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The standard uncertainty of a calculated result follows approximately from input uncertainties, sensitivities and covariances.
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Formula
u(xi) has the unit of xi; (∂f/∂xi)u(xi) and uc(y) have the output unit of y.
| Symbol | Meaning | Unit |
|---|---|---|
| y=f(x1,…,xn) | Calculated result from measured inputs | output unit |
| Standard uncertainty of input quantity | unit of xi | |
| Sensitivity coefficient evaluated at the estimates | unit of y / unit of xi | |
| Covariance of two input quantities | unit of xi·xj |
u_c^2(y)=\sum_i\left(\frac{\partial f}{\partial x_i}\right)^2u^2(x_i)+2\sum_{i<j}\frac{\partial f}{\partial x_i}\frac{\partial f}{\partial x_j}u(x_i,x_j)NIST linearizes the measurement model at the best estimates. It assumes small uncertainties and a smooth model. For uncorrelated inputs, covariance terms vanish and contributions add in quadrature. Correlations can increase or decrease uncertainty. The result is a standard uncertainty, not automatically an expanded uncertainty or confidence interval.
NIST linearizes the measurement model at the best estimates. It assumes small uncertainties and a smooth model. For uncorrelated inputs, covariance terms vanish and contributions add in quadrature. Correlations can increase or decrease uncertainty. The result is a standard uncertainty, not automatically an expanded uncertainty or confidence interval.
The standard uncertainty of a calculated result follows approximately from input uncertainties, sensitivities and covariances.
Uncorrelated input quantities
Use only when covariances are zero or justifiably negligible.
Rework the example for “Propagation of Measurement Uncertainty” and explain why the check is valid.
For A=l·b with l=2.00±0.02 m and b=3.00±0.03 m, uncorrelated, A=6.00 m2 and u(A)=√(0.062+0.062)=0.0849 m2.
Check: terms under the root have m4, so the result has m2.
Ignoring an assumption of the formula: NIST linearizes the measurement model at the best estimates
Check units and model conditions before substitution; then verify the result in the original relation or a limiting case.
Formula cluster
Related relations in the formula sheet: stichprobenvarianz, kovarianz-stichprobe, standardfehler-anteil.
For A=l·b with l=2.00±0.02 m and b=3.00±0.03 m, uncorrelated, A=6.00 m2 and u(A)=√(0.062+0.062)=0.0849 m2. Check: terms under the root have m4, so the result has m2.
Labor reports, calibration and metrological uncertainty budgets.
Here is how to work through a typical Propagation of Measurement Uncertainty (u²c(y) = Σᵢ(ciui)² + 2Σᵢ<ⱼ cicj u(xᵢ,xⱼ)) task step by step:
Task
Rework the example for “Propagation of Measurement Uncertainty” and explain why the check is valid.
Solution path
For A=l·b with l=2.00±0.02 m and b=3.00±0.03 m, uncorrelated, A=6.00 m2 and u(A)=√(0.062+0.062)=0.0849 m2.
Check: terms under the root have m4, so the result has m2.
The standard uncertainty of a calculated result follows approximately from input uncertainties, sensitivities and covariances. The notation u2c(y) = Σi(ciui)2 + 2Σi<j cicj u(xi,xj) shows which quantities are connected. Here, y=f(x1,…,xn): Calculated result from measured inputs (output unit); u(xi): Standard uncertainty of input quantity (unit of xi); ci=∂f/∂xi: Sensitivity coefficient evaluated at the estimates (unit of y / unit of xi). u(xi) has the unit of xi; (∂f/∂xi)u(xi) and uc(y) have the output unit of y. An application depends on whether the supplied quantities match the definitions and reference directions. Common uses include Labor reports, calibration and metrological uncertainty budgets.. Read the variables and their dimensions before substituting numbers; this often reveals whether the result should be a length, rate, probability, or dimensionless statistic.
Start with a diagram or a list of known quantities, assign each one a symbol, and convert units to a consistent form. Then choose the appropriate equation and substitute values only afterward. Example: For A=l·b with l=2.00±0.02 m and b=3.00±0.03 m, uncorrelated, A=6.00 m2 and u(A)=√(0.062+0.062)=0.0849 m2. Check: terms under the root have m4, so the result has m2. Verification is part of the calculation: NIST linearizes the measurement model at the best estimates Also compare the magnitude and unit with the context. Round only at the end, since early rounding can affect multi-step calculations, especially when small differences or sums are involved.
NIST linearizes the measurement model at the best estimates. It assumes small uncertainties and a smooth model. For uncorrelated inputs, covariance terms vanish and contributions add in quadrature. Correlations can increase or decrease uncertainty. The result is a standard uncertainty, not automatically an expanded uncertainty or confidence interval. These are not minor footnotes: when assumptions fail, the formula can produce a precise but inappropriate result. Before calculating, identify which values are observed, estimated, or modeled, and whether special cases change the equation. Labor reports, calibration and metrological uncertainty budgets. For numerical methods, also check step size and stability; for statistics, sampling design and distribution; for calculus, differentiability, boundary, and orientation. Use another method when these conditions do not hold.
Both relations belong to the same topic, but answer different questions. “Propagation of Measurement Uncertainty”: The standard uncertainty of a calculated result follows approximately from input uncertainties, sensitivities and covariances. The companion relation “Sample Variance” The corrected sample variance measures spread around the sample mean and estimates the population variance. Choose based on the quantity sought and the model: Labor reports, calibration and metrological uncertainty budgets. The worked example For A=l·b with l=2.00±0.02 m and b=3.00±0.03 m, uncorrelated, A=6.00 m2 and u(A)=√(0.062+0.062)=0.0849 m2. Check: terms under the root have m4, so the result has m2. shows which quantities actually enter this relation. Compare both formulas using the same data and identify the companion’s extra assumption. This clarifies which relation fits.
Omit covariance terms only for uncorrelated inputs; include sensitivities. The symbols must also match their definitions exactly: y=f(x1,…,xn): Calculated result from measured inputs (output unit); u(xi): Standard uncertainty of input quantity (unit of xi); ci=∂f/∂xi: Sensitivity coefficient evaluated at the estimates (unit of y / unit of xi). Do not calculate mechanically; write the assumption beside the setup, then check dimensions and sign. Also note: NIST linearizes the measurement model at the best estimates The example For A=l·b with l=2.00±0.02 m and b=3.00±0.03 m, uncorrelated, A=6.00 m2 and u(A)=√(0.062+0.062)=0.0849 m2. Check: terms under the root have m4, so the result has m2. lets you follow these checks directly. If the assumptions do not fit, choose another relation from the chapter instead of forcing values into an unsuitable formula.
Quanta exam set
Curated exam set for "Propagation of Measurement Uncertainty":
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Which formula describes Propagation of Measurement Uncertainty?
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How do you rearrange Propagation of Measurement Uncertainty for Uncorrelated input quantities?
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Which common mistake happens with Propagation of Measurement Uncertainty?
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Create a curated FSRS exam set for u²c(y) = Σᵢ(ciui)² + 2Σᵢ<ⱼ cicj u(xᵢ,xⱼ): formula recall, variables, derivation, rearrangement, worked example, common mistakes and exam context.
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