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Multivariate Calculus - Bruce E. Shapiro

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Lecture 23<br />

Green’s Theorem<br />

Theorem 23.1 Green’s Theorem. Let C be a closed, oriented curve enclosing a<br />

region R ⊂ R 2 with no holes, and let F = (M(x, y), N(x, y) be a vector field in R 2 .<br />

The<br />

∮ ∮<br />

( ∂N<br />

F · dr = (Mdx + Ndy) =<br />

∂x − ∂M )<br />

dA (23.1)<br />

∂y<br />

C<br />

C<br />

Proof. One way to evaluate the line integral about a closed path is to divide up<br />

the enclosed area into small rectangles. Focusing on a pair of small rectangles,<br />

R<br />

Figure 23.1: A closed curve may be filled with an large number of tiny rectangles.<br />

say R 1 and R 2 , the integral over the enclosing rectangle R 3 is equal to the sum of<br />

the line integrals over the individual rectangles because the common side cancels<br />

out, assuming the orientation of each individual small square is the same as the<br />

orientation of the enclosing curve.<br />

∫<br />

F · dr =<br />

R 3<br />

∫<br />

F · dr +<br />

R 1<br />

∫<br />

F · dr<br />

R 2<br />

The integral over the shared path cancels out because the two times the path<br />

is traversed it is traversed in different directions - hence the two integrals differ by<br />

a minus sign factor. This cancellation repeats itself as we add additional squares,<br />

191

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