Reference-resistor error in ratiometric resistance measurement is the error left when an instrument converts a measured resistance ratio using an inaccurate value for its reference resistor. Shared excitation removes one nuisance input; it does not establish the denominator's true electrical resistance.
Let be the actual reference resistor value and the value used in calculation. For an ideal simultaneous reading , the inferred sensor resistance is
Writing gives the exact fractional error . The familiar is its first-order approximation. If a deterministic bound is , the inferred fractional error lies in
A symmetric reference tolerance therefore produces a slightly asymmetric resistance-error interval.
For an original example, suppose the instrument uses while the actual reference resistor is . A true sensor is reported as , an error near . Multiplying the shared excitation by any common positive number leaves this error unchanged in the ideal model. Using a measured and corrected instead of its nominal marking can remove the known part, while the corrected value retains its own measurement uncertainty.
Temperature variation can produce the remaining error after measurement calibration. Locally, , where is the temperature coefficient of resistance. For example, a -parts-per-million-per-kelvin coefficient over contributes roughly parts per million; it survives excitation cancellation. The primary circuit guide explicitly requires reference accuracy and low drift, and separates these requirements from shared-current cancellation.[ref]
For small random errors, applying the law of propagation of uncertainty to gives
The covariance term must follow how the reference value and reading were obtained; it cannot simply be assumed zero when inputs are shared.[ref]

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