loca-
the technical support of R. Brourman, Dr. R. Luebbers, and
tion of the narrow BSS flow channel joining the filter section of
C. Penney of REMCOM, Inc.
the cell perfusion apparatus. Thus, the SAR distribution has a
striking resemblance to that obtained when the glass fiber filter
is placed at the maximum in with the field perpendicular
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