Green's Theorem

Green's Theorem for Elementary Regions

see elementary regions

Lemma 1

Let DR2 be y-simple and P:DR be a C1 function on D and D is a C1 path

D+Pdx=DPydA

where + is counter-clockwise

pf:
Say D is like

Pasted image 20241213150401.webp|422

DPydA=abϕ1(x)ϕ2(x)Pydydx=ab(P(x,ϕ2(x))P(x,ϕ1(x)))dx=ab(P(x,ϕ1(x))P(x,ϕ2(x)))dx=c3Pdx+c1Pdx=DPdx

The same follows for x-simple regions

D+Qdy=DQxdA

Green's theorem

Assume D is a closed simple region
and P:DR and Q:DR are C1

D+Pdx+Qdy=D(QxPy)dA

We can think of a vector field F=[P,Q]

This is equivalent to using curl

since curF=|ijkxxzPQ0|=[00QxPy]

So we have

D+Fds=D(curF)kdA

where k=[0,0,1]T

Flux and Green's theorem

If c(t) is a C1 curve in the form of c(t)=[x(t)y(t)]

then we can compute the unit normal at t as:

n(t)=1||c(t)||[y(t)x(t)]

where

n(t)T(t)=0

(see unit tangent)
Let c:[0,T]R2 be a parameterization of D+

DFnds=0TF(c(t))n||c(t)||dt=0T(P(c(t))y(t)Q(c(t))x(t))dt=D+PdyQdx=D(Qy+Px)dA

Using divergence we can write this as:

DFnds=DdivFdA

Area of a Simple Region

A(D)=12D+xdyydx=12Dxx(y)ydA=D1dA