Coverage Factors and Expanded-Uncertainty Reporting

Key Takeaways

  • Expanded uncertainty equals a selected coverage factor times combined standard uncertainty.

  • Small effective degrees of freedom can require a Student t factor larger than two for approximately 95% coverage.

  • Report uncertainty and result consistently, retaining sufficient internal precision before final rounding.

Last updated: October 2026

Determining the Coverage Factor kk and Expanded Uncertainty UU

Combined standard uncertainty uc(y)u_c(y) represents a dispersion of one standard deviation (approximately 68%68\% confidence for a normal distribution). In commerce and regulatory compliance, customers require a higher level of confidence—often specified as approximately 95%95\%, with other coverage levels possible.

The expanded uncertainty (UU) is obtained by multiplying uc(y)u_c(y) by a numerical coverage factor (kk):

U=k⋅uc(y)U = k \cdot u_c(y)

Coverage selection depends on the output distribution, reliability of component uncertainties, model approximation, and requested coverage. With a nearly normal output and adequate effective degrees of freedom, k≈2k\approx2 often gives approximately 95% coverage. Large degrees of freedom alone do not make a single dominant rectangular or arcsine contribution normal.

For a normally distributed, small-sample dominated budget meeting the Welch–Satterthwaite assumptions, use the appropriate Student t factor. There is no universal ISO rule that makes 30 a sharp cutoff. More complex or nonlinear models may require another propagation and coverage method.

Student's tt Reference Table for 95%95\% Confidence

Effective Degrees of Freedom (νeff\nu_{\text{eff}})Coverage Factor k=t95(νeff)k = t_{95}(\nu_{\text{eff}})
112.71
24.30
33.18
42.78
52.57
62.45
82.31
102.23
152.13
202.09
302.04
∞\infty1.96

Compliant Uncertainty Reporting under ISO/IEC 17025

A clear GUM-based expanded-uncertainty statement includes the following information. Applicable accreditation reporting policies can add requirements; ISO/IEC 17025 permits uncertainty in absolute or relative form:

  1. The measured numerical value of the measurand yy
  2. The expanded uncertainty UU
  3. Units for the result and uncertainty, or a clearly identified relative uncertainty with its basis
  4. The coverage factor kk used
  5. The approximate coverage probability (level of confidence, typically stated as "approximately 95%")

Rounding Conventions for Calibration Certificates

  1. Rounding the Expanded Uncertainty (UU): GUM 7.2.6 normally considers at most two significant digits adequate for uncertainty, while allowing more digits when needed for subsequent calculations. For two significant digits, 0.01634 mm0.01634\text{ mm} becomes 0.016 mm0.016\text{ mm}, and 4.782 Ω4.782\ \Omega becomes 4.8 Ω4.8\ \Omega. State and apply any required conservative rounding policy; rounding upward is not a universal mandatory rule.
  2. Rounding the Reported Calibrated Value (yy): For an absolute uncertainty, round the reported result consistently with the uncertainty’s final decimal place. Retain the unrounded values internally for calculations and decisions. Relative-uncertainty reports require their own clearly stated precision and units.

Compliant Reporting Template

Compliant Statement: "The measured resistance is 100.0248 Ω±0.0038 Ω100.0248\ \Omega \pm 0.0038\ \Omega. The reported expanded uncertainty is based on a combined standard uncertainty multiplied by a coverage factor of k=2.23k = 2.23, which for an effective degrees of freedom νeff=10\nu_{\text{eff}} = 10 defines a coverage probability of approximately 95%95\%."

Step-by-Step Worked Calibration Uncertainty Budget

A calibration laboratory calibrates a precision 100.0000 Ω100.0000\ \Omega standard resistor against a master reference standard using an automated direct-reading ratio set. The functional equation is Ruut=Rstd+ΔRR_{\text{uut}} = R_{\text{std}} + \Delta R.

