Materials Science · Measuring and checking material claims
Calibration, uncertainty and repeatability
Apply a calibration correction to an actual set of invented readings, distinguish a shared offset from repeat scatter, and interpret a defined uncertainty budget without treating repetition as a cure for every measurement problem.
Useful background: Units, loads, stress and strain; Processing, structure and useful properties; Energy, stability and environmental context. Each worked case explains the quantities it uses.
Back to the chapterAfter reading, you can
- Distinguish calibration, correction, adjustment and repeatability using a numerical case.
- Calculate a corrected mean and explain which uncertainty contributions repeated observations can reduce.
- Interpret standard and expanded uncertainty under stated assumptions, and identify when a calibration cannot simply be transferred.
A consistent instrument can still be biased
A balance can return nearly the same indication each time while being offset. Calibration relates indications to reference values under stated conditions, including uncertainty. A correction may then be applied; calibration is not automatically an adjustment.
Suppose a balance repeatedly indicates about 50.200 g when a reference item has an assigned mass of 50.000 g. The readings can form a tight cluster while their centre differs from the reference. Repeat scatter describes the cluster’s spread; the comparison with the reference reveals an estimated offset. These answer different questions.
An indication is the instrument’s displayed value. The measurand is the quantity being estimated: here, the mass of the specified item under the stated measurement conditions. The reference value also has uncertainty; it is not an infinitely precise glimpse of a true mass.
In this invented local model, the instrument reads high by 0.200 g. Define an additive correction C as reference value minus mean reference indication. Then C=−0.200 g. Adding this correction moves an indication downward. Reversing its sign would increase the estimated error.
Applying a correction in a calculation does not adjust the instrument. An adjustment changes its response. After adjustment the earlier calibration relationship may no longer describe it, so the relationship must be checked again. The physical object, instrument and reported corrected result should remain identifiable.
| Observation | Reference indication (g) | Coupon indication (g) |
|---|---|---|
| 1 | 50.180 | 50.880 |
| 2 | 50.200 | 50.900 |
| 3 | 50.220 | 50.920 |
| 4 | 50.190 | 50.890 |
| 5 | 50.210 | 50.910 |
Build the measurement picture
Repeatability examines variation under specified repeated conditions. Uncertainty also includes relevant reference, resolution, correction and model contributions. Repetition can reduce some contributions to a mean but cannot erase an unrecognised common offset. Report uncertainty with its meaning rather than an unexplained plus-or-minus sign.
For repeatability, keep the relevant procedure, operator, measuring system, operating conditions and location specified, and take repeats over a short period. Leaving one object untouched and copying an unchanged display five times does not test the variability of removing and replacing it.
A common correction shifts every reading by the same amount, so it does not change differences among them. Correcting the five reference indications gives 49.980, 50.000, 50.020, 49.990 and 50.010 g. Their mean now equals the assigned reference value, but their range is still 0.040 g. Agreement at that calibration point follows from how the correction was estimated; it is not an independent demonstration of perfect performance.
The coupon readings average 50.900 g. Applying the same correction gives an estimated mass 50.700 g. This uses a local constant-offset model. Its suitability depends on the range, load arrangement and conditions; the single reference point alone cannot establish the response everywhere.
The spread of readings and the uncertainty of a mean
For the five coupon readings, subtract their mean 50.900 g. The deviations are −0.020, 0, +0.020, −0.010 and +0.010 g. Their squared deviations sum to 0.001000 g². The sample standard deviation is s=√[0.001000/(5−1)]=0.01581 g. It describes repeat scatter in individual readings under these conditions.
If the observations are independent and their distribution is sufficiently stable for this statistical estimate, the standard uncertainty contribution for their mean is u_rep=s/√n. With n=5, this is 0.007071 g. Averaging can reduce this contribution because independent positive and negative fluctuations partially cancel.
The uncertainty of the shared calibration correction does not get divided by √n when the same correction is applied to every coupon reading. Any uncertainty about that common shift remains in the mean. Drift or correlated fluctuations can also invalidate the simple independent-repeat calculation.
Type A and Type B name evaluation methods, not two physical kinds of error: statistical analysis of observations versus other information. A correction’s uncertainty can itself contain statistically evaluated contributions. A spreadsheet column labelled systematic does not, by itself, establish how a contribution should be combined.
