05 · Foundational → rigorous

Accuracy, uncertainty & reproducible DC workflow

A credible measurement result is more than the displayed digits. Distinguish accuracy, precision, resolution, error and uncertainty; evaluate Type A and Type B components; combine standard uncertainties through a measurement model; interpret coverage factors carefully; separate calibration from adjustment and traceability; and build a reproducible evidence record.

150–190 minFoundational → rigorous
In this lesson
  • Use VIM terminology to distinguish measurement accuracy, precision, error, resolution and measurement uncertainty without treating them as synonyms.
  • Explain why accuracy is a qualitative concept rather than a numerical quantity value, while precision can be characterized by dispersion statistics.
  • Evaluate repeatability from repeated observations and calculate the standard uncertainty of the mean as a Type A contribution under the stated assumptions.
  • Interpret manufacturer accuracy specifications only under their stated range, temperature, time-since-calibration and other conditions, and convert a bounded contribution to standard uncertainty only after choosing and justifying a probability model.
  • Explain that Type A and Type B are methods of uncertainty evaluation, not synonyms for random and systematic error.
  • Propagate independent standard uncertainties through a measurement model with sensitivity coefficients and state when covariance terms cannot be neglected.
  • Distinguish standard, combined standard and expanded uncertainty and explain why k=2 is not a universal synonym for exactly 95% coverage.
  • Distinguish calibration, adjustment and metrological traceability using VIM definitions.
  • Include meter loading/correction in the measurement model when the measurand is the unloaded source quantity rather than the loaded terminal quantity.
  • Create a reproducible DC measurement record containing measurand definition, circuit state, instrument configuration, raw data, corrections, calibration context, uncertainty budget, result statement and evidence provenance.
Starting question

A meter displays 5.000 V. How many of those digits belong in the scientific result?

The display alone cannot answer. A measurement result needs a defined measurand, a model of the measurement, instrument conditions, corrections, calibration context, repeatability information and an uncertainty statement.

05.1Accuracy, precision, error, resolution and uncertainty are different concepts

ConceptUse it for
Measurement accuracyQualitative closeness of agreement between a measured value and a true quantity value. In VIM it is not itself a quantity and is not assigned a numerical quantity value.
Measurement precisionCloseness among repeated indications/values under specified conditions; dispersion statistics such as standard deviation can characterize it.
Measurement errorMeasured value minus a reference quantity value. The exact error is generally not fully known in ordinary measurement work.
ResolutionSmallest change in the measured quantity that causes a perceptible change in the indication, in the stated instrument context.
Measurement uncertaintyNon-negative parameter characterizing the dispersion of quantity values attributed to the measurand, based on the information used.

A display with many digits can have fine resolution and still have poor accuracy. Repeated readings can be very precise yet biased. Uncertainty is not a synonym for error; it expresses the remaining dispersion attributed to the measurand after the measurement model, corrections and information have been considered.

05.2Start from a measurand and a measurement model

A result is meaningless until the quantity intended to be measured is defined. “Measure the voltage” is incomplete if the circuit changes when the meter is connected.

For the unloaded Thévenin voltage from Chapter 02, one possible measurement model is

VTH=Vmeas(1+RTH/RIN)

The output quantity is the desired unloaded voltage. The input quantities are the loaded indication plus source and meter input resistances. This model makes a crucial point explicit: loading correction is not an afterthought; it is part of the definition of how the measurand is obtained.

If the intended measurand is instead the actual terminal voltage with the meter connected, no unloading correction belongs in the model. The model must match the question.

05.3Type A evaluation: learn from repeated observations

Suppose five repeated DC readings under repeatability conditions are:

4.998, 5.001, 4.999, 5.000, 5.002 V

Their arithmetic mean is

x̄=(1/n)Σxi=5.000 V

The sample standard deviation is approximately

s=1.581 mV

If the mean of these n independent observations is used as the estimate and the repeatability model is appropriate, the standard uncertainty of the mean is

uA(x̄)=s/√n=0.707 mV

This is a Type A evaluation because it is obtained by statistical analysis of repeated observations. It does not mean “all random effects belong to Type A” or “all systematic effects belong to Type B.” Type A and Type B classify methods of evaluating uncertainty components, not error mechanisms.

05.4Type B evaluation: specifications become uncertainty only through an explicit model

Consider a deliberately hypothetical meter specification used only to teach the calculation:

±(0.05% of reading + 2 digits)

Assume the reading is 5.000 V and the displayed least significant digit is 1 mV. The specification bound is

a=0.0005·5.000 V+2·0.001 V=4.5 mV

A bound is not automatically a standard uncertainty. If, and only if, a rectangular distribution within ±a is justified by the available information, then

uB=a/√3=2.598 mV

Another distribution would give another standard uncertainty. The probability model must be justified from the specification, calibration information or engineering knowledge.

