How statement and proof provenance work
The first chip identifies the source of the statement or construction; the second identifies the source of its local proof or verification.
- Literature-sourced: the exact statement appears in a cited source; only wording and notation differ.
- AI-adapted: a semantically identical restatement of literature-sourced material, modulo indexing, notation, and boundary cases adopted by the library.
- AI-generated: a genuinely novel statement formulated by AI, with no source for the claim itself.
These labels describe origin, not correctness: citations and verification chips remain separate evidence.
First-order propagation of measurement uncertainty
Statement
Let , let for an open set , and let be differentiable at . Let be an -valued random element on one probability space with square-integrable coordinate variables , means , and almost surely. Let , set , and define Then The equality is exact for the first-order linearized output. To interpret it as an approximation to uncertainty in the nonlinear output , require to be a measurable, square-integrable random output (including a measurable definition on any null event where ) 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.
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.
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.
The real Frechet derivative on real and complex matrix spaces with the Frobenius norm: after identifying with real matrices, differentiability at means a real-linear first-order map whose remainder divided by the Euclidean input norm tends to zero.
Measurands, calibration, and measurement uncertainty: the input estimates are , , and for the stated first-order linearized output.
Proof
Identify with real matrices and let . By [F3], with . For the standard basis , put ; linearity gives . Thus is the first-order Taylor term.
Put . Then , and . Since each is square-integrable and is finite, the right side has finite expectation, so is square-integrable. Thus [F1] defines its variance and all covariances below.
By [F1], . Apply the finite bilinearity in [F2] to step 1.2; the constant has zero covariance, so .
By [F4], each covariance in step 2.1 is , so the double sum is . Symmetry in [F2] pairs the and 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 formula.
Remarks
No independence assumption is used. The formula includes covariance between calibration coefficients, reference standards, corrections, and any later reading included in . 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 nor alone supplies a confidence interval or coverage probability.
Depends on
Used by
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Sources
- JCGM 100:2008, Evaluation of Measurement Data — Guide to the Expression of Uncertainty in Measurement, clauses 4.1 and 5.1–5.2 (standard reference, not scraped)
- JCGM 100:2008/Amd.1:2026, Amendment 1: Nonlinearity in Measurement Models (standard reference, not scraped)
- NIST/SEMATECH Engineering Statistics Handbook, Chapter 2: Measurement Process Characterization (standard reference, not scraped)
- Sai Ravela, MIT OpenCourseWare, Quantifying Uncertainty: Summary lecture notes, Fall 2012 (standard reference, not scraped)