A conservative vector field on is a vector field for a globally defined smooth potential of a conservative vector field . The chain rule givesso its line integral is path independent.
Green theorem states that, for a bounded planar region with piecewise smooth boundary and continuously differentiable on a neighbourhood of its closure,The boundary is positively oriented: the region lies on the left while it is traversed, so outer components run counterclockwise and hole boundaries clockwise.
For the proposed potential of a conservative vector field, the fundamental theorem of calculus and differentiation under the integral sign giveSince , the last integral equals , including negative with the usual signed-integral convention. Hence the proposed potential is global andThe fact that the vector field is defined on all of ensures both straight integration segments stay inside its domain; a hole in the domain could obstruct a global potential.
Integrating the oscillatory term together with the constant components gives a potential of a conservative vector fieldDirect partial derivatives recover both components of , proving it is a conservative vector field. Its line integral is therefore path independent. At an integer endpoint , the sine term vanishes, so for any of the specified pathsAny other potential has the same gradient, so differs from by a constant on the connected plane. In particular every potential changes by under and by under . Equivalently the integral from to is , whereas a unit-periodic potential would make that difference zero. There is no potential periodic with period one in both coordinate directions. This is an example of how periods obstruct a periodic potential: a periodic vector field need not have a periodic potential.
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