lesson 24: areas and distances, the definite integral (slides)

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. . SecƟon 5.1–5.2 Areas and Distances, The Definite Integral V63.0121.011: Calculus I Professor MaƩhew Leingang New York University April 25, 2011

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We can define the area of a curved region by a process similar to that by which we determined the slope of a curve: approximation by what we know and a limit.

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Page 1: Lesson 24: Areas and Distances, The Definite Integral (slides)

..

Sec on 5.1–5.2Areas and Distances, The Definite

Integral

V63.0121.011: Calculus IProfessor Ma hew Leingang

New York University

April 25, 2011

Page 2: Lesson 24: Areas and Distances, The Definite Integral (slides)

Announcements

I Quiz 5 on Sec ons4.1–4.4 April 28/29

I Final Exam Thursday May12, 2:00–3:50pm

I cumula veI loca on TBDI old exams on common

website

Page 3: Lesson 24: Areas and Distances, The Definite Integral (slides)

Objectives from Section 5.1I Compute the area of a region byapproxima ng it with rectanglesand le ng the size of therectangles tend to zero.

I Compute the total distancetraveled by a par cle byapproxima ng it as distance =(rate)( me) and le ng the meintervals over which oneapproximates tend to zero.

Page 4: Lesson 24: Areas and Distances, The Definite Integral (slides)

Objectives from Section 5.2

I Compute the definite integralusing a limit of Riemann sums

I Es mate the definite integralusing a Riemann sum (e.g.,Midpoint Rule)

I Reason with the definite integralusing its elementary proper es.

Page 5: Lesson 24: Areas and Distances, The Definite Integral (slides)

OutlineArea through the Centuries

EuclidArchimedesCavalieri

Generalizing Cavalieri’s methodAnalogies

DistancesOther applica ons

The definite integral as a limitEs ma ng the Definite IntegralProper es of the integralComparison Proper es of the Integral

Page 6: Lesson 24: Areas and Distances, The Definite Integral (slides)

Easy Areas: RectangleDefini onThe area of a rectangle with dimensions ℓ and w is the productA = ℓw.

..ℓ

.

w

It may seem strange that this is a defini on and not a theorem butwe have to start somewhere.

Page 7: Lesson 24: Areas and Distances, The Definite Integral (slides)

Easy Areas: ParallelogramBy cu ng and pas ng, a parallelogram can be made into a rectangle.

..b

.b

.

h

SoFactThe area of a parallelogram of base width b and height h is

A = bh

Page 8: Lesson 24: Areas and Distances, The Definite Integral (slides)

Easy Areas: ParallelogramBy cu ng and pas ng, a parallelogram can be made into a rectangle.

..b

.b

.

h

SoFactThe area of a parallelogram of base width b and height h is

A = bh

Page 9: Lesson 24: Areas and Distances, The Definite Integral (slides)

Easy Areas: ParallelogramBy cu ng and pas ng, a parallelogram can be made into a rectangle.

.

.b

.b

.

h

SoFactThe area of a parallelogram of base width b and height h is

A = bh

Page 10: Lesson 24: Areas and Distances, The Definite Integral (slides)

Easy Areas: ParallelogramBy cu ng and pas ng, a parallelogram can be made into a rectangle.

.

.b

.b

.

h

SoFactThe area of a parallelogram of base width b and height h is

A = bh

Page 11: Lesson 24: Areas and Distances, The Definite Integral (slides)

Easy Areas: ParallelogramBy cu ng and pas ng, a parallelogram can be made into a rectangle.

.

.b

.b

.

h

SoFactThe area of a parallelogram of base width b and height h is

A = bh

Page 12: Lesson 24: Areas and Distances, The Definite Integral (slides)

Easy Areas: TriangleBy copying and pas ng, a triangle can be made into a parallelogram.

..b

.

h

SoFactThe area of a triangle of base width b and height h is

A =12bh

Page 13: Lesson 24: Areas and Distances, The Definite Integral (slides)

Easy Areas: TriangleBy copying and pas ng, a triangle can be made into a parallelogram.

