riemann sums and the definite integral. time velocity after 4 seconds, the object has gone 12 feet....

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Riemann Sums and The Definite Integral

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If the velocity is not constant, we might guess that the distance traveled is still equal to the area under the curve. Example: We could estimate the area under the curve by drawing rectangles touching at their left corners. This is called the Left- hand Rectangular Approximation Method (LRAM). Approximate area: Estimating with Finite Sums

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Page 1: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

Riemann Sums and The Definite Integral

Page 2: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

time

velocity

After 4 seconds, the object has gone 12 feet.

Consider an object moving at a constant rate of 3 ft/sec.Since rate . time = distance:If we draw a graph of the velocity, the distance that the object travels is equal to the area under the line.

ft3 4 sec 12 ftsec

3t d

Estimating with Finite Sums

Page 3: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

If the velocity is not constant,we might guess that the distance traveled is still equalto the area under the curve.

21 18

V t Example:

We could estimate the area under the curve by drawing rectangles touching at their left corners.

This is called the Left-hand Rectangular Approximation Method (LRAM).

1 118

112

128

t v

10

1 118

2 112

3 128

Approximate area: 1 1 1 31 1 1 2 5 5.758 2 8 4

Estimating with Finite Sums

Page 4: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

We could also use a Right-hand Rectangular Approximation Method(RRAM).

118

112

128

Approximate area: 1 1 1 31 1 2 3 7 7.758 2 8 4

3

21 18

V t

Estimating with Finite Sums

Page 5: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

Another approach would be to userectangles that touch at the midpoint. This is the Midpoint Rectangular Approximation Method (MRAM).

1.031251.28125

1.78125

Approximate area:6.625

2.53125

t v

1.031250.5

1.5 1.28125

2.5 1.78125

3.5 2.53125

In this example there are four subintervals.As the number of subintervals increases, so does the accuracy.

21 18

V t

Estimating with Finite Sums

Page 6: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

21 18

V t

Approximate area:6.65624

t v

1.007810.25

0.75 1.07031

1.25 1.19531

1.382811.75

2.25

2.753.253.75

1.63281

1.945312.320312.75781

13.31248 0.5 6.65624

width of subinterval

With 8 subintervals:

The exact answer for thisproblem is .6.6

Estimating with Finite Sums

Page 7: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

Circumscribed rectangles are all above the curve:

Inscribed rectangles are all below the curve:

Estimating with Finite Sums

Page 8: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

We will be learning how to find the exact area under a curve if we have the equation for the curve. Rectangular approximation methods are still useful for finding the area under a curve if we do not have the equation.

Estimating with Finite Sums

Page 9: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

When we find the area under a curve by adding rectangles, the answer is called a Rieman sum.

21 18

V t

subinterval

partition

The width of a rectangle is called a subinterval.

The entire interval is called the partition.

Subintervals do not all have to be the same size.

Definite Integrals

Page 10: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

21 18

V t

subinterval

partition

If the partition is denoted by P, then the length of the longest subinterval is called the norm of P and is denoted by .P

As gets smaller, the approximation for the area gets better.

P

0 1

Area limn

k kP k

f c x

if P is a partition of the interval ,a b

Definite Integrals

Page 11: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

0 1

limn

k kP k

f c x

is called the definite integral of

over .f ,a b

If we use subintervals of equal length, then the length of a

subinterval is:b ax

n

The definite integral is then given by: 1

limn

kn k

f c x

Definite Integrals

Page 12: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

1

limn

kn k

f c x

Leibnitz introduced a simpler notation for the definite integral:

1

limn b

k an k

f c x f x dx

Note: the very small change in x becomes dx.

Definite Integrals

Page 13: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

b

af x dx

IntegrationSymbol

lower limit of integration

upper limit of integration

integrandvariable of integration

(dummy variable)

It is called a dummy variable because the answer does not depend on the variable chosen.

