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Boonton Electronics 71A, 71AR - Differential Capacitance Measurements

Boonton Electronics 71A, 71AR
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from
approximately
10
pF
to
1000
pF.
Because
this
correc-
tion
factor
is
very
nearly
a
direct
function
of
cable
length,
for
small
corrections
(10%
or
less),
the
correction
required
for
pairs
of
other
lengths
can
be
readily
computed.
3.5
Increasing
the
Capacitance
Measuring
Range
The
upper
capacitance
limt
of
1000
pF
may
be
increased
by
a
factor
of
up
to
approximately
10
(to
O.Oll-LF)
by
use
of
the
"DIFF"
posts,
as
follows:
(a)
Set
the
instrument
to
the
1000
pF
range.
(b)
Attach
a
high
quality
mica
capacitor
whose
value
accurately
known
to
the
"DIFF"
terminals.
is
(c)
Attach
the
specimen
to
the
"TEST"
terminals.
(d)
The
sum
of
the
meter
reading
and
the
value
of
the
capacitor
at
the
"DIFF"
terminals
is
the
value
of
the
test.
NOTE
The
value
of
the
capacitor
at
the
"DIFF"
terminals
should
be
selected
to
provide
at
least
15%
of
full
scale
deflection
for
most
satisfactory
results.
It
should
be
noted
that
while
significant
measurements
can
be
made
in
this
manner,
accuracy
will
be
degraded
somewhat
from
that
specified
for
the
normal
operating
range
of
the
instrument.
3.6
Differential
Capacitance
Measurements
Measurement
of
the
capacitance
differential
between
two
speci-
mens
may
be
made
by
attaching
one
sample
at
the
"DIFF"
terminals
and
the
other
to
the
"TEST"
terminals,
using
all
but
the
1
pF
range.
The
scale
will
read
the
capacitance
differential
directly
in
pF.
(NOTE:
If
a
down-scale
reading
is
obtained,
interchange
the
specimens
connected
to
the
"TEST"
and
"DIFF"
posts
for
an
up-scale
reading.)
The
measurements
must
be
made
using
the
range
on
which
one
of
the
specimens
alone
would
normally
be
measured,
or
one
range
below
this
for
increased
resolution.
However,
it
is
important
not
to
switch
down
more
than
I
range
or
serious
errors
may
be
introduced.
Remote
differential
measurements
may
also
be
made
using
coaxial
cables
3-10
7lA
d