Transcript Slide 1

Chapter 16 – Vector Calculus

16.3 The Fundamental Theorem for Line Integrals Objectives:  Understand The Fundamental Theorem for line integrals  Determine conservative vector fields 16.3 The Fundamental Theorem for Line Integrals 1

FTC – Part 2

 Recall from Section 5.3 that Part 2 of the Fundamental Theorem of Calculus (FTC2) can be written as: 

a b

 where

F′

is continuous on [

a

,

b

].

 16.3 The Fundamental Theorem for Line Integrals 2

Fundamental Theorem for Line Integrals

 Let

C

be a smooth curve given by the vector function

r

(

t

),

a

t

b

.

 Let

f

be a differentiable function of two or three variables whose gradient vector is continuous on

C

.  Then, 

C f d

r

f

r

 

f

r

 16.3 The Fundamental Theorem for Line Integrals 3

Note

 Theorem 2 says that we can evaluate the line integral of a conservative vector field (the gradient vector field of the potential function

f

) simply by knowing the value of

f

at the endpoints of

C

.

◦ In fact, it says that the line integral of net change in

f

.

 f is the 16.3 The Fundamental Theorem for Line Integrals 4

Note:

 If f is a function of two variables and

C

is a plane curve with initial point

A

(

x

1 ,

y

1 ) and terminal point

B

(

x

2 ,

y

2 ), Theorem 2 becomes: 

C f d

r

  2 , 2    1 , 1  16.3 The Fundamental Theorem for Line Integrals 5

Note:

 If f is a function of three variables and

C

is a  space curve joining the point

A

(

x

1 ,

y

1 ,

z

1 ) to the point

B

(

x

2 ,

y

2 ,

z

2 ), we have:

C f d

r

  2 , 2 , 2    1 , 1 , 1  16.3 The Fundamental Theorem for Line Integrals 6

Paths

 Suppose

C

1 and

C

same initial point 2 are two piecewise-smooth curves (which are called paths) that have the

A

and terminal point

B

.

 We know from Example 4 in Section 16.2 that, in general, 

C

1

F

d

r

 

C

2

F

d

r

16.3 The Fundamental Theorem for Line Integrals 7

Conservative Vector Field

 However, one implication of Theorem 2 is that 

C

1

r

 

C

2

f d

r

whenever  f is continuous.

◦ That is, the line integral of a conservative vector field depends only on the initial point and terminal point of a curve.

16.3 The Fundamental Theorem for Line Integrals 8

Independence of a Path

 In general, if domain

D

F

is a continuous vector field with independent of path if 

C

F

d

r

is 

C

1

F

d

r

 

C

2

F

d

r

for any two paths

C

1 and

C

2 in

D

same initial and terminal points.

that have the ◦ This means that line integrals of conservative vector fields are independent of path.

16.3 The Fundamental Theorem for Line Integrals 9

Closed Curve

 A curve is called closed if its terminal point coincides with its initial point, that is,

r

(

b

) =

r

(

a

) 16.3 The Fundamental Theorem for Line Integrals 10

Theorem 3

 

F

d

r

is independent of path in

D C

if and only if: 

C

F

d

r

 0 for every closed path

C

in

D

.

16.3 The Fundamental Theorem for Line Integrals 11

Physical Interpretation

 The physical interpretation is that: ◦ The work done by a conservative force field (such as the gravitational or electric field in Section 16.1) as it moves an object around a closed path is 0.

16.3 The Fundamental Theorem for Line Integrals 12

Theorem 4

 Suppose

F

is a vector field that is continuous on an open, connected region

D

.  

F

d

r

conservative vector field on

D .

D

, then

F

is a ◦ That is, there exists a function

f

such that  f=

F

.

16.3 The Fundamental Theorem for Line Integrals 13

Determining Conservative Vector Fields

 The question remains: ◦ How is it possible to determine whether or not a vector field is conservative?

16.3 The Fundamental Theorem for Line Integrals 14

Theorem 5

 If

F

(

x

,

y

) =

P

(

x

,

y

)

i

+

Q

(

x

,

y

)

j

throughout

D

, we have: is a conservative vector field, where

P

and

Q

have continuous first order partial derivatives on a domain

D

, then,

P

y

 

Q

x

16.3 The Fundamental Theorem for Line Integrals 15

Conservative Vector Fields

 The converse of Theorem 5 is true only for a special type of region, specifically simply-connected region.

16.3 The Fundamental Theorem for Line Integrals 16

Simply Connected Region

 A simply-connected region in the plane is a connected region

D

such that every simple closed curve in

D

encloses only points in

D

.

Intuitively, it contains no hole and can’t consist of two separate pieces.

16.3 The Fundamental Theorem for Line Integrals 17

Theorem 6

 Let

F

= P i + Q j be a vector field on an open simply-connected region

D

. Suppose that

P

and

Q

have continuous first-order derivatives and throughout

D .

◦ Then,

F

is conservative.

16.3 The Fundamental Theorem for Line Integrals 18

Example 1 – pg. 1106

3.

 Determine whether or not

F

is a conservative vector field. If it is, find a function

f

such that

F

=  f .

F

  2

x

 3

y x

4

y

 8 

j

4.

F

( , ) 

e x

cos

y

i

e x

sin

y

j F

 

xy

cos

xy

 sin

xy

i

 

x

2 cos

xy

j

16.3 The Fundamental Theorem for Line Integrals 19

Example 2

a) Find a function

f

such that

F

= 

f

.

b)

F

given curve

C

. 

C

F

d

r

  2

xz

y

2 

i

 2

xy

j

 

x

2  3

z

2 

k

, 

t

2 ,

y

1,

z

1, 0 1 16.3 The Fundamental Theorem for Line Integrals 20

Example 3 – pg. 1107 # 24

 Find the work done by the force field F in moving an object from P to Q.

F

e

y

i

xe

y

j

;

P

(0,1),

Q

(2, 0) 16.3 The Fundamental Theorem for Line Integrals 21

Example 4

 Determine whether or not the given set is a) b) c) open, connected, and simply-connected.

x

0

 16.3 The Fundamental Theorem for Line Integrals 22

Example 5 – pg. 1106 # 12

a) Find a function

f

such that

F

= 

f

.

b) given curve

C

. 

C

F

d

r F

x

2

i

y

2

j

,

C

is the arc of the parabola

y

from

  

 2

x

2 16.3 The Fundamental Theorem for Line Integrals 23

Example 6 – pg. 1107 # 16

a) Find a function

f

such that

F

= 

f

.

F

b)  given curve

C

. 

C

F

d

r

  2

y z

 2

xz

2 

i

 2

xyz

j

 

xy

2  2 2

x z

k

,

t

,

y

1,

z

t

2 , 0 1 16.3 The Fundamental Theorem for Line Integrals 24

Example 7 – pg. 1107 # 17

a) Find a function

f

such that

F

= 

f

.

F

C

:

r

b) given curve

C

. 

C

F

d

r

  

t

 2

yze

xz

i

1   

t

2

e xz

j

xye xz

k

,  1  

t

2  2

t

k

, 0 2 16.3 The Fundamental Theorem for Line Integrals 25

Example 8 – pg. 1107 # 18

a) Find a function

f

such that

F

= 

f

.

F

b)

C

:

r

given curve

C

. 

C

F

d

r

  sin

i

 

x

cos

y

 cos

z

j

y

i

t

j

k

0 2

k

16.3 The Fundamental Theorem for Line Integrals 26