Definite Integrals

Page 14: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

b

af x dx

We have the notation for integration, but we still need to learn how to evaluate the integral.

Definite Integrals

Page 15: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

Definite IntegralsDefinition -- a Definite IntegralIf y = f(x) is non negative and integrable over a closed interval[a,b], then the DEFINITE INTEGRAL (area under the curve) y = f(x) from a to b is the integral of f(x) from a to b.

b

af x dxA =

Page 16: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

0 1

limn

k kP k

f c x

b

af x dx

F x F a

Area

Where F(x) is the antiderivative of f(x)!

Definite Integrals

Page 17: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

( ) An indefinite integral

is a family of functions

f x dx

( ) A definite integral

is a number

b

a

f x dx

( )f x dx F x C

( ) 7.6b

a

f x dx

Page 18: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

Using integrals to find area works extremely well as long as we can find the antiderivative of the function.

Sometimes, the function is too complicated to find the antiderivative.

At other times, we don’t even have a function, but only measurements taken from a real-life object.

What we need is an efficient method to estimate area when we can not find the antiderivative.

Trapezoid Rule

Page 19: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

Trapezoidal Rule:

0 1 2 12 2 ... 22 n nhT y y y y y

where [a,b] is partitioned into n subintervals ofequal lengthh = (b – a)/n

This gives us a better approximation than either left or right rectangles.

Trapezoid Rule

2nn RRAMLRAMT

lyEquivalent

Page 20: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

1 9 1 9 3 1 3 17 1 171 32 8 2 8 2 2 2 8 2 8

T

1 9 9 3 3 17 171 32 8 8 2 2 8 8

T

1 272 2

T

274

6.75

Trapezoid Rule

Page 21: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

Consider the function f whose graph is shown below. Use theTrapezoid Rule with n = 4 to estimate the value of

9

1f x dx

A. 21 B. 22 C. 23 D. 24 E. 25

1 3 2 1 4 2 5 222

2 B

X

X

X

X

X

Page 22: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

Trapezoidal Rule:

1 altitude sum of bases2 1 2 3 n

1 x y 2 y y ... y2

Error in Trapezoidal Rule:

3b2

2a

2

M b af x dx Trap n

nwhere M is the maximum value of

12 f" x

Midpoint Rule midpt. altitude sum of bases

Error in Midpoint Rule:

3b2

2a

2

M b af x dx Mid n

nwhere M is the maximum value of

24 f" x

Page 23: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

Rules for definite integrals

( ) ( ) a b

b a

f x dx f x dx

( ) 0a

a

f x dx

( ) ( )b b

a a

kf x dx k f x dx

( ( ) ( )) ( ) ( )a a a

b b b

f x g x dx f x dx g x dx

( ( )) ( ) ( ) ,b c b

a a c

f x dx f x dx f x dx a c b

Page 24: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

5. b c c

a b af x dx f x dx f x dx

Intervals can be added(or subtracted.)

a b c

y f x

Definite Integrals and Antiderivatives

Page 25: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

6.

Definite Integrals and Antiderivatives

b

aabfdxxfabf )(max)()(min

a b

Page 26: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

Example

a) (x2 x) 1

4

dx x3

3

x2

2

1

4

43

3

42

2

( 1)3

3

( 1)2

2

643

162

13

12

643

8 13

12

1416

Page 27: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

Example:b) ex dx

0

3

ex 0

3 e3 e0

e3 1

Page 28: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

Example:c) 1 2x

1x

1

e

dx x x2 ln x 1

e

(e e2 lne) (112 ln1) (e e2 1) (11 0) e e2 1 1 1 e e2 3

Page 29: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

Example:

