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TABLE OF CONTENTS
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VIBRATING WIRE PI EZOMETERS AND PRESSURE TRANSDUCERS
1. GENERAL INFORMATION
The CR10 is the only CSI datalogger that has
the capability of measuring the vibrating wire
pressure sensor in addition to the piezoresistive
type of strain gage sensor. The CR10 can
measure vibrating wire sensors with short leads
without the AVW1 or AVW4. However, the
AVW1 and AVW4 provide important signal
conditioning that 1) completes the thermistor
bridge for the measurement of the sensor's
temperature, 2) converts the swept frequency
excitation from 2.5 volts peak to peak to 12
volts peak to peak, 3) provides transformer
isolation and consequent noise reduction for the
vibrating wire signal, and 4) provides additional
transient protection for both the temperature
and vibrating wire circuits.
The AVW1 and AVW4 are designed and tested
over the environmental range from -25°C to
+50°C. CSI recommends that special
temperature testing be done at the factory if the
AVW's are to operate at temperatures outside
this range.
1.1 SENSOR SELECTION
The vibrating wire sensors may be purchased
as either vented or sealed sensors. The vented
sensors have a small hollow "vent tube" that
connects the hollow chamber behind the
diaphragm to the atmosphere. The vent tube
allows the barometric pressure to act on both
sides of the diaphragm equally which removes
the barometric pressure from the reading. A
pressure reading with out a barometric pressure
component is referred to as "gage" pressure. A
pressure reading with a barometric pressure
component is referred to as "absolute"
pressure. One disadvantage of the vented
sensor is that the cable, which contains the vent
tube, is more expensive than the cable for the
unvented sensor. For this reason, it may be
more economical to buy unvented sensors and
use an extra one as a barometer to remove the
barometric pressure. A second small
disadvantage of the vented sensors is that they
require the use of desiccant, which must be
changed periodically, to dry the air entering the
vent tube.
The vibrating wire pressure sensor has a good
reputation for long term stability. The sensor
utilizes a change in the frequency of a vibrating
wire to sense pressure. Two measurements
are usually made on a vibrating wire sensor.
The first is the measurement of the temperature
of the probe to compensate for changes in its
temperature. The second is the measurement
of the frequency of the vibrating wire.
This manual covers the use of the CR10 and
AVW1 or AVW4 with Geokon's Model 4500
vibrating wire sensor series. Sections 2 and 3
of this manual cover the temperature and
vibrating wire measurements respectively.
Sections 4 and 5 give detail concerning the use
of the AVW1 and AVW4.
Geokon includes a calibration sheet and
instruction manual with each sensor or group of
sensors they sell. Geokon's manual should be
consulted for information on sensor selection
and installation. Geokon's address and phone
number are: 48 Spencer Street, Lebanon, NH
03766, (603) 448-1562.
1.2 SENSOR CARE AND INSTALLATION
The moisture trap of the vented models should
be kept closed until readings are to be taken.
DO NOT FORGET to remove the screw that
plugs the moisture trap when readings are to be
taken.
The large diameter diaphragm used in the low
pressure sensor requires special care when
handling. Avoid bumping or jarring the sensor.
Orientation of the 4500 series sensors will affect
the zero reading. Readings should be taken
with the sensor in the same orientation at all
times. When installing the 4500 series sensors,
certain steps should be followed to obtain
proper zero readings.
The cavity between the sintered filter cap and
the diaphragm should be filled with clean water
without any air bubbles.
In most cases the sensor is made to output
water height or pressure relative to a measured
level. In this case the pressure sensor should
1-1
AVW1/AVW4
be placed at the desired level and allowed to
come to temperature equilibrium with its
surroundings (5 minutes or more). The
multiplier determined in equation 3.2-2 should
be entered and 0.0 should be entered for the
offset. After the temperature and the reading
has stabilized, determine the value that would
have to be added to the reading to obtain the
measured level. Enter this value as the offset.
In some cases there is no measured reference.
In order to obtain the correct offset under these
conditions, lower the sensor to a point just
above the water level and wait 5 minutes. Use
the multiplier, an offset of 0.0, and the
temperature correction function determined in
Sections 3.2 and 3.5 to obtain a reading.
Record the reading. Solve equation 3.2-3 for
the new offset by plugging in the "reading" in the
place of the "[Gage Factor * Zero Reading]" and
the "Barometric Pressure" from an accurate
barometer or a reference sensor in the place of
"Po" unless it is a vented sensor then use 0 in
the place of "Po". Enter the new offset.
1-2
SECTION 2. TEMPERATURE MEASUREMENT
2.1 GENERAL
The vibrating wire probe includes a thermistor
which is used to measure the temperature of
the probe. Probe temperature is used to correct
errors in the vibrating wire measurement
caused by changes in the temperature of the
probe. The temperature correction is most
important when the temperature of the medium
the probe is measuring is changing (e.g. water
temperature in a river or shallow lake). When
concerned with the absolute reading, it is also
important to make the temperature correction if
the medium temperature differs from the
calibration temperature. In a deep well where
the water temperature does not change, the
error due to temperature can be removed by
allowing the sensor to come to thermal
equilibrium and adjusting the sensor reading to
read the correct depth by means of an offset.
2.2 ACCURACY AND RESOLUTION
The accuracy of the temperature measurement
is a function of the following factors listed in
decreasing importance: 1) the thermistor's
interchangeability, 2) the resistance of the wire,
3) the linearization error, 4) the precision of the
bridge resistors, 5) the accuracy of the
datalogger's voltage measurement, and 6) the
temperature coefficient of the bridge resistors.
The interchangeability of the thermistor is
o
C although a thermistor with ±0.2oC
±0.5
interchangeability is an option. The error due to
wire resistance is normally less than ±0.5
(see Figure 2.2-1 through 2.2-4). The
linearization error is ±0.15
over the range from -5 to +60
ο
C (see Figure 2.2-5)
o
C. The precision
of the bridge resistors (±0.1%) results in a
o
tolerance of ±0.03
C. The accuracy of the
datalogger's voltage measurement (±0.015%)
o
results in a tolerance of ±0.01
C. The
temperature coefficient of the bridge resistors
o
(10 ppm/
±0.0003
C) results in a tolerance of
oC/o
C.
Errors four, five, and six mentioned above are
o
all less than ±0.03
C each and can probably be
ignored. The wire resistance is primarily an
offset error and its affect on the pressure
measurement is removed by the initial
calibration. Errors caused by the change in wire
resistance due to temperature, thermistor
interchangeability, and the linearization error are
not removed by the initial calibration.
Ignoring the offset errors, the remaining
temperature accuracy is expected to be about
o
C. The temperature correction for the
±0.7
vibrating wire measurement is typically less than
o
0.05 psi/
C. A ±0.7oC temperature error would
result in a 0.035 psi (±1.0 inch H2O) error on a
50 psi Full Scale range.
The thermistor, Dale Electronics part number
1C3001-B3 is the standard with an
o
interchangeability of ±0.5
C. The optional
thermistor, Dale Electronics part number
1C3001-C3 has an inter-changeability of
o
C. Both of the above thermistors have the
±0.2
same resistance vs. temperature relationship as
o
C
the YSI thermistor number 44005.
The following table shows the relationship
between temperature and resistance, volts,
CR10 output, and linearization error.
o
TABLE 2.2-1. Temperature vs. Thermistor Resistance, V,