We have discussed the orientation of curves and the orientation of surfaces. To state Stoke’s Theorem, we need to discuss boundary orientation:

Sketch

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We say has positive boundary orientation if is always on your left as you traverse while standing in the direction of the unit normal vector .

Remark

The boundary curve can be thought of as where the surface, ends, or the “edge” of a surface. Some surfaces have more than one boundary curve, and closed surfaces have no boundary curve.

Sketch

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We will mainly be dealing with surfaces with one boundary curve with positive boundary orientation.


Recall the circulation form of Green’s Theorem:

Where is the circulation around boundary and is the circulation throughout

The circulation form of Green’s theorem tell us the circulation throughout a flat surface is equal to the line integral around the boundary of . Stokes’ Theorem generalizes this result to higher-dimensional surfaces

Stoke's Theorem (Fundamental theorem for the Curl)

Let be an oriented surface whose boundary curve has positive boundary orientation, and let be a vector field whose component functions have continuous partial derivatives. Then:

Another way of stating Stokes’ Theorem:

where is the boundary of and is the curl of

Verbally

The circulation around the boundary of S is equal to the flux of the curl through S.

Moral

We can calculate a line integral as a flux integral


Proof of Stoke’s Theorem

We’ll do this for the special case where is the graph of a function, , and

Set-up

Sketch

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  • Parameterize by
  • Let be the projection of in the xy-plane. Parameterize by:
  • Then a parameterization of is found by “lifting” up to :

We Must Show

1. Right-Hand Side of (*)

We have:

has parameterization , so:

The surface integral is therefore:

2. Left-Hand Side of (*)

Using the parameterization of on the previous page, we compute the line integral directly:

Observe

, so by the chain rule:

graph TD
  z --> x
   z --> y
  x --> t["t"]
 y --> t2["t"]

Substituting and replacing , yields:

Observe

This is a line integral around the curve , which is , so by Green’s Theorem, we get:

Recall: , so by the chain rule:

graph TD
   P --> x
   P --> y
   P --> z
   z --> x2["x"]
	z --> y2["y"]

By the Chain and Product Rules, the part of the integrand in (***) are:

Subtracting the 2nd from the 1st, using Clairut’s Theorem o the “end” terms, and going back into the integrand gives:

This equals the surface integral from step 1 exactly, verifying (*) and therefore proving the theorem.


Remark

Observe that Green’s Theorem is a special case of Stokes’ Theorem. If is flat, , and

Which is the circulation form of Green’s Theorem.

Remark

We can finally prove:

(So far, we’ve only proved conservative .)

Proof

Let be any simple closed curve in . If is any surface with boundary curve , then by Stokes’:

And, because :

C was any simple closed curve, so for every simple closed curve . The result now falls like a stack of dominos: using results from sec. 16.3,

( For non-simple closed curves, break up into a union of simple closed curves. )