
Equation
13,13-7 can
be solved
for
the
maximum
lead
length,
l,
permitted
to
maintain a
specified
error
limit.
Qombining
Equations
13.3-7 and
13.3-4 and splving for
L
gives:
1-
=
-(RoC1+ (Vln(V"A/"o)))/RoC*
[13.3-15]
where V" is
the
measurement error
limit.
EXAMPLE
I-.]EAD
LENGTH
CALCU
LATION
FOR CAMPtsELL
SCIENTIFIC
107
TEMPERATURE
SENSOR
Assume a
lirhit of O.05oC
over
a OoC
to
+40oC
range is est4blished
for
the
transient
settling
error.
This limit is
a
reasonable
choice
since
it
approximatep
the
polynomial
error
over
that
range.
The
putput
signalfrom
the thermistor
bridge
varie$ nonlinearly
with temperature
(refer
to 107 Operdtor's
Manual),
ranging from about
2oopvfc
atlo"c to l
oopvfc
at
4ooc.
Taking
the
most corfservative
figure
yields
an
error
limit
of
V"
=
5pV. The other values
needed
to
calculate
th( maximum lead
length are
summarized
in Table
13.3-5
and
listed
below:
SECTION
13.
21X
MEASUREMENTS
1)
Veo
=
100mV,
peak
transient
at
4V
excitation
2) V"
=
SltV, allowable
measurement
error
3)
t
=
4501rs, 21X
input
settling time
4) Ro
=
1 kohm,
107
probe
source
resistance
5) Cr
=
3.3nfd,
21X input capacitance
6)
C*=
42pld/ft.,
lead
wire capacitance
Solving Equation
13.3-15
gives
a maximum
lead
length of:
L
=
1003 ft., error
=
0.O5oC
Setting
the allowable
error at 0.1oC or
approximately
1OpV, the maximum
lead length
increases
to:
L
=
1085
ft.. error
=
0.1oC
Input
Range(mV)
15
150
15
500
50
500
TABLE
Sensor
Model
#
Ro Cw
(kohms) (pfd/ft.)
1
1
1
0.1-1
1
0-5
Vx(mV)
V"o(mV)**
4000
100
3000
130
4000
0
500
0
5000
125
1000 0-90
Summary
of Input
Settling
Data For
CampbellScientific
Resistive Sensors
T,*
(us)
107
207(RH)
WVU-7
227
237
o24A
8641
8771
8723
8641
8641
8771
42
41
62
42
42
41
45
44
65
5-45
45
't-222
*
Estimated time constants
are
for 1000
foot
lead lengths
and
include 3.3nfd 21X input capacitance.
**
Measured
peak
transients
for 1000 foot lead lengths at corresponding
excitation, V*.
13.3.4
SUMMAFY
OF
SETTLING
ERRORS FOR
SCIENTIFIC RESISTIVE
SENSORS
Table
13.3-$ summarizes the
data
required
to
estimate
thQ effect
of
lead length
on settling
errors
for
sensors.
the
input
Scientif
ic's resistive
the transient
level, V"o, to
,
one suspects
that transient
errors
are the
most
likely
limitation
for
the 107
sensor.
Thd sensors in the WVU-7
are
the
same as
in
lhe
Model
107
(the
lead
wire
is
different), bqt
the
signal
leads
for the WVU-7
wet and
dry'bulbs are not subject
to excitation
transients
because
they
are
shielded
independently
f rom the excitation.
The
comparatively
smalltransient
yet
large
source resistance of the 0244 sensor
indicates
that
signal
rise time may
be
the rnost
important
limitation. The analysis in Section
13.3.2
confirms
this.
The
Model 227 Soil
Moisture Block has a
relatively
short
time constant and essentially no
transient. Lead
lengths
in excess
of 2000 feet
produce
less than a 0.1 bar
(0-10
bar
range)
input
settling error.
With
this sensor,
the drive
capability of the excitation channel
limits the
13-7
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