Campbell Scientific CR10 CR10 Measurement and Control - Page 95

Lysimeter, Bridge

Page 95 highlights

SECTION 7. MEASUREMENT PROGRAMMING'EXAMPLES ADJUSTABLE COUNTER BALANCE LOAD CELL FIGURE 7.13-1. Lysimeter Weighing Mechanism 7.13 LYSIMETER - 6 WIRE FULL BRIDGE When a long cable is required between a load cell and the CR10, the resistance of the wire can create a substantialerror in the measurement if the 4 wire full bridge (lnstruction 6) is used to excite and measure the load cell. This error arises because the excitation voltage is lower at the load cellthan at the CRl0 due to voltage drop in the cable. The 6 wire full bridge (lnstruction 9) avoids this problem by measuring the excitation voltage at the load cell. This example shows the errors one would encounter if the actual excitation voltage was not measured and shows the use of a 6 wire full bridge to measure a load cell on a weighing lysimeter (a container buried in the ground, filled with plants and soil, used for measuring evapotranspiration). The lysimeter is 2 meters in diameter and 1.5 melers deep. The totalweight of the lysimeter with its container is approximately 8000 kg. The lysimeter has a mechanically adjustable counterbalance, and changes in weight are measured with a 250 pound (1 13.6 kg) capacity Sensotec Model 41 tension/compression load cell. The load cell has a 4:1 mechanicaladvantage on the lysimeter (i.e., a change of 4 kg in the mass of the lysimeter will change the force on the load cell by 1 kg-force or 980 N). The surface area of the lysimeter is 3.1416 m2 dr 31,416 cm2, so 1 cm of rainfall or evaporation results in a 31.416 kg change in mass. The load ceff can measure t113.6 kg, a227 kg range. This represents a maximum change of 909 kg (28 cm of water) in the lysimeter before the counterbalance would have to be readjusted. There is 1000 feet of 22 AWG cable between the CR10 and the load cell. The output of the load cell is directly proportional to the excitation voltage. When Instruction 6 (4 wire half bridge) is used, the assumption is that the voltage drop in the connecting cable is negligible. The average resistance of 22 AWG wire is 16.5 ohms per 1000 feet. Thus, the resistance in the excitation lead going out to the load cell added to that in the lead coming back to ground is 33 ohms. The resistance of the bridge in the load cell is 350 ohms. The voltage drop across the load cell is equal to the voltage at the CR10 multiplied by the ratio of the load cell resistance, R", to the total resistance, Rr, of the circuit. lf Instruction 6 were used to measure the load cell, the excitation voltage actually applied to the load cell, V1, would be: V1 = V* RS/RT = Vx 350/(350+33) = 0.91 Vx Where V" is the excitation voltage. This means that the voltage output by the load cell would only be 91% of that expected. lf recording of the lysimeter data was initiated with the load cell output at 0 volts, and 100 mm of evapotranspiration had occurred, calculation of the change with Instruction 6 would indicate that only 91 mm of water had-been lost. Because the error is a fixed percentage of the output, the actual magnitude of the error increases with the force applied to the load cell. lf the resistance of the wire was constant, one could correct for the voltage drop with a fixed multiplier. However, the resistance of 7-11

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7.13
LYSIMETER
-
6
WIRE
FULL
BRIDGE
When
a
long
cable
is required between
a
load cell
and
the
CR10,
the
resistance
of
the
wire
can
create a
substantialerror
in
the
measurement if
the
4
wire
full
bridge
(lnstruction 6)
is used
to
excite
and
measure
the
load
cell.
This
error arises
because
the
excitation
voltage
is lower at
the
load
cellthan
at
the
CRl0
due to voltage
drop
in
the
cable.
The
6
wire
full
bridge (lnstruction 9) avoids
this
problem by measuring the excitation
voltage
at
the
load
cell.
This example shows
the
errors one
would
encounter
if
the
actual
excitation voltage
was
not measured and shows
the
use of a
6
wire
full
bridge
to
measure a load cell on
a
weighing
lysimeter
(a
container
buried
in
the
ground, filled
with plants and
soil,
used
for
measuring
evapotranspiration).
The
lysimeter
is
2 meters
in
diameter
and
1.5
melers
deep.
The
totalweight
of
the
lysimeter
with
its
container
is approximately 8000
kg.
The
lysimeter has a mechanically adjustable counter-
balance, and changes in weight
are
measured
with a 250 pound
(1
13.6
kg)
capacity Sensotec
Model 41
tension/compression
load
cell.
The
load
cell
has a 4:1
mechanicaladvantage
on
the
lysimeter (i.e.,
a
change of
4
kg
in
the
mass
of
the
lysimeter will change the force
on
the
load cell by
1
kg-force
or
980
N).
The
surface
area of
the
lysimeter is 3.1416
m2
dr
31,416
cm2,
so
1
cm
of
rainfall or evaporation
results in a 31.416 kg
change
in
mass.
The
load
ceff
can measure
t113.6
kg,
a227
kg
range.
This
represents
a
maximum change
of 909
kg (28 cm
of
SECTION
7.
MEASUREMENT PROGRAMMING'EXAMPLES
ADJUSTABLE
COUNTER BALANCE
LOAD
CELL
FIGURE
7.13-1. Lysimeter Weighing Mechanism
water)
in
the
lysimeter before the counterbalance
would
have
to be
readjusted.
There is
1000
feet
of 22 AWG
cable
between
the
CR10 and
the
load
cell.
The
output
of
the
load cell
is
directly proportional to
the
excitation voltage.
When
Instruction
6
(4
wire
half bridge) is used,
the
assumption
is
that the voltage
drop
in
the
connecting
cable
is
negligible.
The average
resistance of 22 AWG
wire is
16.5 ohms
per
1000
feet.
Thus,
the
resistance in the
excitation
lead
going out to
the
load cell added to
that
in
the
lead
coming
back to
ground
is
33
ohms.
The
resistance
of
the
bridge
in
the
load
cell
is 350
ohms.
The
voltage
drop across
the
load
cell
is
equal to the
voltage
at
the CR10 multiplied by
the
ratio
of
the
load cell resistance, R", to the
total
resistance,
Rr,
of
the
circuit.
lf
Instruction
6
were
used
to
measure
the
load cell, the excitation
voltage
actually applied
to
the
load cell,
V1,
would
be:
V1
=
V*
RS/RT
=
Vx
350/(350+33)
=
0.91
Vx
Where V"
is
the excitation
voltage.
This
means
that the voltage
output
by
the
load cell would only
be 91% of that
expected.
lf
recording
of
the
lysimeter data
was
initiated with
the
load cell
output at
0
volts, and
100 mm of evapotranspira-
tion
had occurred, calculation of the change with
Instruction
6
would
indicate
that
only
91
mm of
water
had-been
lost.
Because
the error
is a
fixed
percentage
of
the
output,
the actual
magnitude
of
the
error
increases with the
force
applied to
the
load
cell.
lf
the
resistance
of
the wire was
constant, one could correct for the
voltage
drop
with
a
fixed
multiplier.
However,
the
resistance of
7-11