Chapter 16 – Vector Calculus

26
Chapter 16 – Vector Calculus 16.3 The Fundamental Theorem for Line Integrals 16.3 The Fundamental Theorem for Line Integrals 1 Objectives: Understand The Fundamental Theorem for line integrals Determine conservative vector fields

description

Chapter 16 – Vector Calculus. 16.3 The Fundamental Theorem for Line Integrals. Objectives: Understand The Fundamental Theorem for line integrals Determine conservative vector fields. FTC – Part 2. - PowerPoint PPT Presentation

Transcript of Chapter 16 – Vector Calculus

Page 1: Chapter 16 – Vector Calculus

1

Chapter 16 – Vector Calculus16.3 The Fundamental Theorem for Line Integrals

16.3 The Fundamental Theorem for Line Integrals

Objectives: Understand The

Fundamental Theorem for line integrals

Determine conservative vector fields

Page 2: Chapter 16 – Vector Calculus

16.3 The Fundamental Theorem for Line Integrals

2

FTC – Part 2Recall from Section 5.3 that Part 2 of the

Fundamental Theorem of Calculus (FTC2) can be written as:

where F′ is continuous on [a, b].

'( ) ( ) ( )b

aF x dx F b F a

Page 3: Chapter 16 – Vector Calculus

16.3 The Fundamental Theorem for Line Integrals

3

Fundamental Theorem for Line IntegralsLet 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,

Cf d f b f a r r r

Page 4: Chapter 16 – Vector Calculus

16.3 The Fundamental Theorem for Line Integrals

4

NoteTheorem 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 f is

the net change in f.

Page 5: Chapter 16 – Vector Calculus

16.3 The Fundamental Theorem for Line Integrals

5

Note: If f is a function of two variables and C is a

plane curve with initial point A(x1, y1) and terminal point B(x2, y2), Theorem 2 becomes:

2 2 1 1, ,Cf d f x y f x y r

Page 6: Chapter 16 – Vector Calculus

16.3 The Fundamental Theorem for Line Integrals

6

Note: If f is a function of three variables and C is a

space curve joining the point A(x1, y1, z1) to the point B(x2, y2, z2), we have:

2 2 2 1 1 1, , , ,Cf d f x y z f x y z r

Page 7: Chapter 16 – Vector Calculus

16.3 The Fundamental Theorem for Line Integrals

7

PathsSuppose C1 and C2 are two piecewise-smooth

curves (which are called paths) that have the same initial point A and terminal point B.

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

1 2C Cd d F r F r

Page 8: Chapter 16 – Vector Calculus

16.3 The Fundamental Theorem for Line Integrals

8

Conservative Vector FieldHowever, one implication of

Theorem 2 is that

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.

1 2C Cf d f d r r

Page 9: Chapter 16 – Vector Calculus

16.3 The Fundamental Theorem for Line Integrals

9

Independence of a Path In general, if F is a continuous vector field

with domain D, we say that the line integral is independent of path if

for any two paths C1 and C2 in D that have the same initial and terminal points.

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

CdF r

1 2C Cd d F r F r

Page 10: Chapter 16 – Vector Calculus

16.3 The Fundamental Theorem for Line Integrals

10

Closed CurveA curve is called closed if its terminal point

coincides with its initial point, that is, r(b) = r(a)

Page 11: Chapter 16 – Vector Calculus

16.3 The Fundamental Theorem for Line Integrals

11

Theorem 3 is independent of path

in D if and only if:

for every closed path C in D.

CdF r

0C

d F r

Page 12: Chapter 16 – Vector Calculus

16.3 The Fundamental Theorem for Line Integrals

12

Physical InterpretationThe 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.

Page 13: Chapter 16 – Vector Calculus

16.3 The Fundamental Theorem for Line Integrals

13

Theorem 4Suppose F is a vector field that is continuous

on an open, connected region D.

If is independent of path in D, then F is a conservative vector field on D.

◦ That is, there exists a function f such that f=F.

