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CR1000 Manual - Campbell Scientific

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Section 8. Operation<br />

Table 63. StrainCalc() Instruction Equations<br />

StrainCalc()<br />

BrConfig Code<br />

6<br />

Configuration<br />

Full-bridge strain gage. Half the bridge has two gages parallel to + and<br />

- , and the other half to - and + :<br />

where:<br />

• : Poisson's Ratio (0 if not applicable)<br />

• GF: Gage Factor<br />

• V r : 0.001 (Source-Zero) if BRConfig code is positive (+)<br />

• V r : -0.001 (Source-Zero) if BRConfig code is negative (-)<br />

and where:<br />

• "source": the result of the full-Wheatstone-bridge measurement (X = 1000 *<br />

V 1 / V x ) when multiplier = 1 and offset = 0.<br />

• "zero": gage offset to establish an arbitrary zero (see FieldCalStrain() in<br />

FieldCal() Demonstration Programs (p. 153) ).<br />

StrainCalc Example: See FieldCalStrain() Demonstration Program (p. 162)<br />

8.1.4 Thermocouple<br />

Note Thermocouples are easy to use with the <strong>CR1000</strong>. They are also<br />

inexpensive. However, they pose several challenges to the acquisition of accurate<br />

temperature data, particularly when using external reference junctions. <strong>Campbell</strong><br />

<strong>Scientific</strong> strongly encourages any user of thermocouples to carefully evaluate<br />

Error Analysis (p. 302). An introduction to thermocouple measurements is located in<br />

Hands-on Exercise: Measuring a Thermocouple (p. 42).<br />

The micro-volt resolution and low-noise voltage measurement capability of the<br />

<strong>CR1000</strong> is well suited for measuring thermocouples. A thermocouple consists of<br />

two wires, each of a different metal or alloy, joined at one end to form the<br />

measurement junction. At the opposite end, each lead connects to terminals of a<br />

voltage measurement device, such as the <strong>CR1000</strong>. These connections form the<br />

reference junction. If the two junctions (measurement and reference) are at<br />

different temperatures, a voltage proportional to the difference is induced in the<br />

wires. This phenomenon is known as the Seebeck effect. Measurement of the<br />

voltage between the positive and negative terminals of the voltage-measurement<br />

device provides a direct measure of the temperature difference between the<br />

measurement and reference junctions. A third metal (e.g., solder or <strong>CR1000</strong><br />

terminals) between the two dissimilar-metal wires form parasitic-thermocouple<br />

junctions, the effects of which cancel if the two wires are at the same temperature.<br />

Consequently, the two wires at the reference junction are placed in close<br />

proximity so they remain at the same temperature. Knowledge of the referencejunction<br />

temperature provides the determination of a reference-junction<br />

compensation voltage, corresponding to the temperature difference between the<br />

301

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