Green's theorem
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In physics and mathematics, Green's theorem gives the relationship between a line integral around a simple closed curve C and a double integral over the plane region D bounded by C. Green's theorem was named after British scientist George Green and is a special case of the more general Stokes' theorem.
The theorem statement is the following. Let C be a positively oriented, piecewise smooth, simple closed curve in the plane and let D be the region bounded by C. If L and M have continuous partial derivatives on an open region containing D, then
- [\int_ L\, dx + M\, dy = \iint_ \left(\frac - \frac\right)\, dA.]
- [\oint_]
Proof of Green's theorem when D is a simple region
We will prove the theorem for the simplified area D where C2 and C4 are vertical lines, however the theorem remains valid for any area D as defined above.
If it can be shown that
- [\int_ L\, dx = \iint_ \left(- \frac\right) dA\qquad\mathrm]
- [\int_ M\, dy = \iint_ \left(\frac\right)\, dA\qquad\mathrm]
We define a region D that is simple enough for our purposes. If region D is expressed such that:
- [D = \]
[ \iint_ \left(\frac\right)\, dA] [=\int_a^b\!\!\int_^ \left[frac (x,y), dy, dx right] ] [ = \int_a^b \Big\ \, dx\qquad\mathrm] Now C can be rewritten as the union of four curves: C1, C2, C3, C4.
With C1, use the parametric equations, x = x, y = g1(x), a ≤ x ≤ b. Therefore:
- [\int_ L(x,y)\, dx = \int_a^b \Big\\, dx]
- [\int_ L(x,y)\, dx = -\int_ L(x,y)\, dx = - \int_a^b [L(x,g_2(x))]\, dx]
- [ \int_ L(x,y)\, dx = \int_ L(x,y)\, dx = 0]
[ \int_ L\, dx ] [ = \int_ L(x,y)\, dx + \int_ L(x,y)\, dx + \int_ L(x,y) + \int_ L(x,y)\, dx ] [ = -\int_a^b [L(x,g_2(x))]\, dx + \int_a^b [L(x,g_1(x))]\, dx\qquad\mathrm] Combining (3) with (4), we get:
- [\int_ L(x,y)\, dx = \iint_ \left(- \frac\right)\, dA]
See also
- Planimeter
- Method of image charges - A method used in electro statics that takes strong advantage of the uniqueness theorem (derived from Green's theorem)
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