x3 3x 1 dx 1

2

x4

4

32

x2 x

1

2

24

4

32

22 2

1 4

4

32

1 2 1

4 6 2 14

32

1

0 214

214

Page 30: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

Definite Integrals and Antiderivatives

Suppose that f and g are continuous functions and that

4

2

2

2

4

26)(,3)(,5)( dxxhdxxfdxxf

Find

2

4)( dxxf

4

2)( dxxf

2

2)(2 dxxf

3

3)( dxxf

2

4)( dxxf

4

2)](2)(3[ dxxhxf

3 2*5=10 -5 – -3 = -2

-3 + 5 = 2 0 3*(-3)- 2 * 6 = -21

Page 31: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

Example: Northeast Airlines determines that the marginal profit resulting from the sale of x seats on a jet traveling from Atlanta to Kansas City, in hundreds of dollars, is given by

Find the total profit when 60 seats are sold.

P (x) x 6.

Page 32: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

Example (continued): We integrate to find P(60).

P 60 P x dx0

60

x 6 dx

0

60

23

x3 2 6x

0

60

23

603 2 6 60

23

03 2 6 0

50.1613

Page 33: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

The average value of a function is the value that would give the same area if the function was a constant:

212

y x

3 2

0

12

A x dx3

3

0

16

x276

92

4.5

4.5Average Value 1.53

Area 1Average Value Width

b

af x dx

b a

1.5

Definite Integrals and Antiderivatives

Page 34: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

Average Value of a Function Over an Interval

Page 35: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

EXAMPLEEXAMPLE

SOLUTIONSOLUTION

Determine the average value of f (x) = 1 – x over the interval -1 ≤ x ≤ 1.

Using (2) with a = -1 and b = 1, the average value of f (x) = 1 – x over the interval -1 ≤ x ≤ 1 is equal to

.111

1 1

1

dxx

An antiderivative of 1 – x is . Therefore,2

2xx

.123

21

21

211

211

21

2211

21 221

1

21

1

xxdxx

So, the average value of f (x) = 1 – x over the interval -1 ≤ x ≤ 1 is 1.

Page 36: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

Average Value of a FunctionSuppose f is integrable on [a,b]. Then the average value of f over [a,b] is

b

a

dxxfab

)(1

Find the average value of over the interval [0,4] xxf )(

34

6846

1

0461

32

41

041

3

23

40

234

0

xdxx

Page 37: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

For what value(s) in the interval does the function assume the average value?

212

y x

4.5Average Value 1.53

1.5

Definite Integrals and Antiderivatives

5.121 2 x 32 x 3x

Page 38: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

EXAMPLEEXAMPLE

SOLUTIONSOLUTION

(Average Temperature) During a certain 12-hour period the temperature at time

t (measured in hours from the start of the period) was degrees. What was the average temperature during that period?

2

31447 tt

The average temperature during the 12-hour period from t = 0 to t = 12 is 12

0

3212

0

2

9247

121

31447

0121

tttdttt

9002047

9121221247

121 3

23

2

.degrees 550660121

Page 39: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

The mean value theorem for definite integrals says that for a continuous function, at some point on the interval the actual value will equal the average value.

Mean Value Theorem (for definite integrals)

If f is continuous on then at some point c in , ,a b ,a b

1 b

af c f x dx

b a

Definite Integrals and Antiderivatives

Page 40: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

If you were being sent to a desert island and could take only one equation with you,

x

a

d f t dt f xdx

might well be your choice.

Fundamental Theorem of Calculus

Page 41: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

The Fundamental Theorem of Calculus, Part 1

If f is continuous on , then the function ,a b

x

aF x f t dt

has a derivative at every point in , and ,a b

x

a

dF d f t dt f xdx dx

Fundamental Theorem of Calculus

Page 42: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

a

xd f t dtx

f xd

2. Derivative matches upper limit of integration.

First Fundamental Theorem:

1. Derivative of an integral.

Fundamental Theorem of Calculus

Page 43: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

a

xd f t dt f xdx

1. Derivative of an integral.

2. Derivative matches upper limit of integration.

3. Lower limit of integration is a constant.

First Fundamental Theorem:

Fundamental Theorem of Calculus

Page 44: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

x

a

d f t dt f xdx

1. Derivative of an integral.

2. Derivative matches upper limit of integration.

3. Lower limit of integration is a constant.

New variable.

