We return to Green's theorem

Setting

we have

Thus in terms of

,
Green's theorem can be written

Since any plane can be coordinatized as the

-plane,
this result can be phrased as follows: Let

be a flat surface in space bounded by a Jordan curve

.
If

is continuously differentiable on

,
then

where

is a unit normal for

and the line integral is taken in the positive sense, meaning, in the
direction of the unit tangent

for which

points away from the surface. (An observer marching along

in the attitude of

keeps the surface to his or her left.)
Consider a polyhedral surface

bounded by a closed polygonal path

.
The surface

consists of a finite number of flat faces

with polygonal boundaries

and unit normals

.
We choose these unit normals in a consistent manner; that is, they emanate
from the same side of the surface. Now let

be a vector function of norm

which is

on

,

on

,

on

,
etc. How

is defined on the line segments that join the different faces is immaterial.
Suppose now that

is a vector function continuously differentiable on an open set that contains

.
Then

the integral over

being taken in the positive sense with respect to

Now when we add these line integrals, we find that all the line segments that
make up the

but are not part of

are traversed twice and in opposite directions. Thus these line segments
contribute nothing to the sum of the line integrals and we are left with the
integral around

.
It follows that for a polyhedral surface

with boundary



This result can be extended to smooth surfaces with smooth bounding curves by approximating these configurations by polyhedral configurations of the type considered and using a limit process. In an admittedly informal way we have arrived at Stokes's theorem.
THEOREM STOKES'S THEOREM
Let

be a smooth surface with a smooth bounding curve

.
If

is continuously differentiable on an open set that contains

,
then

where

is a unit normal that varies continuously on

and the line integral is taken in the positive sense with respect to

Problem 1. Verify Stokes's theorem for

taking

as the portion of the ellipsoid

that lies above the plane

Solution. A little algebra shows that

is the graph of

with

restricted to the disc

Now

Taking

as the upper unit normal, we have



The bounding curve for

is the set of all

with

and

.
We can parametrize

by setting

Since

is the upper unit normal, this parametrization gives

in the positive sense. Thus


This is the value we obtained for the surface integral.
Problem 2. Verify Stokes's theorem for

taking

as the upper half of the unit sphere

Solution. We use the upper unit normal

.
Now

Therefore


The first integral is zero because

is symmetric about the

-plane
and the integrand is odd with respect to

.
The second integral is zero because

is symmetric about the

-plane
and the integrand is odd with respect to

.
Thus

This is also the value of the integral along the bounding base circle taken in
the positive sense:

Earlier we saw that the curl of a gradient is zero. Using Stokes's theorem we can prove a partial converse.
If a vector field

is continuously differentiable on an open convex set

and

on all of

,
then

is the gradient of some scalar field

defined on

Proof. Choose a point

in

and for each point

in

define

(This is the line integral from

to

taken along the line segment that joins these two points. We know that this
line segment lies in

because

is convex.)
Since

is open,

is in

for all

sufficiently small. Assume then that

is sufficiently small for

to be in

.
Since

is convex, the triangular region with vertices at

lies in

.
Since

on

,
we can conclude from Stokes's theorem that

Therefore


By our definition of

we have

We can parametrize the line segment from

to

by

with

.
Therefore




That

follows from observing that

is

:
as

,


as Circulation per Unit Area; Irrotational Flow
Interpret

as the velocity of a fluid flow. We stated that

measures the rotational tendency of the fluid. Now we can be more precise.
Take a point

within the flow and choose a unit vector

.
Let

{}
be the

-disc
that is centered at

and is perpendicular to

.
Let

be the circular boundary of

directed in the positive sense with respect to

.
By Stokes's theorem

The line integral on the right is called the circulation of

around

.
Thus we can say that
(the average

-component
of

on

(the area of

)
= the circulation of

around

It follows that
the average

-component
of

on

Taking the limit as

shrinks to

,
we see that
the

-component
of

at P


At each point

the component of

in any direction

is the circulation of

per unit area in the plane normal to

.
If

identically, the fluid has no rotational tendency and the flow is called
irrotational.
The Cauchy Mean Value Theorem is the basic tool needed to prove a theorem
which facilitates evaluation of limits of the form

when

Theorem. Suppose that

and suppose also that

exists. Then

exists, and

PROOF. The hypothesis that

exists contains two implicit assumptions:
(1) there is an interval

such that

and

exist for all

in

except, perhaps, for

,
(2) in this interval

with, once again, the possible exception of

On the other hand,

and

are not even assumed to be defined at

.
If we define

(changing the previous values of

and

,
if necessary), then

and

are continuous at

.
If

,
then the Mean Value Theorem and the Cauchy Mean Value Theorem apply to

and

on the interval

(and a similar statement holds for

).
First applying the Mean Value Theorem to

,
we see that

,
for if

there would be some

in

with

,
contradicting (2). Now applying the Cauchy Mean Value Theorem to

and

,
we see that there is a number

.
in

such that

or

Now

approaches

as

approaches

,
because

,
is in

;
since

exists, it follows that

Theorem. Suppose that

is a function for which

all exists. Let

and define

Then

Proof. Define

and

.
We prove that

Notice that


Thus




and

We may therefore apply l'H\opital's Rule

times to obtain

Since

is a polynomial of degree

,
its

st
derivative is constant; in fact,

.
Thus

Therefore

Definition. The polynomial

is called the Taylor polynomial of degree

for

at

.
Two functions

and

are said to be equal up to order

at

if

The above theorem says that the Taylor polynomial equals

up to order

near

.
Theorem. Let

and

be two polynomials in

,
of degree

,
and suppose that

and

are equal up to order

neat

.
Then

Proof. Let

.
Then

is a polynomial of degree

.
Write

The given condition

implies that

For

,
we have

Thus

and

Therefore

For

,
we have

Thus

and

Continuing this way we see that

Corollary. Let

be

-times
differentiable at

,
and suppose that

is a polynomial in

of degree

,
which equals

up to order

at

.
Then

,
the Taylor polynomial of degree

for

near a.
Write






Adding up these identities, we have

Theorem. Suppose that

,

are defined on

and

is defined by

Then
(1) there exists some

in

such that

(2) there exists some

in

such that

Moreover, if

is integrable on

then
(3)

Proof. Fix

and

.
Define

for

in

.
Then

Applying the Mean Value Theorem to

on the interval

there
exists some

in

such that

Note that


Therefore

This is called the Cauchy form of remainder.
Set

.
Now apply the Cauchy Mean value Theorem to

and

there exists some

in

such that

Therefore

or

This is called the Lagrange form of the remainder.
If

is integrable on

,
it follows from the Fundamental Theorem of Calculus that

Therefore

This is called the integral form of the remainder.



From the equation

we have

for all

From the equation

we have

