
Time
Domain
RCS
Measurements
Gating
During
RCS
Calibration
The
HP
8530A
RCS
Calibration
procedure
allows
you
to
use
gating
during
calibration.
The
gated
calibration
applies
the
Gate
to
the
frequency
response
error
term
(Er)
only
,
allowing
removal
of
the
eects
of
shadowing
and
scattering
caused
by
the
reference
target.
Gating
(during
RCS
calibration)
better
characterizes
the
reference
target
and
the
frequency
response
error
(Er)
of
the
measurement
system.
The
\Gating
during
Calibration"
feature
is
located
in
the
T
arget
Response
menu.
There
are
two
selections:
NNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNN
GATING
YES
If
selected,
the
HP
8530
will
use
the
current
gate
settings
during
the
gated
calibration.
If
Gating
is
currently
turned
OFF
,
the
HP
8530
will
prompt
you
to
rst
set
up
and
turn
on
the
gate
before
measuring
the
reference
target.
NOTE:
you
can
re-enter
the
existing
calibration
by
pressing
\RESUME
CAL".
Once
you
have
set
up
the
gate
,
you
do
not
have
to
start
the
calibration
over
again.
NNNNNNNNNNNNNNNNNNNNNNNNNNNNN
GATING
NO
If
selected,
no
gate
is
used
(in
the
calibration),
regardless
of
whether
gating
is
turned
ON
or
OFF
.
With
gating
ON
during
RCS
calibration,
the
receiver
applies
the
current
Time
Domain
gate
settings
to
the
data
that
results
from
the
raw
measured
data
of
the
reference
target
minus
the
background.
The
gate
provides
better
characterization
of
the
reference
target,
because
it
removes
the
eects
of
interactions
of
the
reference
target
with
the
test
chamber
.
Gating
can
remove
the
eects
of
reference
target
scattering,
and
it
can
also
reduce
the
eects
of
reference
target
shadowing.
Remember
that
gating
only
removes
responses
that
lie
outside
of
the
gate
.
Setting
the
Gate
for
a
Gated
RCS
Calibration
Y
ou
should
select
gate
Start,
Stop
,
Center
,
and
Span
times
while
viewing
the
reference
target
response
in
the
Time
Domain.
Make
the
gate
span
wide
enough
to
include
the
full
target
zone
response
.
At
minimum,
the
gate
span
should
be
at
least
wide
enough
to
be
centered
on
the
peak
response
of
the
reference
target
and
include
its
full
Time
Domain
response
.
If
your
target
is
a
sphere
,
the
placement
of
the
gate
is
critical.
Spheres
produce
a
secondary
reection
caused
by
RF
energy
propagating
around
the
back
of
the
sphere
,
which
ultimately
arrives
back
at
the
receive
antenna.
This
produces
the
secondary
reection,
known
as
a
\creeping
wave
,"
located
in
time
by
(2
+
)
2
radius
2
c
(c=velocity
of
light)
after
the
main
(specular)
response
from
the
front
of
the
sphere
.
If
the
creeping
wave
is
clearly
separate
from
the
main
target
response
,
place
the
gate
around
just
the
main
response
.
In
this
case
make
sure
you
select
the
NNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNN
OPTICAL
SPHERE
model
when
you
dene
the
RCS
target
(as
explained
the
section
on
RCS
calibration).
If
the
main
target
response
and
the
creeping
wave
are
not
clearly
distinct
and
separate
,
position
the
gate
around
both
of
them.
In
this
case
make
sure
you
select
the
NNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNNN
TARGET:
SPHERE
model
when
you
dene
the
RCS
target.
Because
the
gate
start
and
stop
indicators
show
the
06
dB
points
of
the
gate
lter
,
it
is
important
to
locate
them
beyond
the
peak
of
the
responses
that
are
to
be
kept
within
the
gate
to
prevent
distorting
the
responses
.
Do
Not
Use
Gating
When
.
.
.
Y
ou
are
measuring
a
small
frequency
span
or
number
of
points
.
If
using
a
frequency
list
where
the
points
are
not
evenly
spaced.
Introduction
to
Time
Domain
RCS
and
Antenna
Measurements
13-15
Содержание 8530A
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