State the measurement model before combining contributions
Use the deliberately limited additive model m=mean(I)+C +Δ_env. Here mean(I) is the mean coupon indication, C is the calibration correction, and Δ_env corrects for a specified environmental difference from calibration conditions. In this example Δ_env is estimated as zero; uncertainty about it remains.
The following invented budget supplies standard uncertainties: uncertainty values expressed on an estimated-standard-deviation scale. The supplied u_C already includes the relevant reference and calibration-evaluation contributions. They must not be added a second time as separate rows. All listed contributions are stipulated uncorrelated, and each enters this additive model with coefficient +1.
Under these assumptions, add variances rather than adding the standard uncertainties directly: u_c²=u_rep²+u_C²+u_env². Thus u_c=√(0.007071²+0.010²+0.003²)g=0.01261 g. The subscript c denotes combined standard uncertainty. This is a result for the specified model and budget, not a universal rule for every material test.
If inputs share information, covariance can matter. A force/area property also has a different measurement function and sensitivities. Reused reference data, geometry, temperature correction, sampling and model inadequacy need their own assessment. Do not add an unexplained resolution term when the same effect has already been counted elsewhere.
| Contribution | Standard uncertainty (g) | How used here |
|---|---|---|
| Independent repeat contribution of mean | 0.007071 | Estimated from the five coupon observations |
| Shared correction C | 0.010 | Supplied calibration uncertainty; not divided by √5 |
| Environmental transfer Δ_env | 0.003 | Supplied separate uncertainty for the stated conditions difference |
Say what the uncertainty statement means
An expanded uncertainty U is a chosen coverage factor k times u_c. For the illustrative choice k=2, U=0.02522 g, which can be rounded to 0.025 g. Report, for example: corrected coupon mass m=50.700 g, expanded uncertainty U=0.025 g, k=2, using the stated additive model and budget. Keep the calibration and observation conditions with that result.
This numerical statement defines the expanded-uncertainty interval approximately 50.675 g to 50.725 g after rounding. It is not a guaranteed bound on all possible mistakes. Nor does choosing k=2 by itself establish 95% coverage. Such an interpretation needs a justified distribution and adequate knowledge of the uncertainty estimates. Five repeats alone do not establish those conditions.
A smaller uncertainty requires better information about the important contributions. More independent coupon repeats can reduce u_rep; a better calibration or better control of the environmental transfer addresses different terms. Correcting a known offset and estimating uncertainty are complementary tasks.
A calibration at one load, temperature or contact arrangement is not automatically valid for another. A later reference at 100.000 g that indicates 100.400 g suggests a different offset from the 50 g comparison; the constant-offset model needs investigation across that range. For a material test, instrument calibration also does not establish specimen representativeness, correct gripping, or that the chosen test measures the intended property.
Worked examples
Averaging retains the common shift
Five readings agree closely but a reference check reveals a common offset. Does averaging remove it?
- The five reference indications sum to 251.000 g, so their mean is 50.200 g. Compared with the assigned 50.000 g reference, the estimated indication offset is +0.200 g.
- A mean of any number of observations affected by that same fixed offset retains it. The correction for this local additive model is C=50.000−50.200=−0.200 g.
- Adding C shifts every reference reading equally. The range remains 50.220−50.180=0.040 g; the shift in the centre is separate from the repeat scatter.
- The correction has uncertainty because its reference and determination have uncertainty. Its value is not the uncertainty, and using it at the calibration point is not an independent verification.
No. Agreement among repeats does not establish freedom from systematic effects.
From indications to a corrected estimate
Use the coupon column and the local correction. What mass estimate follows, and which assumption permits the transfer?
- The five indications sum to 254.500 g, giving mean(I)=50.900 g.
- Use m=mean(I)+C +Δ_env. With C=−0.200 g and the stipulated environmental correction Δ_env=0, m=50.700 g.
- The calculation assumes that the calibrated local response applies at the coupon load and its specified placement/conditions. A single reference comparison does not validate every load or specimen.
- Changing every indication by the same correction leaves the sample standard deviation 0.01581 g unchanged. The independent-repeat contribution to the mean is 0.01581/√5=0.007071 g.
The corrected estimate is 50.700 g under the stated local model. Its uncertainty needs the full budget, not just the scatter of these readings.
Choose which information to improve
Assume twenty independent coupon observations have the same single-reading s=0.01581 g, while the supplied correction and environmental uncertainties remain unchanged. How does u_c change?
