Experimental Circuit Validation & Measurement Uncertainty

A circuit experiment validates a model only when measurement loading, instrument uncertainty, component tolerance, and residual definitions are explicit. Agreement is a quantitative comparison, not two rounded numbers that look close.

The purpose of a circuit lab is not to "prove Kirchhoff's laws" by producing a small remainder. It is to test whether a particular lumped model, with measured component values and instrument models, predicts observations within stated uncertainty. Conservation-law residuals are powerful diagnostics, but only after sign conventions and measurement loading are correct.

Build the prediction from measured inputs #

Measure the quantities the model actually uses: resistor values rather than color-code nominals, source open-circuit voltage and output resistance rather than the front-panel setting, and meter burden where it is not negligible. Record units, ranges, and reference directions before energizing the circuit.

For a predicted quantity ymy_m and observation yoy_o, useful residuals include

r=yo−ym,rrel=yo−ymmax⁡(∣ym∣,yfloor).r=y_o-y_m,\qquad r_{rel}=\frac{y_o-y_m}{\max(|y_m|,y_{floor})}.

The floor prevents meaningless relative errors near zero. Compare rr with a combined uncertainty, not with an arbitrary percentage.

Conservation residuals #

At a measured node, define

rI=∑kskIk,r_I=\sum_k s_k I_k,

where sks_k follows the declared arrows. Around a loop,

rV=∑kskVk.r_V=\sum_k s_k V_k.

For a whole network under the passive sign convention,

rP=∑kVkIk.r_P=\sum_k V_kI_k.

Each residual should be near zero relative to its propagated uncertainty. A shared calibration error can move several readings together, so uncertainties are not always independent.

Failure classification #

Symptom First suspect
one KCL residual is large reversed current sign or missing branch
every voltage is scaled source setting or meter range
measured voltage collapses only when probed voltmeter loading
power residual is large but KCL/KVL close polarity convention or source power sign
disagreement changes with temperature component self-heating or source regulation

A valid conclusion names the model, operating point, residuals, uncertainty budget, and any systematic deviation. "Theory confirmed" without those items is not a reproducible result.

A compact uncertainty budget #

Suppose a calculated divider output is Vo=VsR2/(R1+R2)V_o=V_sR_2/(R_1+R_2). Treat VsV_s, R1R_1, and R2R_2 as input quantities with standard uncertainties and propagate them through the same measurement model. For uncorrelated inputs,

uc2(Vo)=∑i(∂Vo∂xiu(xi))2.u_c^2(V_o)=\sum_i\left(\frac{\partial V_o}{\partial x_i}u(x_i)\right)^2.

NIST TN 1297 separates statistically evaluated Type A components from Type B components evaluated by other information, then combines standard uncertainties. It also makes the reporting rule explicit: a result without a quantitative uncertainty statement is incomplete.

Sources

  1. docsGuidelines for Evaluating and Expressing the Uncertainty of NIST Measurement Resultspdf
  2. docsABCs of Probes Primer

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