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A field with vanishing curl on a star-shaped open subset of is conservative
Statement
Let be open and star-shaped and let be with on . Then a field with vanishing curl on a star-shaped open subset of is exact, conservative and path-independent: there is a function with , any two piecewise- paths in with the same endpoints give the same vector line integral, and
for every closed piecewise- path in . Conversely, a field exact on such a set has vanishing curl, so on a star-shaped open subset of vanishing curl and exactness are equivalent.
Facts & Assumptions
Given: The star-shaped open set with a star centre , and the field with on .
A nonempty open set is star-shaped with respect to when for every and (Star-shaped open subsets of Euclidean space).
For a continuous field on an open , a function is a potential when ; is conservative when it has a potential, and path-independent when any two piecewise- paths in with the same initial and terminal points have equal vector line integrals (Piecewise-C1 path-connected domains, potential functions, conservative fields, and path independence).
The curl of a field on an open is (Divergence and curl of a vector field).
A field on an open subset of is closed if and only if its curl vanishes identically (A field on an open subset of is closed exactly when its curl vanishes).
Let be open and star-shaped and let be . Then the five conditions that be closed, exact, conservative, path-independent, and give every closed piecewise- path in zero integral are equivalent (On a star-shaped open domain, closed, exact, conservative, path-independent, and zero-loop are equivalent).
Proof
The field is on the open set and its curl vanishes identically, so by the reverse direction of [L1] it is closed.
By [F1] the set is nonempty, open and star-shaped with respect to its centre . With these are exactly the hypotheses [L2] places on the domain, and is as [L2] requires of the field.
By steps 1.1 and 1.2, [L2] applies and its first condition holds, so all five hold: is exact, hence there is a function on with ; is conservative, so it has a potential in the sense of [F2]; is path-independent; and every closed piecewise- path in gives integral zero.
For the converse reading, suppose instead that is exact on . Then the first condition of [L2] holds by the same equivalence, so is closed, and the forward direction of [L1] makes vanish identically. Together with step 2.1 this gives the stated equivalence between vanishing curl and exactness on a star-shaped open subset of .
Remarks
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The hypothesis on the domain is doing work. Star-shapedness is not a convenience: the companion examples page gives a field with vanishing curl on a connected open subset of that has no potential. What fails there is exactly [F1], since no point of the complement of a line is a star centre for it.
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Why the potential is and not merely . Exactness in Exact and closed C1 vector fields asks for a potential, which is what makes all mixed second partial derivatives of available and continuous; a conservative field in the sense of [F2] is only required to have a one. Step 2.1 supplies the stronger form because [L2] does.
Depends on
- A $C^1$ field on an open subset of $\mathbb R^3$ is closed exactly when its curl vanishes
- On a star-shaped open domain, closed, exact, conservative, path-independent, and zero-loop are equivalent
- Star-shaped open subsets of Euclidean space
- Piecewise-C1 path-connected domains, potential functions, conservative fields, and path independence
- Divergence and curl of a $C^1$ vector field
Used by
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Sources
- M. Corral, Vector Calculus, chapter 4 (LibreTexts) (standard reference, not scraped)
- J. Feldman, A. Rechnitzer and E. Yeager, CLP-4 Vector Calculus (University of British Columbia), section 4.1 (standard reference, not scraped)