HUFF et al.: DIRECTIONAL RECONFIGURABLE ANTENNAS ON LAPTOP COMPUTERS
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TABLE I
RESULTS FROM THE EVS
in (3) below), for which the electric
field polarization for these directions can be given as
(3)
IV.
The magnitude of steady state conduction current
on
generated by
density
can then be determined. Once
is known
is revisited on the set
for
residing on
.
of possible locations
Fig. 4. Fabricated model of laptop computer's internal shielding, showing
In the FDTD solution space, this is realized as the
, (for
1, 2, 3, and 4) for antenna integration.
candidate positions,
surface of the laptop with discritized spatial dimensions
confined by
[Fig. 3(e)]. For
V. ELECTROMAGNETIC ENVIRONMENT STUDY
3 [9] is used to perform
this study in particular, XFDTD
In order to fully evaluate the candidate positions for antenna
simulations, and
at 3.7
integration, it is important to take into consideration both the
GHz.
integration parameters around which the antenna will operate
V.
With the information generated in Guideline IV, the
with maximum performance, as well as the conditions that arise
conduction current density in the region(s) confined by
from operation in harsh, unfavorable, or changing electromag-
, (with
being the total number of cells
netic environments. To investigate the environmental effects
), can then be used to find the average
on the antenna as it assumes different positions on the laptop,
, over all incoming an-
conduction current density,
several test environments were created to mimic different
gles,  , and its standard deviation,
working situations. They include: 1) a dielectric surface [Lucite
]; 2) a conductive surface; 3) a dielectric surface with
scattering objects; and 4) a conductive surface with scattering
(4)
objects. These conditions are chosen to represent four basic
environmental conditions likely to be encountered by the laptop
computer. The scattering objects are an assortment of items
(5)
placed in the plane of the laptop (stacks of CDs, beverage
containers, etc.) that serves as one example of possible "real
world" environments.
VI.
Using (4) and (5), the areas of interest
can
be evaluated and ranked using the average steady state
VI. EXPERIMENTAL RESULTS
conduction current densities as well as the standard
.
deviation within the areas confined by
To experimentally verify the results from the EVS, the an-
For the generic laptop computer model used in this study,
tenna was conformally mounted onto the laptop chassis such
the candidate positions  can be seen in Fig. 4 and the results
plane of the antenna, was aligned with
that the H plane, or
from the EVS for these positions presented in Table I. For this
the azimuthal plane of the laptop chassis base unit. With the
example, a set of four candidate locations provides a sample
laptop sitting in the horizontal plane, the radiation character-
of nonoverlapping positions for comparison. Table I contains
configuration have linear polarization
istics from 1) the
the rankings of the four candidate locations from high to low
along the diagonal; 2) the
configuration is horizontally po-
visibility based on their respective local current densities and
configurations are vertically polarized.
larized; and 3) the
standard deviations. We hypothesize that positions with higher
For all positions and antenna configurations, input impedance,
and
levels of electromagnetic visibility (higher values of
2:1 VSWR bandwidth, and radiation patterns were measured.
lower values of ) will support antenna operation closer to that
The experimental setup used for this study, including the rel-
of free space.
ative antenna coordinate system on the laptop and the desired
free-space radiation of the reconfigured antenna configurations
3XFDTD
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in their primary polarizations, is shown in Fig. 5. To provide
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