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.
Exact finite Reynolds averaged equation
Statement
Let be an open interval, let be integers, let be open, and fix constants with and a common . For , let be continuously differentiable in with continuous second spatial derivatives, let be continuously differentiable, and let be continuous. Suppose pointwise that
Here , of a matrix field is rowwise, , and acts componentwise. Define the weighted means , , and , the fluctuations , and the covariance tensor . Then, pointwise on ,
and the exact averaged equation is
The tensor is symmetric positive semidefinite, with for every . With for , the pointwise energy split is . These are identities for the specified smooth functions; they assert neither existence of such solutions nor a statistical or physical interpretation.
Statement references
Facts & Assumptions
Finite weighted ensemble and covariance: For fixed weights summing to one, the weighted mean is and the fluctuation is .
Finite weighted ensemble and covariance: The cross-covariance is ; in particular the covariance tensor is .
The fields, fixed weights, common viscosity, divergence constraints, and pointwise equations satisfy every hypothesis in the Statement.
Given: The data in the Statement, including [A1] and the finite weighted mean and covariance convention [F1].
Proof
Because the weights are fixed constants and all sums are finite, each displayed derivative of a weighted mean is the same weighted sum of the corresponding derivatives. Thus , while .
For each , write and expand the outer product. Summing with weights gives , using step 1.1 and the covariance definition [F2].
Multiply the th equation in [A1] by and sum over . Fixed weights commute with all indicated linear differential operators, so the time, pressure, viscosity, and forcing terms become their barred means; substituting step 2.1 into the summed nonlinear term yields . The divergence constraint is step 1.1.
By [F2], , so it is symmetric and . Also , so expanding and using step 1.1 gives .