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Philips PM 6672 - Page 12

Philips PM 6672
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14
The
low-pass
filter
The
built-in
50kHz
low-pass
filter
is
used
for
improved
triggering
on
noisy
LF-signals.
The
filter
characteristic
is
shown
in
Fig.
3.6.
It
is
also
possible
to
use
this
filter
for
signals
with
frequencies
above
50kHz,
but
at
a
reduced
sensitivity.
SO
-
A
t
ienuQ
i
ion
in
d
B
AO
-
30-
20-
JO-
ErcCfucncy
in
MHz
1
1
1
0.02
0.05
0.1
0.2
1
1
0.5
\
2
Fig.
3.6.
The
low—pass
filter
reduces
noise
and
inter
ference.
Input
C
PM
6672
has
a
special
RF
input,
called
input
C.
Note
that
not
more
than
1
2Vrivis's
allowed
at
input
C
and
that
the
input
sensitivity
is
adjusted
automatically.
MEASURING
MODES
Frequency
A,
Period
A
and
RPM
PM
6670...72
perform
a
frequency
and
period
measurement
as
given
in
the
definitions;
Frequency
Period
=
Number
of
cycles
Time
Time
Number
of
cycles
The
counter:
1
.Measures
the
effective
measuring
time.
2.Counts
the
number
of
input
cycles
during
the
measuring
time.
3.Computes
the
number
of
cycles
per
second
(frequency)
or
time
units
per
cycle
(period).
The
measurement
is
synchronized
with
the
input
signal.
This
is
called
the
input
synchronized
or
reciprocal
method.
In
the
input
synchronized
mode,
both
the
opening
and
closure
of
the
main
gate
is
synchronized
with
the
input
signal,
so
that
only
completed
input
cycles
are
counted.
This
means
that
a±1
input
cycle
error
is
avoided.
During
the
gate
time,
the
counter
also
totalizes
the
number
of
100ns
crystal
clock
cycles;
see
Fig.
3.7.
fOOns
X-
TAL
CLOCK
TRiGGCR
OUTPUT
"MEASURE'
S
yNCHRON/EC
GATE
SIGNAL
CO
UN
TED
INPU
T
CYCLES
TIME
COUNTS
[Nurnber
of
/OOns
clockpu
(ses
)
COUNTED
INPUT
CYCLES
rRcguENcv
TIM£
COUNTS
'
10-''s
COUNTCD
INPUT
CYCLES
Fig.
3.7.
input
synchronized
mode.
The
resolution
in
the
input
synchronized
mode,
is
caused
by
truncation
of
the
clock
pulses,
which
results
in
a
±
1
clock
pulse
error
(100ns).
The
resolution
of
the
measurement
thus
only
depends
on
the
measuring
time,
e.g.
the
resolution
for
Is
measuring
time
is
10"'
(lOOns/ls)
independent
of
frequency.
In
conventional
counters,
the
gate
time
is
synchron
ized
with
the
clock
signal.
The
first
and
last
input
cycle,
can
therefore
be
truncated,
causing
a
±1
cycle
error.
This
results
in
a
good
resolution
for
high
frequency
measurements,
but
a
poor
resolution
for
low
frequency
measurements
(±1/frequency
for
Is
measuring
time).
A
RPM
measurement
is
in
fact
a
normal
frequency
mea
surement,
but
the
microcomputer
multiplies
the
fre
quency
for
60
before
displaying
the
result.
Measuring
time
The
measuring
time
can
be
varied
in
33
steps
per
decade
between
10ms
and
96s.
Set
measuring
time
can
be
displayed
by
pushing
the
measuring
time
rotary
knob.
This
resets
the
counter
and
a
new
measurement
will
start.
The
counter
continues
to
totalize
input
cycles
until
the
set
measuring
time
has
elapsed
and
the
synchronization
conditions
are
met.
Hence,
the
effective
measuring
time
(also
called
gate
time)
is
longer
than
the
set
measuring
time.

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