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What to Look for in an EMC Antenna
The standard that defines the requirements for
antennas to be used in EMC measurement is CISPR
publication 16-1: 1993, "Specification for Radio
Disturbance and Immunity Measuring Apparatus and
Methods, Part 1."
CISPR measurements officially require tuned
dipoles, but a note in most standards allows the
use of broadband antennas where they can be shown
to give equivalent results. For this to be the case,
the antenna must be calibrated to yield an antenna
factor (AF).
The allowed system uncertainty in CISPR 16
is ±3 dB, comprising the receiver, antenna,
cable loss, and mismatch uncertainties, but not
including the test site. Directivity should be low
so that signals from off-axis are not significantly
attenuated. CISPR 16 mandates linear polarization.
The VSWR (Voltage Standing Wave Ratio) should be
less than 2:1, which, strictly speaking, demands
an attenuator on the output of most biconical antennas.
Types of Broadband Antennas
Historically, the two types of antenna used
for emissions measurement have been the biconical
and the log-periodic. These are electric-field linear
polarized and typically cover complementary frequency
ranges from 30 to 300 MHz and 300 to 1000 MHz, respectively.
Early biconical designs could reach only 200 MHz,
but a modification to the structure has removed
a resonance between 200 and 300 MHz, allowing that
specification to be stretched.
The two types can also be combined into one
device that will exhibit the characteristics of
each of its components over the relevant frequency
range (see Figure 1). Because these antennas are
so commonly used, the correlation between measurements
from different test facilities is generally quite
good.
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| Figure 1. Common antenna types are a) BiLog,
b) log-periodic, and c) biconical |
Some other antenna types on the market are based
on different principles than the biconical and log-periodic.
One such antenna is the log spiral, which receives
or generates fields with circular rather than linear
polarization; it is widely utilized for military
susceptibility tests but is unsuited to commercial
IEC/CISPR testing. Other types of biconical are
sometimes used, but the lower frequency limit of
30 MHz places a fundamental constraint on their
size and construction, and more compact designs
that do not obey this limit inevitably have compromised
performance.
The maximum achievable field strength, as
shown in Figure 2, is related to the power that
can be radiated from the antenna: for a dipole,
the field strength E (V/m) at a distance d (meters)
with P (watts) radiated is calculated according
to the formula
E=7
Power handling is principally a function of the
balun design. Some power is dissipated in the balun,
and the resulting temperature rise limits the power
that can be applied. Good VSWR is essential to minimize
the power reflected from the antenna and hence to
make the best use of the power amplifier's capabilities.
For these reasons, many antennas designed for radiated
emissions testing cannot be used for radiated immunity.
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| Figure 2. Antenna as a source of RF immunity
test field. |
Low directivity maximizes the area that can be
covered with a constant field strength. IEC 61000-4-3
mandates a uniform area of field at the position
at which the EUT is located, a condition that is
affected not only by reflections from the walls
of the screened room but also by the uniformity
of coverage of the antenna. To cover a given area,
a narrow-beam-width antenna must be located farther
away from the EUT. If even a broad-beam antenna
is too close, different parts of the elements will
be at significantly different distances from the
EUT, and uniformity will suffer.
The field strength E is obtained by multiplying
the voltage V at the receiver by the AF, allowing
for attenuation in the connecting cable. The conversion
can be expressed in dB by
E(dBµV/m) = V(dBµV) +
AF(dB/m) + A(dB)
Since the noise floor of the measuring instrument
(minimum measurable V) is fixed, a good system noise
floor (minimum measurable E) requires a low antenna
factor.
It has become common practice to use an antenna
factor that applies to operation in free space with
a 50 load. The AF varies with the antenna's
proximity to the groundplane and the EUT. Errors
due to mutual coupling cannot be avoided, but if
all the test antennas used are based on a similar
design, they will at least be consistent. With small
EUTs, mutual coupling is unlikely even at 3 m to
cause errors greater than 1 dB. For a biconical
or combination antenna, variation of the AF according
to the antenna's height above the groundplane is
most pronounced in horizontal polarization and is
typically 1 dB at resonance (around 70 MHz), falling
to 0.5 dB above 300 MHz.
Variations in the slope of the AF curve due to
resonances are undesirable. The AF values are generally
programmed into test software that interpolates
for a particular frequency; for minimum error, a
smooth curve is essential.
Polarization, Polar Pattern, and Distance
When a single antenna factor is specified, an assumption
has been made that the antenna will be used under
conditions of maximum gain. For the log-periodic
antenna, this is in the direction toward which the
antenna is pointing, while for the biconical, it
is perpendicular to the antenna axis. In all other
directions, the response of the antenna falls off
and the antenna factor becomes invalid. The polar-pattern
response for a dipole is within 1 dB of the on-axis
value over an azimuth variation of 45°; for
a log-periodic array, the beam is narrower. This
is particularly significant when the antenna is
used at high frequencies with a height scan from
1 to 4 m and a close-in distance of 3 m. Under such
conditions, the antenna will no longer be properly
aligned with the EUT, and an error may result.
Polarization of the antenna refers to the
plane of polarization of the electric-field component.
CISPR 16 requires that the cross-polarization be
better than 20 dB, which implies that the design
of the antenna must ensure linear polarization.
EMC testing requires a fixed and known distance
between the antenna and the EUT. In log-periodic
or combination antennas, the active element (known
as the phase center) shifts with frequency, and
so the measuring distance must change. It is therefore
a practical necessity to choose a specific point
on the antenna boom against which the AF should
be calibrated and to mark this permanently on the
antenna itself.
Antenna VSWR affects the accuracy of emissions
measurements and the power required to perform radiated-immunity
tests. The mismatch uncertainty on receiver measurements
is given by the formula
U(dB) = 20log10
(1 ± |rA|
|rR|)
where rA
and rR
are antenna and receiver reflection
coefficients, given by the formula
The CISPR 16 requirement calls for a maximum
antenna VSWR of 2:1. This is rarely met in practice
below about 80 MHz, but with this figure for both
antenna and receiver, the uncertainty from the above
equations is +0.9/1.0 dB.
Most EMC antennas employ similar mechanical
designs and thus have many comparable properties.
One parameter of which this is not true, however,
is balun design. The antenna balun converts from
the unbalanced coax feed to the balanced termination
between the antenna elements; the resulting balance
may be assessed by comparing signals received in
the two possible vertical orientations. A well-designed
balun will limit the difference to less than 1 dB,
while a poor one may show differences greater than
10 dB.
Poor balance will evidence itself in several
ways. The antenna factor clearly is going to depend
on how the antenna is mounted and will be different
for horizontal and vertical polarizations. Equally
important is the fact that poor balance will severely
affect the uncertainty due to proximity to the ground
and to the antenna cable in vertical polarization.
An unbalanced termination will result in appreciable
common-mode RF currents flowing on the sheath of
the antenna cable; these will in turn couple to
the vertical antenna elements and cause a change
in both the polar pattern and the antenna factor.
This problem can be mitigated by locating the antenna
cable far away from the antenna or applying ferrite
sleeves to it, but good balance reduces the need
for such measures.
Ground proximity, for its part, cannot be
avoided; the only way to minimize error is thus
to improve the antenna balance.
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