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Section 8. Operation
460
Vibrating Wire Temperature Measurement
Temperature data from the two-wire thermistor that is often embedded in
vibrating wire sensors is used to correct measurement errors caused by thermal
expansion and contraction of the sensor body. Resistance thermistor changes with
sensor temperature. Leads connect to the
U
terminal pair numerically following
the
U
terminal pair to which the vibrating wire coil leads are connected.
Measurement of the thermistor is enabled in the
VibratingWire()
instruction with
an argument other than zero in the
ThermFnotch
parameter . The measurement is
made as follows: excite
U1
, and while exciting, measure differentially
U1 U2
, and
then measure differentially across an internal 5.99K ohm resistor. This is the same
sequence as that used in
four-wire half-bridge
measurements, but the wiring has
no provision for long-lead compensation.
Thermistor temperature can be calculated automatically by inputing arguments
other than
0
in the
A
,
B
,
C
parameters in the
VibratingWire()
instruction. The
values to input are the Steinhart-Hart coefficients supplied by the sensor
manufacturer.
A few vibrating wire sensors use a resistive element other than a thermistor to
measure temperature. Inputing
0
as the argument for
A
,
B
, and
C
results in the
output of resistance expressed as ohms.
Converting Thermistor Resistance to Temperature
The Steinhart-Hart equation is expressed as follows:
T = 1 / (A + B • LN(R) + C • (LN(R))^3)
– 273.15
Where
T
is the temperature of the thermistor,
A
,
B
, and
C
are coefficients, and
R
is
the resistance of the thermistor.
Note
Coefficients for Steinhart-Hart are specific to the thermistor in the
sensor. Obtain coefficients from the sensor manufacturer.
For example, if the coefficients for Steinhart-Hart are provided from the
manufacturer as follows,
A
= 1.4051E
–03
B
= 2.369E
–04
C
= 1.019E
–07
the equation for converting the resistance measurement to degrees Celsius is:
T = 1 / (1.4051E
–03 + 2.369E–
04 • LN(R) + 1.019E
–
7 • (LN(R))^3)
–
273.15
Where R is the measured resistance. If the measured resistance is 2221 Ω, the
equation is,
T = 1/(1.4051E
–03 + 2.369E–
04 • LN(2221) + 1.019E
–
7 • (LN(2221))^3)
–
273.15
Summary of Contents for CR6 Series
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Page 76: ...Section 5 Overview 76 FIGURE 20 Half Bridge Wiring Example Wind Vane Potentiometer ...
Page 80: ...Section 5 Overview 80 FIGURE 23 Pulse Input Wiring Example Anemometer ...
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Page 454: ...Section 8 Operation 454 FIGURE 104 Narrow Sweep High Noise ...
Page 459: ...Section 8 Operation 459 FIGURE 106 Vibrating Wire Sensor Calibration Report ...
Page 535: ...Section 8 Operation 535 8 11 2 Data Display FIGURE 121 CR1000KD Displaying Data ...
Page 537: ...Section 8 Operation 537 FIGURE 123 CR1000KD Real Time Custom ...
Page 538: ...Section 8 Operation 538 8 11 2 3 Final Storage Data FIGURE 124 CR1000KD Final Storage Data ...
Page 539: ...Section 8 Operation 539 8 11 3 Run Stop Program FIGURE 125 CR1000KD Run Stop Program ...
Page 541: ...Section 8 Operation 541 FIGURE 127 CR1000KD File Edit ...
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Page 610: ...Section 11 Glossary 610 FIGURE 137 Relationships of Accuracy Precision and Resolution ...
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