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Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

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Chapter 6 The Integral Sections 6.1, 6.2, and 6.3
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Page 1: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

Chapter 6The Integral

Sections 6.1, 6.2, and 6.3

Page 2: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

The Indefinite Integral

Substitution

The Definite Integral As a Sum

The Definite Integral As Area

The Integral

Page 3: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

A physicist who knows the velocity of a particle might wish to know its position at a given time.

A biologist who knows the rate at which a bacteria population is increasing might want to deduce what the size of the population will be at some future time.

Introduction

Page 4: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

In each case, the problem is to find a function F whose derivative is a known function f.

If such a function F exists, it is called an antiderivative of f.

Antiderivatives

Definition

A function F is called an antiderivative of f on

an interval I if F’(x) = f (x) for all x in I.

Page 5: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

For instance, let f (x) = x2.

• It is not difficult to discover an antiderivative of f if we keep the Power Rule in mind.

• In fact, if F(x) = ⅓ x3, then F’(x) = x2 = f (x).

Antiderivatives

Page 6: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

However, the function G(x) = ⅓ x3 + 100 also satisfies G’(x) = x2.

• Therefore, both F and G are antiderivatives of f.

Indeed, any function of the form H(x)=⅓ x3 + C, where C is a constant, is an antiderivative of f.

• The question arises: Are there any others?

Antiderivatives

Page 7: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

If F is an antiderivative of f on an interval I, then the most general antiderivative of f on I is

F(x) + C

where C is an arbitrary constant.

Theorem

Antiderivatives

Page 8: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

Going back to the function f (x) = x2, we see that the general antiderivative of f is ⅓ x3 + C.

Antiderivatives

Page 9: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

Family of Functions By assigning specific values to C, we obtain a

family of functions.

• Their graphs are vertical

translates of one another.

• This makes sense, as each

curve must have the same

slope at any given value

of x.

Page 10: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

Notation for Antiderivatives

The symbol is traditionally used to represent the most general an antiderivative of f on an open interval and is called the indefinite integral of f .

Thus, means F’(x) = f (x)

( )f x dx

( ) ( )F x f x dx

Page 11: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

( )f x dxThe expression:

read “the indefinite integral of f with respect to x,” means to find the set of all antiderivatives of f.

( )f x dx

Integral sign Integrand

x is called the variable of integration

Indefinite Integral

Page 12: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

For example, we can write

• Thus, we can regard an indefinite integral as representing an entire family of functions (one antiderivative for each value of the constant C).

3 32 2because

3 3

x d xx dx C C x

dx

Indefinite Integral

Page 13: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

Every antiderivative F of f must be of the form F(x) = G(x) + C, where C is a constant.

Example: 26 3xdx x C

Represents every possible antiderivative of 6x.

Constant of Integration

Page 14: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

1

if 11

nn x

x dx C nn

Example:4

3

4

xx dx C

Power Rule for the Indefinite Integral

Page 15: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

1 1lnx dx dx x C

x

x xe dx e C

Indefinite Integral of ex and bx

ln

xx b

b dx Cb

Power Rule for the Indefinite Integral

Page 16: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

Sum and Difference Rules

f g dx fdx gdx

Example:

2 2x x dx x dx xdx 3 2

3 2

x xC

Page 17: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

( ) ( )kf x dx k f x dx ( constant)k

4 43 32 2 2

4 2

x xx dx x dx C C

Constant Multiple Rule

Example:

Page 18: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

Example - Different Variable

Find the indefinite integral:

273 2 6ue u du

u

213 7 2 6ue du du u du du

u

323 7ln 6

3ue u u u C

Page 19: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

Position, Velocity, and Acceleration Derivative Form

If s = s(t) is the position function of an object at time t, then

Velocity = v = Acceleration = a = ds

dtdv

dt

Integral Form

( ) ( )s t v t dt ( ) ( )v t a t dt

Page 20: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

Integration by Substitution

Method of integration related to chain rule. If u is a function of x, then we can use the formula

/

ff dx du

du dx

Page 21: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

Example: Consider the integral:

92 33 5x x dx3 2pick +5, then 3 u x du x dx

10

10

uC

9u du 103 5

10

xC

Sub to get Integrate Back Substitute

23

dudx

x

Integration by Substitution

Page 22: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

2Let 5 7 then 10

duu x dx

x

Example: Evaluate

3/ 21

10 3/ 2

uC

3/ 225 7

15

xC

25 7x x dx

2 1/ 215 7

10x x dx u du

Pick u, compute du

Sub in

Sub in

Integrate

Page 23: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

3ln

dx

x xLet ln then u x xdu dx

3

3ln

dxu du

x x

2

2

uC

2ln

2

xC

Example: Evaluate

Page 24: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

3

3 2

t

t

e dt

e 3

3Let +2 then

3t

t

duu e dt

e

3

3

1 1

32

t

t

e dtdu

ue

ln

3

uC

3ln 2

3

teC

Example: Evaluate

Page 25: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

Let f be a continuous function on [a, b]. If F is any antiderivative of f defined on [a, b], then the definite integral of f from a to b is defined by

( ) ( ) ( )b

af x dx F b F a

The Definite Integral

( )b

af x dx is read “the integral, from a to b of f (x) dx.”