CdF r

Page 14: Chapter 16 – Vector Calculus

16.3 The Fundamental Theorem for Line Integrals

14

Determining Conservative Vector FieldsThe question remains:

◦ How is it possible to determine whether or not a vector field is conservative?

Page 15: Chapter 16 – Vector Calculus

16.3 The Fundamental Theorem for Line Integrals

15

Theorem 5 If F(x, y) = P(x, y) i + Q(x, y) j is a conservative

vector field, where P and Q have continuous first-order partial derivatives on a domain D, then, throughout D, we have:

P Q

y x

Page 16: Chapter 16 – Vector Calculus

16.3 The Fundamental Theorem for Line Integrals

16

Conservative Vector FieldsThe converse of Theorem 5 is

true only for a special type of region, specifically simply-connected region.

Page 17: Chapter 16 – Vector Calculus

16.3 The Fundamental Theorem for Line Integrals

17

Simply Connected RegionA 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.

Page 18: Chapter 16 – Vector Calculus

16.3 The Fundamental Theorem for Line Integrals

18

Theorem 6Let 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.

Page 19: Chapter 16 – Vector Calculus

16.3 The Fundamental Theorem for Line Integrals

19

Example 1 – pg. 1106Determine whether or not F is a conservative

vector field. If it is, find a function f such that F = f.

2

3. ( , ) 2 3 3 4 8

4. ( , ) cos sin

( , ) cos sin cos

x x

x y x y x y

x y e y e y

x y xy xy xy x xy

F i j

F i j

F i j

Page 20: Chapter 16 – Vector Calculus

16.3 The Fundamental Theorem for Line Integrals

20

Example 2a) Find a function f such that F=f.

b) Use part (a) to evaluate along the given curve C.

CdF r

2 2 2

2

( , , ) 2 2 3 ,

: , 1, 2 1, 0 1

x y z xz y xy x z

C x t y t z t t

F i j k

Page 21: Chapter 16 – Vector Calculus

16.3 The Fundamental Theorem for Line Integrals

21

Example 3 – pg. 1107 # 24Find the work done by the force

field F in moving an object from P to Q.( , ) ; (0,1), (2,0)y yx y e xe P Q F i j

Page 22: Chapter 16 – Vector Calculus

16.3 The Fundamental Theorem for Line Integrals

22

Example 4Determine whether or not the given set is

a) open,

b) connected,

c) and simply-connected.

( , ) | 0x y x

Page 23: Chapter 16 – Vector Calculus

16.3 The Fundamental Theorem for Line Integrals

23

Example 5 – pg. 1106 # 12a) Find a function f such that F=f.

b) Use part (a) to evaluate along the given curve C.

CdF r

2 2

2

( , ) ,

is the arc of the parabola 2

from 1,2 to 2,8

x y x y

C y x

F i j

Page 24: Chapter 16 – Vector Calculus

16.3 The Fundamental Theorem for Line Integrals

24

Example 6 – pg. 1107 # 16a) Find a function f such that F=f.

b) Use part (a) to evaluate along the given curve C.

CdF r

2 2 2 2

2

( , , ) 2 2 2 ,

: , 1, , 0 1

x y z y z xz xyz xy x z

C x t y t z t t

F i j k

Page 25: Chapter 16 – Vector Calculus

16.3 The Fundamental Theorem for Line Integrals

25

Example 7 – pg. 1107 # 17a) Find a function f such that F=f.

b) Use part (a) to evaluate along the given curve C.

CdF r

2 2 2

( , , ) ,

: 1 1 2 , 0 2

xz xz xzx y z yze e xye

C t t t t t t

F i j k

r i j k

Page 26: Chapter 16 – Vector Calculus

16.3 The Fundamental Theorem for Line Integrals

26

Example 8 – pg. 1107 # 18a) Find a function f such that F=f.

b) Use part (a) to evaluate along the given curve C.

CdF r

( , , ) sin cos cos sin ,

: sin 2 , 0 2

x y z y x y z y z

C t t t t t

F i j k

r i j k