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If F\vec{F} Is a Path-Independent Field, Then CFdr=0\int _ { C } \vec { F } \cdot d \vec { r } = 0

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If F\vec{F} is a path-independent field, then CFdr=0\int _ { C } \vec { F } \cdot d \vec { r } = 0 where C has the parameterization r(t)=costi+sintj,0<t<3π\vec { r } ( t ) = \cos t \vec { i } + \sin t \vec { j } , 0 < t < 3 \pi


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