Theorem (Green's Theorem): If D is a simple region and P, Q have continuous partial derivatives on an open set containing D, then
∮∂DPdx+Qdy=∬D(∂x∂Q−∂y∂P)dA
It suffices to prove separately that ∮Pdx=−∬D∂y∂PdA and ∮Qdy=∬D∂x∂QdA.
Step 1: Prove ∮CPdx=−∬D∂y∂PdA.
Assume D is a type I region: D={(x,y):a≤x≤b,g1(x)≤y≤g2(x)}. The boundary ∂D consists of four pieces:
- C1: bottom, y=g1(x) from x=a to x=b
- C2: right side, x=b from y=g1(b) to y=g2(b)
- C3: top, y=g2(x) from x=b to x=a
- C4: left side, x=a from y=g2(a) to y=g1(a)
On C2 and C4, x is constant so dx=0, hence ∫C2Pdx=∫C4Pdx=0.
On C1: parametrize by x from a to b:
∫C1Pdx=∫abP(x,g1(x))dx
On C3: parametrize by x from b to a:
∫C3Pdx=∫baP(x,g2(x))dx=−∫abP(x,g2(x))dx
Therefore:
∮CPdx=∫ab[P(x,g1(x))−P(x,g2(x))]dx
For the double integral, using Fubini:
−∬D∂y∂PdA=−∫ab∫g1(x)g2(x)∂y∂Pdydx=−∫ab[P(x,g2(x))−P(x,g1(x))]dx
=∫ab[P(x,g1(x))−P(x,g2(x))]dx=∮CPdx✓
Step 2: Prove ∮CQdy=∬D∂x∂QdA.
The argument is analogous, treating D as a type II region D={(x,y):c≤y≤d,h1(y)≤x≤h2(y)}. On the portions where y is constant, dy=0. The remaining integrals give:
∮CQdy=∫cd[Q(h2(y),y)−Q(h1(y),y)]dy=∫cd∫h1(y)h2(y)∂x∂Qdxdy=∬D∂x∂QdA
Step 3: Combine.
Adding the two results:
∮CPdx+Qdy=∬D(∂x∂Q−∂y∂P)dA□