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First-order propagation of measurement uncertainty

Statement

Let d≥1, let x^∈U for an open set U⊆Rd, and let f:U→R be differentiable at x^. Let X be an Rd-valued random element on one probability space with square-integrable coordinate variables Xi, means E[Xi]=x^i, and X∈U almost surely. Let Σij=Cov⁡(Xi,Xj), set g=∇f(x^), and define Qlin=f(x^)+gT(X−x^),uc2=Var⁡(Qlin). Then uc2=gTΣg=∑i=1dgi2Σii+2∑1≤i<j≤dgigjΣij. The equality is exact for the first-order linearized output. To interpret it as an approximation to uncertainty in the nonlinear output f(X), require f(X) to be a measurable, square-integrable random output (including a measurable definition on any null event where X∉U) and require the first-order model to be adequate. This interpretation is not an assertion of exact finite-sample variance or interval coverage.

Facts & Assumptions

Given: The objects and hypotheses of the Statement.

[F1]

Moments, variance, and covariance on a probability space: for square-integrable real random variables, variance and covariance are the expectations of the centered square and centered product.

[F2]

Covariance is symmetric and bilinear in finite linear combinations: covariance is symmetric and bilinear on finite linear combinations of square-integrable real random variables on one common probability space; constant summands are allowed.

[F3]

The real Frechet derivative on real and complex matrix spaces with the Frobenius norm: after identifying Rd with d×1 real matrices, differentiability at x^ means a real-linear first-order map whose remainder divided by the Euclidean input norm tends to zero.

[F4]

Measurands, calibration, and measurement uncertainty: the input estimates are x^i=E[Xi], Σij=Cov⁡(Xi,Xj), and uc2=Var⁡(Qlin) for the stated first-order linearized output.

Proof

1.1givenF3choosealgebra

Identify Rd with real d×1 matrices and let L=Df(x^). By [F3], f(x^+h)=f(x^)+L[h]+r(h) with r(h)/∥h∥→0. For the standard basis ei, put gi=L[ei]; linearity gives L[h]=∑igihi=gTh. Thus Qlin is the first-order Taylor term.

1.2givenF1algebra

Put c=f(x^)−gTx^. Then (∑igiXi)2≤d∑igi2Xi2, and (c+∑igiXi)2≤2c2+2d∑igi2Xi2. Since each Xi is square-integrable and d is finite, the right side has finite expectation, so Qlin is square-integrable. Thus [F1] defines its variance and all covariances below.

2.1F1F2step 1.2algebra

By [F1], Var⁡(Qlin)=Cov⁡(Qlin,Qlin). Apply the finite bilinearity in [F2] to step 1.2; the constant has zero covariance, so Var⁡(Qlin)=∑i=1d∑j=1dgigjCov⁡(Xi,Xj).

3.1F1F2F4step 2.1algebra∎

By [F4], each covariance in step 2.1 is Σij, so the double sum is gTΣg. Symmetry in [F2] pairs the (i,j) and (j,i) terms to give the stated diagonal and off-diagonal form. It is nonnegative because it equals the variance in [F1], and [F4] therefore gives the stated uc2 formula.

Remarks

No independence assumption is used. The formula includes covariance between calibration coefficients, reference standards, corrections, and any later reading included in X. The first-order Taylor rule is appropriate only when the nonlinear remainder is negligible for the measurement at hand. JCGM 100:2008/Amd.1:2026 calls for higher-order terms when nonlinearity is significant; Monte Carlo methods are outside this result. Neither uc nor uc2 alone supplies a confidence interval or coverage probability.

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