- Only the repeat contribution changes: u_rep=0.01581/√20=0.003536 g, half its five-reading value. This assumption concerns a genuinely independent, stable series.
- The common correction contribution remains 0.010 g and the environmental contribution remains 0.003 g. Neither was independently redetermined twenty times.
- Combine the stipulated uncorrelated contributions: u_c=√(0.003536²+0.010²+0.003²)=0.01102 g, compared with 0.01261 g for five observations.
- Even if the repeat contribution could become negligible, the unchanged terms give √(0.010²+0.003²)=0.01044 g. This lower limit belongs to this supplied budget, not every measurement system.
Four times as many independent repeats halve the repeat contribution, but u_c falls only to about 0.01102 g. Improving the dominant shared information can matter more.
Try the reasoning
Is calibration the same as adjusting an instrument? A technician subtracts 0.200 g in a worksheet while the balance still displays the old indications. What changed?
Show the answer and reasoning
No. The worksheet applies a correction; the instrument response has not been adjusted.
Calibration establishes the relationship used for interpreting indications. Applying that relationship changes the reported estimate. Adjustment changes the measuring system and can require a new calibration relationship.
What does a bare ±0.025 g leave unclear? Does writing k=2 automatically settle every missing detail?
Show the answer and reasoning
It leaves the kind of uncertainty, underlying model/conditions and any justified coverage interpretation unclear. k=2 identifies a multiplier but does not by itself establish 95% coverage.
Specify the measured quantity and corrected value, whether the uncertainty is standard or expanded, its budget/model and the coverage factor when used. A probability statement requires its own basis.
A different reference has assigned mass 20.000 g and gives indications 20.080, 20.100 and 20.120 g. In a valid local constant-offset model, find C and correct a coupon mean indication 21.340 g.
Show the answer and reasoning
The reference mean is 20.100 g, so C=−0.100 g. The corrected coupon estimate is 21.240 g.
Subtract the mean reference indication from the assigned reference value, then add the correction to the coupon indication. Adding +0.100 g would move a high indication farther in the wrong direction. Reference/correction uncertainty still remains.
The 50.000 g reference has mean indication 50.200 g. A 100.000 g reference has mean indication 100.400 g. Can one simply subtract 0.200 g throughout this larger range?
Show the answer and reasoning
These two central observations do not support one constant offset across the range; the observed offsets are 0.200 g and 0.400 g.
Investigate an appropriate calibration relationship and associated uncertainty across the intended range. The pattern might motivate a scale-factor model, but two values alone do not establish its validity, time stability or behaviour elsewhere.
A colleague uses the calibrated balance to compare two material coupons, then declares their tensile strengths equal because their corrected masses agree within uncertainty. What additional issue remains?
Show the answer and reasoning
Mass agreement does not establish tensile-strength agreement, and the mass measurement’s uncertainty does not cover every other material property.
Identify the intended property and its test, specimen geometry, preparation and conditions. Calibration supports a specified measurement relationship; it does not turn one measured quantity into evidence for every service claim.
What to carry forward
- A shared offset can remain in a highly repeatable set of readings. Estimate a justified correction with its own uncertainty.
- Averaging reduces a repeat contribution only under suitable statistical conditions; it does not erase a shared calibration uncertainty.
- Define the measurement model before combining standard uncertainties, and avoid double counting or ignoring covariance.
- Report the kind of uncertainty, coverage factor when used and conditions; transfer beyond the calibration range requires evidence.
References
Teaching resources and research supporting this lesson’s explanations and examples.
- International Vocabulary of Metrology (VIM3)Joint Committee for Guides in Metrology (JCGM)ReferenceInternational Vocabulary of Metrology · 2.39 CalibrationInternational Vocabulary of Metrology · 2.26 Measurement uncertaintyInternational Vocabulary of Metrology · 2.20 Repeatability condition of measurement
- Guidelines for Evaluating and Expressing the Uncertainty of NIST Measurement ResultsBarry N. Taylor and Chris E. Kuyatt · National Institute of Standards and TechnologyNIST Technical Note 1297, 1994 edition · selected explanatory sectionsGuidelines for Evaluating and Expressing the Uncertainty of NIST Measurement ResultsEvaluation methodsType A evaluationCombined standard uncertaintyExpanded uncertaintyReporting uncertainty