Regard the planar vector field as , with no dependence on . Its curl is
Thus, for continuously differentiable and , the necessary and sufficient pointwise condition is
To deduce global path independence from this local condition also requires a suitable domain, for example a simply connected domain.
Set and . Their partial derivatives satisfy throughout . The vector field is smooth on the entire simply connected plane, so zero curl proves path independence.
Choose the broken straight path . Along its horizontal segment and , giving
Along its vertical segment and , giving
Therefore the line integral is
Figure 1.
Original sketch of the chosen oriented path through the corner at (2,0)
. Details.
An exact differential is an expression that equals for a single-valued differentiable function on the domain. Its line integral is an endpoint difference by the fundamental theorem for line integrals.
Integrating with respect to gives . Matching to requires . Hence
The arbitrary additive constant cancels. This constructs the vector-field potential globally and provides a second proof of path independence.
Assume a simple, piecewise smooth closed curve oriented counterclockwise around its enclosed region . Apply Green's theorem with and :
The orientation assumption is essential. A clockwise unit circle, , for , gives although its enclosed area is . For a self-intersecting curve the same line integral measures twice the signed area, with multiplicity, rather than necessarily twice an ordinary enclosed area.
For positive semiaxes , the ellipse has the counterclockwise parametrization , . Then
Therefore
If nonzero signed constants are allowed in place of positive semiaxes, the geometric area is .

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