Page 26: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

In the notation ,

f (x) is called the integrand.

a and b are called the limits of integration; a is the lower limit and b is the upper limit.

For now, the symbol dx has no meaning by itself; is all one symbol. The dx simply indicates that the independent variable is x.

( )b

af x dx

Notation

Page 27: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

The procedure of calculating an integral is called

integration. The definite integral is a

number. It does not depend on x.

Also note that the variable x is a “dummy variable.”

( )b

af x dx

( ) ( ) ( )b b b

a a af x dx f t dt f r dr

The Definite Integral

Page 28: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

Geometric Interpretationof the Definite Integral

The Definite Integral As Area

The Definite Integral As Net Change of Area

Page 29: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

If f is a positive function defined for a ≤ x ≤ b,

then the definite integral represents the

area under the curve y = f (x) from a to b

( )b

af x dx

( )b

aA f x dx

Definite Integral As Area

Page 30: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

If f is a negative function for a ≤ x ≤ b, then the

area between the curve y = f (x) and the x-axis

from a to b, is the negative of ( ) .b

af x dx

Definite Integral As Area

Area from to ( )b

aa b f x dx

Page 31: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

Consider y = f (x) = 0.5x + 6 on the interval [2,6]

whose graph is given below,

Definite Integral As Area

6

2Find ( )

) by using geometry

) by using the definition

of definite integral

f x dx

a

b

Page 32: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

Definite Integral As Area

6

2( ) Area of

Trapezoid

f x dx

Consider y = f (x) = 0.5x + 6 on the interval [2,6]

whose graph is given below,

Page 33: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

( )b

af x dx Area of R1 – Area of R2 + Area of R3

a b

R1

R2

R3

If f changes sign on the interval a ≤ x ≤ b, then definite integral represents the net area, that is, a difference of areas as indicated below:

Definite Integral as Net Area

Page 34: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

a b

R1

R2

R3

If f changes sign on the interval a ≤ x ≤ b, and we need to find the total area between the graph and the x-axis from a to b, then

Total Area

c d

Total Area Area of R1 + Area of R2 + Area of R3

Area of R1 ( )a

cf x dx

Area of R2 ( )d

cf x dx

Area of R3 ( )d

bf x dx

Page 35: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

Example: Use geometry to compute the integral

5

1

1x dx

Area = 2

5

1

1 8 2 6x dx

Area = 8

Area Using Geometry

( ) 1y f x x

–1

5

Page 36: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

Example: Use an antiderivative to compute the integral

5

1

1x dx

Area Using Antiderivatives

First, we need an antiderivative of ( ) 1y f x x

21( ) 1 . Thus,

2F x x dx x x C

5

1

15 3

2 21 (5) ( 1) 6C Cx dx F F

Page 37: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

Example: Now find the total area bounded by the curve and the x-axis from x –1 to x 5.

Area Using Antiderivatives

( ) 1y f x x

( ) 1y f x x

–11 5

R1

R2

Total Area Area of R1 + Area of R2

Page 38: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

( ) 1y f x x

–11 5

R1

R2

Area of R1

121

11

( ) 22

xf x dx x

Area of R2

525

11

( ) 82

xf x dx x

Total Area 2 + 8 10

Page 39: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

Evaluating the Definite Integral

Example: Calculate5

1

12 1x dx

x

55 2

1 1

12 1 lnx dx x x x

x

2 25 ln 5 5 1 ln1 1

28 ln 5 26.39056

Page 40: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

Substitution for Definite Integrals

1 1/ 22

02 3x x dx

2let 3u x x

then 2

dudx

x

1 41/ 22 1/ 2

0 02 3x x x dx u du

43/ 2

0

2

3u

16

3

Notice limits change

Example: Calculate

Page 41: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

Computing Area Example: Find the area enclosed by the x-axis, the vertical lines x = 0, x = 2 and the graph of

23

02x dx Gives the area since 2x3 is

nonnegative on [0, 2].

22

3 4

00

12

2x dx x 4 41 1

2 02 2

8

Antiderivative

22 .y x

Page 42: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

The Definite Integral As a Total

If r (x) is the rate of change of a quantity Q (in units of Q per unit of x), then the total or accumulated change of the quantity as x changes from a to b is given by

Total change in quantity ( )b

a

Q r x dx

Page 43: Chapter 6 The Integral Sections 6.1, 6.2, and 6.3.

Example: If at time t minutes you are traveling at a rate of v(t) feet per minute, then the total distance traveled in feet from minute 2 to minute 10 is given by

10

2

Total change in distance ( )v t dt

The Definite Integral As a Total


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