Identifying the Uncertainty Components

  1. Type A Repeatability (u1u_1): Technician performs n=5n = 5 repeated observations: s=0.00300 Ωs = 0.00300\ \Omega.
u1=u(xˉ)=sn=0.00300 Ω5=0.001342 Ω,ν1=5−1=4u_1 = u(\bar{x}) = \frac{s}{\sqrt{n}} = \frac{0.00300\ \Omega}{\sqrt{5}} = 0.001342\ \Omega, \quad \nu_1 = 5 - 1 = 4
  1. Reference Standard Certificate (u2u_2): The hypothetical certificate states U=0.00200 ΩU=0.00200\ \Omega with k=2.00k=2.00. This example treats the reliability of the Type B uncertainty estimates as sufficient to use infinite degrees of freedom; the provider’s name alone would not justify that assumption.
u2=0.00200 Ω2.00=0.001000 Ω,ν2=∞u_2 = \frac{0.00200\ \Omega}{2.00} = 0.001000\ \Omega, \quad \nu_2 = \infty
  1. Digital Multimeter Resolution (u3u_3): Digital readout displays 0.001 Ω0.001\ \Omega (1 mΩ1\text{ m}\Omega). Rectangular semi-range a=0.0005 Ωa = 0.0005\ \Omega:
u3=0.000500 Ω3=0.000289 Ω,ν3=∞u_3 = \frac{0.000500\ \Omega}{\sqrt{3}} = 0.000289\ \Omega, \quad \nu_3 = \infty
  1. Oil Bath Temperature Variation (u4u_4): Bath temperature stable within ±0.10∘C\pm 0.10^\circ\text{C} (rectangular distribution). Resistor temperature coefficient α=10 ppm/∘C=10×10−6/∘C\alpha = 10\text{ ppm}/^\circ\text{C} = 10 \times 10^{-6}/^\circ\text{C}. Maximum resistance shift: a=100 Ω×(10×10−6/∘C)×0.10∘C=0.000100 Ωa = 100\ \Omega \times (10 \times 10^{-6}/^\circ\text{C}) \times 0.10^\circ\text{C} = 0.000100\ \Omega.
u4=0.000100 Ω3=0.000058 Ω,ν4=∞u_4 = \frac{0.000100\ \Omega}{\sqrt{3}} = 0.000058\ \Omega, \quad \nu_4 = \infty

Master Uncertainty Budget Table

Source of Uncertainty (XiX_i)Value (±a\pm a)Probability DistributionDivisorStandard Uncertainty u(xi)u(x_i)Sensitivity Coeff (cic_i)Uncertainty Contrib ui(y)u_i(y)Degrees of Freedom (νi\nu_i)
Repeatability (Type A)s=3.00 mΩs = 3.00\text{ m}\OmegaNormal (s/5s/\sqrt{5})5\sqrt{5}1.342 mΩ1.342\text{ m}\Omega1.01.01.342 mΩ1.342\text{ m}\Omega44
Master Standard (Type B)2.00 mΩ2.00\text{ m}\OmegaNormal (k=2k=2)2.02.01.000 mΩ1.000\text{ m}\Omega1.01.01.000 mΩ1.000\text{ m}\Omega∞\infty
Digital Resolution (Type B)0.50 mΩ0.50\text{ m}\OmegaRectangular3\sqrt{3}0.289 mΩ0.289\text{ m}\Omega1.01.00.289 mΩ0.289\text{ m}\Omega∞\infty
Temperature Bath (Type B)0.10 mΩ0.10\text{ m}\OmegaRectangular3\sqrt{3}0.058 mΩ0.058\text{ m}\Omega1.01.00.058 mΩ0.058\text{ m}\Omega∞\infty

Combine unrounded contributions

The contributions in milliohms are 3/53/\sqrt{5}, 11, 0.5/30.5/\sqrt{3}, and 0.1/30.1/\sqrt{3}. Their squared sum is 1.8+1+0.0833333+0.0033333=2.8866667 (mΩ)21.8+1+0.0833333+0.0033333=2.8866667\ (\mathrm{m}\Omega)^2. Thus uc=1.6990193mΩ=0.0016990193 Ωu_c=1.6990193\mathrm{m}\Omega=0.0016990193\ \Omega.

