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CR1000 Manual - Campbell Scientific

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Section 8. Operation<br />

• Effects due to the following are not included in the specification:<br />

o<br />

o<br />

o<br />

Bridge-resistor errors<br />

Sensor noise<br />

Measurement noise<br />

The ratiometric-accuracy specification is applied to a three-wire half-bridge<br />

measurement that uses the BrHalf() instruction as follows:<br />

The relationship defining the BrHalf() instruction is X = V1/Vx, where V1<br />

is the voltage measurement and Vx is the excitation voltage. The<br />

estimated accuracy of X is designated as ∆X, where ∆X = ∆V1/Vx. ∆V1 is<br />

derived using the following method.<br />

The ratiometric-accuracy specification is applied to a four-wire full-bridge<br />

measurement that uses the BrFull() instruction as follows:<br />

The relationship defining the BrFull() instruction is X = 1000*V1/Vx,<br />

where V1 is the voltage measurement and Vx is the excitation voltage.<br />

Result X is expressed as mV/V. Estimated accuracy of X is ∆X, where ∆X<br />

= 1000*∆V1/Vx. ∆V1 is derived using the following method.<br />

∆V1 is derived using the ratiometric‐accuracy equation. The derivation<br />

is illustrated in this example, which is supported by the assumption that<br />

the measurement is differential with input reversal, datalogger<br />

temperature is between ‐25° to 50°C, analog‐input range is ±250 mV, V1<br />

= 110 mV, and excitation is reversed during the excitation phase of the<br />

measurement. The effect each assumption has on the magnitude of<br />

∆V1 in this example is noted in the following figure.<br />

Figure 91: Deriving ∆V1<br />

299

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