First Fundamental Theorem:

Fundamental Theorem of Calculus

Page 45: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

cos xd t dt

dx cos x1. Derivative of an integral.

2. Derivative matches upper limit of integration.

3. Lower limit of integration is a constant.

sin xd tdx

sin sind xdx

0

sind xdx

The long way: First Fundamental Theorem:

Fundamental Theorem of Calculus

Page 46: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

20

1 1+t

xd dtdx 2

11 x

1. Derivative of an integral.

2. Derivative matches upper limit of integration.

3. Lower limit of integration is a constant.

Fundamental Theorem of Calculus

Page 47: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

2

0cos

xd t dtdx

2 2cos dx xdx

2cos 2x x 22 cosx x

The upper limit of integration does not match the derivative, but we could use the chain rule.

Fundamental Theorem of Calculus

Page 48: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

53 sin

x

d t t dtdx

The lower limit of integration is not a constant, but the upper limit is.

53 sin

xd t t dtdx

3 sinx x

We can change the sign of the integral and reverse the limits.

Fundamental Theorem of Calculus

Page 49: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

2

2

1 2

x

tx

d dtdx e

Neither limit of integration is a constant.

2 0

0 2

1 1 2 2

x

t tx

d dt dtdx e e

It does not matter what constant we use!

2 2

0 0

1 1 2 2

x x

t t

d dt dtdx e e

2 2

1 12 222 xx

xee

(Limits are reversed.)

(Chain rule is used.)

2 2

2 222 xx

xee

We split the integral into two parts.

Fundamental Theorem of Calculus

Page 50: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

The Fundamental Theorem of Calculus, Part 2

If f is continuous at every point of , and if

F is any antiderivative of f on , then

,a b

b

af x dx F b F a

,a b

(Also called the Integral Evaluation Theorem)

Fundamental Theorem of Calculus

Page 51: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

Definite Integral

Substitution

Page 52: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

The substitution rule for definite integrals

If g’ is continuous on [a,b], and f is continuous on the range of u=g(x) then

( )

( )

( ( )) '( ) ( )g bb

a g a

f g x g x dx f u du

Page 53: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

240

tan sec x x dx

Let tanu x2sec du x dx

0 tan 0 0u

tan 14 4

u

1

0 u du

Find new limits

new limit

new limit

12

0

12

u

12

Example

Page 54: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

Example e

1

lnCompute .x dxx

1e 1 2

1 0 0

ln 1Hence .2 2

x tdx tdtx

The substitution ln is suggested bythe function to be integrated. We have

1 0 and e 1.

t x

x t x t

Page 55: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

1 2 3

13 x 1 x dx

3Let 1u x 23 du x dx

1 0u

1 2u

122

0 u du

232

0

23

u Don’t forget to use the new limits.

322 2

3

2 2 23

4 23

Example

Page 56: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

Integrals of Even and Odd Functions

Assume that f is an odd function, i.e., that

f f . Then f 0.a

a

x x x x dx

0

Assume that f is an even function, i.e., that

f f . Then f 2 f .a a

a

x x x x dx x dx

Theorem

Theorem

Page 57: Riemann Sums and The Definite Integral. time velocity After 4 seconds, the object has gone 12 feet. Consider an object moving at a constant rate of 3

Integrals of Even and Odd Functions

Problem 5 7Compute cos .x xdx

Solution5 7

5 7

Observe that the function cos is odd.Since the interval of integration is symmetric with

respect to the origin, cos 0.

x x

x xdx

An odd function is symmetric with respect to the origin. The definite integral from -a to a, in the case of the function shown in this picture, is the area of the blue domain minus the area of the red domain. By symmetry these areas are equal, hence the integral is 0.

-aa