In the following 2D case, Green's theorem solves the following problem:
$$\vec{F}=\langle{xy+\ln{(\sin{e^{x})},x^2+e^{y^2}}}\rangle$$
$$\oint_C\vec{F}\cdot{d\vec{r}}=\iint_Dx\space{dA}$$
where C is the unit circle $x^2+y^2=1$, and D is the unit disk $x^2+y^2\le{1}$.
But what if instead the problem were:
$$\vec{F}=\langle{\frac{\sqrt{2}}{2}(xy+\ln{(\sin{e^x}}),x^2+e^{y^2},-\frac{\sqrt{2}}{2}(xy+\ln{(\sin{e^x}})}\rangle$$
$$\oint_C\vec{F}\cdot{d\vec{r}}$$
And $C$ is instead the unit circle $\vec{r}(t)=\langle{\frac{\sqrt{2}}{2}\cos{t},\sin{t},-\frac{\sqrt{2}}{2}\cos{t}}\rangle$.
This is the same problem as the first one, but rotated 45 degrees about the y-axis. I know I could solve the second problem by simply rotating the path and the vector field back 45 degrees. But is there any way to apply Green's theorem to the second problem directly?