Effective degrees of freedom

With only the repeatability contribution assigned finite degrees of freedom, νeff=(2.8866667)2/(1.82/4)=10.28746\nu_{eff}=(2.8866667)^2/(1.8^2/4)=10.28746. Using the integer t table conservatively, use 10 degrees of freedom. This calculation assumes the conditions for the independent-component Welch–Satterthwaite approximation; do not use it unchanged for correlated inputs.

Determine Coverage Factor (kk) and Expanded Uncertainty (UU)

For the conservative integer-table choice of 10 effective degrees of freedom, the approximate two-sided 95% Student t factor is 2.23. This choice relies on the stated model assumptions; k = 2 is not automatically a 95% factor for every small-sample budget.

U=k⋅uc(y)=2.23×0.0016990 Ω=0.003789 ΩU = k \cdot u_c(y) = 2.23 \times 0.0016990\ \Omega = 0.003789\ \Omega

Rounding UU to two significant figures yields U=0.0038 ΩU = 0.0038\ \Omega (3.8 mΩ3.8\text{ m}\Omega).

If the measured mean was 100.00423 Ω100.00423\ \Omega, it is rounded to match UU at four decimal places:

Ruut=100.0042 Ω±0.0038 Ω(k=2.23,νeff=10,≈95% confidence)R_{\text{uut}} = 100.0042\ \Omega \pm 0.0038\ \Omega \quad (k = 2.23, \nu_{\text{eff}} = 10, \approx 95\% \text{ confidence})

Interpreting the reported interval

A reported expanded uncertainty is not the instrument’s allowable error, the customer’s tolerance, or a promise that every future indication will lie in the reported interval. It describes the stated measurement result under the conditions and coverage model used for that evaluation. Transfer to a different range, environment, time, or measurement use may require additional contributions.

Keep the result and conformity decision separate. A resistor can have a well-characterized value and uncertainty yet fail the customer’s tolerance under the agreed rule. Conversely, a result may lie numerically inside tolerance while uncertainty prevents acceptance under a guarded rule. Reporting the uncertainty supports that decision; it does not choose the rule.

For a relative report, identify the basis unambiguously. An absolute expanded uncertainty of 0.0038 ohm at a result near 100 ohms is approximately 38 ppm of that result. It is not 38 ppm of an arbitrary full-scale range. State the quantity, relevant conditions, coverage information, and any limitations so the recipient can use the report without guessing the denominator.

Test Your Knowledge

In a combined uncertainty budget, the combined standard uncertainty is u_c = 1.00 µm. The dominant uncertainty component is a Type A repeatability evaluation with u_1 = 1.00 µm based on n = 5 repeated observations (ν_1 = 4), while all other components are negligible Type B evaluations with infinite degrees of freedom. Using the Welch-Satterthwaite equation, what is the effective degrees of freedom ν_eff and the appropriate coverage factor k for approximate two-sided 95% coverage, assuming independent normal repeatability observations and the usual t-model approximation?

A

ν_eff = 5 and k = 2.00

B

ν_eff = 20 and k = 2.09

C

ν_eff = 1 and k = 12.71

D

ν_eff = 4 and k = 2.78

Test Your Knowledge

A laboratory calculates y = 50.01274 g and U = 0.00342 g, with k = 2 and approximately 95% coverage under its model. Its reporting policy uses two significant digits for U and rounds y to the same decimal place. Which report follows that policy?

A

y = 50.0127 g ± 0.0034 g (k = 2, approx. 95% confidence)

B

y = 50.01274 g ± 0.00342 g (k = 2, approx. 95% confidence)

C

y = 50.01 g ± 0.003 g (k = 2, approx. 95% confidence)

D

y = 50.01274 g ± 0.0034 g (k = 2, approx. 95% confidence)

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