Why is Green's theorem for circular boundaries a consequence of Stoke's theorem?

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In summary, Green's theorem for circular boundaries is a mathematical theorem that relates the line integral of a two-dimensional vector field around a closed circular curve to the double integral of the curl of the same vector field over the area enclosed by the curve. Stoke's theorem is a fundamental theorem that relates the flux of a vector field through a surface to the line integral of the same vector field around the boundary of the surface. Green's theorem for circular boundaries is a special case of Stoke's theorem, where the surface is a circle and the vector field is defined in a two-dimensional space. It can be derived from Stoke's theorem using the parametrization of a circle and the definition of a curl in two dimensions. The practical applications of Green's theorem
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Chris L T521
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Here's this week's problem.

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Problem: Show that Green's theorem for regions in $\mathbb{R}^2$ with boundary consisting of a disjoint union of one or more circles is a consequence of Stoke's theorem.

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No one answered this week's question. You can find my solution below:

Pf: Let $C_1\subset\mathbb{R}$ be a circle with counterclockwise (positive) orientation and let $C_i\subset\text{Int}\,C_1$ for $i\geq 2$ be circles with clockwise (negative) orientation. For some region in $\mathbb{R}^2$ who's boundary is (homotopic to) a circle $C$, we know by Green's theorem that
\[\int_C f\,dx+g\,dy = \iint\limits_{R}\left(\frac{\partial g}{\partial x}-\frac{\partial f}{\partial y}\right)\,dA.\]
Now, if we take our region $M=M_1\backslash M_2\backslash M_3\backslash\cdots$ where $M_i=\text{Int}\,C_i$ for each $i\geq 1$, then it follows that $\displaystyle\partial M=\bigsqcup_i C_i$ (here, the box cup represents a disjoint union).

By Stoke's theorem, if we take $\omega=f\,dx+g\,dy$, we have that
\[\begin{aligned}\int_{\partial M}\omega &= \int_{\bigsqcup_i C_i} f\,dx+g\,dy\\ &= \sum_i \int_{C_i}f\,dx+g\,dy \\ &= \sum_i\int_{M_i}\left(\frac{\partial g}{\partial x}-\frac{\partial f}{\partial y}\right)\,dA\\ &= \int_M\left(\frac{\partial g}{\partial x}-\frac{\partial f}{\partial y}\right)\,dA\\ &= \int_M \,d\omega.\end{aligned}\]

Thus, Green's theorem for a region who's boundary is a disjoint union of one or more circles is a consequence of Stoke's theorem. Q.E.D.
 

FAQ: Why is Green's theorem for circular boundaries a consequence of Stoke's theorem?

What is Green's theorem for circular boundaries?

Green's theorem for circular boundaries is a mathematical theorem that relates the line integral of a two-dimensional vector field around a closed circular curve to the double integral of the curl of the same vector field over the area enclosed by the curve.

What is Stoke's theorem?

Stoke's theorem is a fundamental theorem in vector calculus that relates the flux of a vector field through a surface to the line integral of the same vector field around the boundary of the surface.

How is Green's theorem for circular boundaries related to Stoke's theorem?

Green's theorem for circular boundaries is a special case of Stoke's theorem, where the surface in question is a circle and the vector field is defined in a two-dimensional space.

Why is Green's theorem for circular boundaries a consequence of Stoke's theorem?

Green's theorem for circular boundaries can be derived from Stoke's theorem by using the parametrization of a circle and applying the definition of a curl in two dimensions.

What are the practical applications of Green's theorem for circular boundaries?

Green's theorem for circular boundaries is used in various fields such as physics, engineering, and computer graphics to calculate line integrals and solve problems involving circular boundaries and vector fields. It is also an important tool in the study of potential theory and fluid dynamics.

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