Campbell 21X Manual do Operador Página 72

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SECTION
7.
MEASUREMENT
PROGRAMMING
EXAMPLES
7.13
L
.6
WIRE
FULL
BRIDGE
When a
long
is required between
a load
cell and the
X, the
resistance
of the
wire
can
create a
ial error in the
measurement
if
bridge
(lnstruction
6)
is used to
the
load cell.
This
error
arises
the
excitation
voltage
is lower at
the
load cell
at
the
21X
due
to
voltage
droP
in
the cable.
The 6
wire full bridge
(lnstruction
9) avoids thi$
problem
by
measuring
the
excitation
voltage
at
the
load
cell.
This example
shows the
errors
one
would encounter
if
the
actual excitafion
voltage was not
measured and
shows the
uge
of a
6 wire full bridge
to
measure
a
load
cell
orlr a
weighing
lysimeter
(a
container
buried
in thelground,
filled with
plants
and
soil,
used
for me{suring
evapotranspiration).
The
lysimeter
is 2 meters in diameter
and 1.5
meters deepl
The
total weight
of the
lysimeter
with
its
cont4iner
is approximately
8000 kg.
The
lysimeter ha$
a mechanically
adjustable
counterbalarfce,
and changes
in
weight
are
measured
wlth a
250
pound
(1
13.6
kg) capacity
Sensotec
M0del
41 tension/compression
load
cell. The
lo{d cell
has a
4:1 mechanical
advantage
ofr
the
lysimeter
(i.e.,
a change
of
4
kg
in
the
maps
of the
lysimeter
will change the
force on the
jload
cell by 1 kg-force
or 980 N).
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 21X
multiplied by the
ratio of the
load
cell resistance,
R",
to
the total
resistance, R1,
of the
circuit.
lf
Instruction 6
were
used
to
measure the
load
cell,
the
excitation
voltage
actually
applied to
the load cell,
V.t
would
be:
V1
=
V, Rs/R1=
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 100mm
of
evapotranspiration
had occurred,
calculation
of
the
change
with
Instruction 6
would indicate
that
only
91mm
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
copper changes
O.4o/o
per
degree
C change
in temperature.
Assume
that
the
cable
between
the
load cell
and
the
21X
lays
on
the
soil
surface and undergoes
a 25oC
diurnal
temperature
fluctuation.
lf the resistance
is
33 ohms
at
the maximum
temperature,
then
at
the minimum
temperature,
the
resistance is:
(1-25x0.004)33
ohms
=
29.7 ohms
The actual
excitation
voltage
at the load
cell
is:
Vr
=
350/(350+29.7)
Vx
=
.92 Vx
The excitation
voltage has
increasedby
1"/",
relative to the
voltage applied
at the 21X.
ln this
case,
where
we
were
recording
a
91mm change
in water content,
there
would
be a 1mm diurnal
change
in the
recorded
water
content that
would
actually
be due
to
the
change
in temperature.
Instruction
9 solves this
problem
by
actually
measuring
the
voltage
drop
across the
load cell
bridge.
The drawbacks
to using
Instruction
9
the
4
wire
excite and
ADJUSTABLE
COUNTER
BALANCE
FIGURF
7.13-1. Lysimeter
Weighing
Mechanism
The surface
area
of
the lysimeter
is 3.1416
m2
or
31
,416
cin2,
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
wgter)
in the
lysimeter
before the
counterbalahce
would have to
be
readjusted.
There is 1000
feet of 22
AWG
cable
between
the 21X and
the
load cell.
The
output
of
the
load
cell
is
{irectly
proportionalto
the
excitation
7-9
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