05.5Combine standard uncertainties through sensitivity coefficients

For a measurement model y=f(x1,…,xN), the first-order law of propagation uses sensitivity coefficients

ci=∂f/∂xi

For uncorrelated input quantities,

uc2(y)=Σ[ciu(xi)]2

If relevant input quantities are correlated, covariance terms must be included rather than silently set to zero:

uc2(y)=Σci2u2(xi)+2Σi<jcicju(xi,xj)

For the simple teaching example where the Type A mean uncertainty 0.707 mV and the hypothetical Type B specification uncertainty 2.598 mV are treated as independent contributions to the same voltage estimate,

uc=√[(0.707 mV)2+(2.598 mV)2]=2.693 mV

The larger component dominates. Collecting many repeated readings cannot compensate for a much larger specification/calibration contribution.

05.6Expanded uncertainty and coverage factor: do not turn k=2 into a slogan

An expanded uncertainty is commonly written

U=k uc

For the teaching example, choosing k=2 gives

U=2·2.693 mV=5.386 mV

But k=2 is not a universal mathematical synonym for exactly 95% coverage. Coverage depends on the probability distribution represented by the result, effective degrees of freedom and the method used. If a coverage probability is claimed, the basis must be stated.

A defensible teaching-style report could therefore be: V = 5.0000 V ± 0.0054 V, U, k=2, followed by the conditions and budget used. The number of reported digits should be consistent with the uncertainty rather than copied mechanically from the display.

05.7Calibration, adjustment and metrological traceability are not the same thing

Calibration establishes, under specified conditions, a relation between reference quantity values with uncertainties and indications with associated uncertainties, then uses that information to obtain a measurement result from an indication. Calibration does not necessarily change the instrument.

Adjustment is a set of operations performed on a measuring system so that it provides prescribed indications corresponding to given values. Adjustment can change the instrument and may require recalibration afterward.

Metrological traceability is a property of a measurement result whereby it can be related to a reference through a documented unbroken chain of calibrations, each contributing to measurement uncertainty.

Therefore “the meter is calibrated” is not enough for a reproducible record. We also need the calibration status/date or interval context, the applicable certificate or specification information, and whether the conditions of use fall within that information.

05.8A reproducible DC measurement record is an engineering artifact

AoN treats measurement evidence as first-class technical data. A minimum reproducible record should capture:

  1. Measurand: what quantity is intended, between which nodes, under what circuit state and environmental conditions.
  2. Circuit state: source settings, loads, relevant topology, power state and any loading/correction model.
  3. Instrument identity: manufacturer/model, asset or serial identifier when appropriate, and calibration status/context.
  4. Configuration: function, range, terminals, integration/filter settings if relevant, probe/lead arrangement and polarity/reference convention.
  5. Raw observations: individual readings, not only their final average.
  6. Corrections: loading, offsets, lead compensation or other corrections, with sign and source of correction.
  7. Uncertainty budget: each input quantity, estimate, standard uncertainty, distribution/evaluation method, sensitivity coefficient and contribution.
  8. Result statement: estimate, uncertainty type, coverage factor/probability when used, units and significant digits.
  9. Provenance: date/time, operator or automated workflow, raw-data file, script/version and links to calibration or instrument documentation when needed.

This transforms “I saw 5.000 V” into evidence another engineer can inspect, recompute and reproduce.

05.9Mastery exercises and course synthesis

  1. Five readings are 4.998, 5.001, 4.999, 5.000 and 5.002 V. Compute mean, sample standard deviation and standard uncertainty of the mean.
  2. A hypothetical specification is ±(0.05% of reading + 2 digits), reading 5.000 V, least significant digit 1 mV. Find the bound and, assuming a justified rectangular distribution, the standard uncertainty.
  3. Combine the Type A and Type B standard uncertainties from exercises 1 and 2 as independent contributions.
  4. Using k=2, calculate expanded uncertainty. Why may you not write “exactly 95%” without further justification?
  5. Explain in one sentence each the difference among accuracy, precision and uncertainty.
  6. A technician adjusts a meter until its indication changes, then says “calibration is complete.” What conceptual step is missing?
  7. For VTH=Vmeas(1+RTH/RIN), list the three input quantities whose uncertainty can contribute to the corrected unloaded voltage.
  8. Design the minimum record you would require before accepting a 5 V DC measurement into AoN's Real Measurement Library.
Solutions

1. Mean 5.000 V; sample standard deviation ≈1.581 mV; standard uncertainty of the mean ≈0.707 mV.

2. Bound a=4.5 mV; under the stated rectangular model, uB=a/√3≈2.598 mV.

3. uc=√(0.707²+2.598²) mV≈2.693 mV.

4. U≈5.386 mV. Coverage probability depends on the represented distribution, degrees of freedom and method; k=2 alone does not prove exact 95% coverage.

5. Accuracy describes closeness to a true value; precision describes agreement among repeated results; uncertainty quantifies the dispersion of values attributed to the measurand from the information used.

6. Adjustment changes the system; calibration must establish the indication/reference relation and associated uncertainty under specified conditions, and recalibration may be needed after adjustment.

7. Vmeas, RTH and RIN, plus any additional quantities required by the actual instrument/source model.

8. At minimum: measurand and nodes, circuit state, instrument identity/calibration context, mode/range/terminals, raw readings, corrections/model, uncertainty budget, final result statement and provenance/raw-file/script links.