
PATA
[YPE
I
l2
2
2
2
01:
02:
03:
04:
4
'4
4
iFP
FP
05:
06:
07:
08:
09:
PARAM.
NUMBER
DESCRIPTION
Repetitions
Range code
Input
channel
number for
first measurement
Excitation channel
number
Delay
(0.01s)
Excitation
voltage
(millivolts)
Input
location
number for
first
measurement
Multiplier
Offset
Input locatiQns altered:
1
per
measurement
***
9 FULL
BRIDGE
WITH EXCITATION
***
COMPENSATION
FUNCTION
This
instrucfion
is used to
apply an excitation
voltage
and
make two differential
voltage
meas
then
reverse the
polarity
of the
excitation afrd repeat
the
measurements. The
measu are
made on sequential
result
is the voltage
measured on
the
exci
channel
SECTION
9.
INPUT/OUTPUT
INSTRUCTIONS
PARAM.
DATA
NUMBER
TYPE DESCRIPTION
Repetitions
Range code
for Vl
Range code
for
V2
Input channel
number
for
first measurement
Excitation
channel
number
Excitation
voltage
(millivolts)
Input location
number
for
first measurement
Multiplier
Offset
lnput
locations altered:
1
per
measurement
***
10
BATTERY
VOLTAGE
***
FUNCTION
This
instruction reads
the
battery
voltage and
writes it to an input
location. Battery
voltage is
stored
in
volts.
PARAM. DATA
NUMBER
TYPE
DESCRIPTION
01:
4
Input location
Input
locations altered:
1
***
11
107
THERMISTOR
PROBE
***
FUNCTION
This
instruction
applies
a 4
VAC excitation
voltage
to Campbell Scientific's
Model
107
Thermistor
Probe, makes a fast, single-ended
voltage
measurement on the
15mV
range and
then calculates
the temperature
in degrees C
with a
polynomial.
The maximum
polynomial
error
from
-40oC
to
+55oC
is
given
below:
Curve
Fit Error
--
Range
(oC)
2
2
2
2
2
4
4
FP
FP
01:
02:
03:
o4:
05:
06:
07:
08:
09:
channels.
the secondthe second
phannel (Vr)
divided by
the
voltage
measured
Qn
the first
(V1).
lf
V1 is measured
on
(code
5
or
15 in Parameter 2),
then the
is 1000
timesV2A/1.
Al before
number
(1X)
causes the
channelto
be
incremented
with
each
repetition.
When used
as
a
6
wire full
bridge
(Figure
13.5-
1), the
conrtections
are
made
so
that
V.t
is
the
measuremQnt
of the
voltage drop
across the
full
bridge,
and
V2
is the
measurement
of the bridge
output.
Bedause the
excitation
voltage
for
a
full
bridge
meaburement
is usually
in
the
5V range,
the
output
i$ usually
1000
V2A/1 or
millivolts
output
per
volt
excitation.
When used
to measure
a
4
wire
half bridge, the
connectionq
are made
so that
V1 is the
voltage
drop
acrosg
the fixed
resistor
(R),
and
Vr
is the
drop
acrosg
the
sensor
(R.).
As
long as V1 is
not
measurpd on
the 5V
range, the
result is
VrA/1
whic$ equals
Rs/Rf.
The
fast integration time used
in Instruction 11
does
not
provide
rejection of 60
Hz noise. See
example
7.16 for a
method of
measuring the
107 thermistor
where 60 Hz
noise
is a
problem.
-40
to +55
-35
to
+48
Error
(oC)
+1.0
+0.1
9-5
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