ProofComplete

Proof of Green's Theorem

We prove Green's theorem for a simple region, demonstrating the fundamental connection between line integrals and double integrals.


Proof

Theorem (Green's Theorem): If DD is a simple region and PP, QQ have continuous partial derivatives on an open set containing DD, then DPdx+Qdy=D(QxPy)dA\oint_{\partial D} P\,dx + Q\,dy = \iint_D \left(\frac{\partial Q}{\partial x} - \frac{\partial P}{\partial y}\right) dA

It suffices to prove separately that Pdx=DPydA\oint P\,dx = -\iint_D \frac{\partial P}{\partial y}\,dA and Qdy=DQxdA\oint Q\,dy = \iint_D \frac{\partial Q}{\partial x}\,dA.

Step 1: Prove CPdx=DPydA\oint_C P\,dx = -\iint_D \frac{\partial P}{\partial y}\,dA.

Assume DD is a type I region: D={(x,y):axb,  g1(x)yg2(x)}D = \{(x,y) : a \leq x \leq b, \; g_1(x) \leq y \leq g_2(x)\}. The boundary D\partial D consists of four pieces:

  • C1C_1: bottom, y=g1(x)y = g_1(x) from x=ax = a to x=bx = b
  • C2C_2: right side, x=bx = b from y=g1(b)y = g_1(b) to y=g2(b)y = g_2(b)
  • C3C_3: top, y=g2(x)y = g_2(x) from x=bx = b to x=ax = a
  • C4C_4: left side, x=ax = a from y=g2(a)y = g_2(a) to y=g1(a)y = g_1(a)

On C2C_2 and C4C_4, xx is constant so dx=0dx = 0, hence C2Pdx=C4Pdx=0\int_{C_2} P\,dx = \int_{C_4} P\,dx = 0.

On C1C_1: parametrize by xx from aa to bb: C1Pdx=abP(x,g1(x))dx\int_{C_1} P\,dx = \int_a^b P(x, g_1(x))\,dx

On C3C_3: parametrize by xx from bb to aa: C3Pdx=baP(x,g2(x))dx=abP(x,g2(x))dx\int_{C_3} P\,dx = \int_b^a P(x, g_2(x))\,dx = -\int_a^b P(x, g_2(x))\,dx

Therefore: CPdx=ab[P(x,g1(x))P(x,g2(x))]dx\oint_C P\,dx = \int_a^b [P(x, g_1(x)) - P(x, g_2(x))]\,dx

For the double integral, using Fubini: DPydA=abg1(x)g2(x)Pydydx=ab[P(x,g2(x))P(x,g1(x))]dx-\iint_D \frac{\partial P}{\partial y}\,dA = -\int_a^b \int_{g_1(x)}^{g_2(x)} \frac{\partial P}{\partial y}\,dy\,dx = -\int_a^b [P(x, g_2(x)) - P(x, g_1(x))]\,dx

=ab[P(x,g1(x))P(x,g2(x))]dx=CPdx= \int_a^b [P(x, g_1(x)) - P(x, g_2(x))]\,dx = \oint_C P\,dx \quad \checkmark

Step 2: Prove CQdy=DQxdA\oint_C Q\,dy = \iint_D \frac{\partial Q}{\partial x}\,dA.

The argument is analogous, treating DD as a type II region D={(x,y):cyd,  h1(y)xh2(y)}D = \{(x,y) : c \leq y \leq d,\; h_1(y) \leq x \leq h_2(y)\}. On the portions where yy is constant, dy=0dy = 0. The remaining integrals give: CQdy=cd[Q(h2(y),y)Q(h1(y),y)]dy=cdh1(y)h2(y)Qxdxdy=DQxdA\oint_C Q\,dy = \int_c^d [Q(h_2(y), y) - Q(h_1(y), y)]\,dy = \int_c^d \int_{h_1(y)}^{h_2(y)} \frac{\partial Q}{\partial x}\,dx\,dy = \iint_D \frac{\partial Q}{\partial x}\,dA

Step 3: Combine.

Adding the two results: CPdx+Qdy=D(QxPy)dA\oint_C P\,dx + Q\,dy = \iint_D \left(\frac{\partial Q}{\partial x} - \frac{\partial P}{\partial y}\right) dA \quad \square


RemarkExtension to general regions

For regions that are not simultaneously type I and type II, Green's theorem is proved by cutting the region into pieces that are both types, applying the theorem to each piece, and noting that line integrals along the cuts cancel (they are traversed in opposite directions by adjacent pieces). This "cutting and pasting" argument extends the theorem to any region bounded by finitely many piecewise smooth curves.