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.
The vector field (y,0) gives different integrals along two paths with the same endpoints
Statement refuted
The field has the same vector line integral along every path from to .
Facts & Assumptions
Given: The paths and on .
A vector line integral is the integral of on a path (Scalar line integrals with respect to arc length and vector-field line integrals).
Vector line integrals add under concatenation and negate under reversal (Line integrals under reversal and concatenation).
Path independence is equivalent to zero integral around every closed piecewise- path on a piecewise- path-connected domain (Path independence is equivalent to zero integral around every closed piecewise-C1 path).
The power rule (For a natural the function is differentiable everywhere with derivative ; for it is the constant , with derivative ; for a natural the function is differentiable at every with derivative ; consequently every polynomial function is differentiable at every real, with the derivative computed term by term), together with Newton-Leibniz for a continuous function whose interior derivative admits an integrable extension (Newton–Leibniz needs only continuity on , differentiability on , and a Riemann-integrable extension of the interior derivative), evaluates polynomial integrals by endpoint increments.
Counterexample
Both paths run from to . Along , the first component is zero, so [L1] gives .
Along , one has and . Hence [L1] and [L4] give
The two values differ, so the field is not path-independent.
The concatenation is closed, and [L2] gives its integral as . This is the corresponding nonzero-loop failure in [L3].
Depends on
- Scalar line integrals with respect to arc length and vector-field line integrals
- Line integrals under reversal and concatenation
- Path independence is equivalent to zero integral around every closed piecewise-C1 path
- For a natural $n \ge 1$ the function $x \mapsto x^{n}$ is differentiable everywhere with derivative $\iota(n)\,x^{\,n-1}$; for $n = 0$ it is the constant $1$, with derivative $0$; for a natural $n \ge 1$ the function $x \mapsto x^{-n}$ is differentiable at every $x \ne 0$ with derivative $-\iota(n)\,x^{-n-1}$; consequently every polynomial function is differentiable at every real, with the derivative computed term by term
- Newton–Leibniz needs only continuity on $[a,b]$, differentiability on $(a,b)$, and a Riemann-integrable extension of the interior derivative
Used by
Nothing in the library uses this result yet.
Dependency tree · next 3 levels
Direct dependencies and their dependencies through the next three levels: 96 results over 20 levels. An arrow runs from a result to what uses it, and this result sits at the bottom with a heavier outline. Click the chart to enlarge it.
Sources
- J. Lebl, Basic Analysis II, Example 9.3.1 (standard reference, not scraped)