..b

.

h

SoFactThe area of a triangle of base width b and height h is

A =12bh

Page 14: Lesson 24: Areas and Distances, The Definite Integral (slides)

Easy Areas: TriangleBy copying and pas ng, a triangle can be made into a parallelogram.

..b

.

h

SoFactThe area of a triangle of base width b and height h is

A =12bh

Page 15: Lesson 24: Areas and Distances, The Definite Integral (slides)

Easy Areas: Other PolygonsAny polygon can be triangulated, so its area can be found bysumming the areas of the triangles:

.

.

Page 16: Lesson 24: Areas and Distances, The Definite Integral (slides)

Hard Areas: Curved Regions

.

.

???

Page 17: Lesson 24: Areas and Distances, The Definite Integral (slides)

Meet the mathematician: Archimedes

I Greek (Syracuse), 287 BC– 212 BC (a er Euclid)

I GeometerI Weapons engineer

Page 18: Lesson 24: Areas and Distances, The Definite Integral (slides)

Meet the mathematician: Archimedes

I Greek (Syracuse), 287 BC– 212 BC (a er Euclid)

I GeometerI Weapons engineer

Page 19: Lesson 24: Areas and Distances, The Definite Integral (slides)

Meet the mathematician: Archimedes

I Greek (Syracuse), 287 BC– 212 BC (a er Euclid)

I GeometerI Weapons engineer

Page 20: Lesson 24: Areas and Distances, The Definite Integral (slides)

Archimedes and the Parabola

.

Archimedes found areas of a sequence of triangles inscribed in aparabola.

A =

1+ 2 · 18+ 4 · 1

64+ · · · = 1+

14+

116

+ · · ·+ 14n

+ · · ·

Page 21: Lesson 24: Areas and Distances, The Definite Integral (slides)

Archimedes and the Parabola

..

1

Archimedes found areas of a sequence of triangles inscribed in aparabola.

A = 1

+ 2 · 18+ 4 · 1

64+ · · · = 1+

14+

116

+ · · ·+ 14n

+ · · ·

Page 22: Lesson 24: Areas and Distances, The Definite Integral (slides)

Archimedes and the Parabola

..

1

.

18

.

18

Archimedes found areas of a sequence of triangles inscribed in aparabola.

A = 1+ 2 · 18

+ 4 · 164

+ · · · = 1+14+

116

+ · · ·+ 14n

+ · · ·

Page 23: Lesson 24: Areas and Distances, The Definite Integral (slides)

Archimedes and the Parabola

..

1

.

18

.

18

.

164

.

164

.164

.164

Archimedes found areas of a sequence of triangles inscribed in aparabola.

A = 1+ 2 · 18+ 4 · 1

64+ · · ·

= 1+14+

116

+ · · ·+ 14n

+ · · ·

Page 24: Lesson 24: Areas and Distances, The Definite Integral (slides)

Archimedes and the Parabola

..

1

.

18

.

18

.

164

.

164

.164

.164

Archimedes found areas of a sequence of triangles inscribed in aparabola.

A = 1+ 2 · 18+ 4 · 1

64+ · · · = 1+

14+

116

+ · · ·+ 14n

+ · · ·

Page 25: Lesson 24: Areas and Distances, The Definite Integral (slides)

Summing the series

We need to know the value of the series

1+14+

116

+ · · ·+ 14n

+ · · ·

Using the corollary,

1+14+

116

+ · · ·+ 14n

=1− (1/4)n+1

1− 1/4→ 1

3/4=

43as n → ∞.

Page 26: Lesson 24: Areas and Distances, The Definite Integral (slides)

Summing a geometric seriesFactFor any number r and any posi ve integer n,

(1− r)(1+ r+ r2 + · · ·+ rn) = 1− rn+1.

Proof.

(1− r)(1+ r+ r2 + · · ·+ rn)= (1+ r+ r2 + · · ·+ rn)− r(1+ r+ r2 + · · ·+ rn)= (1+ r+ r2 + · · ·+ rn)− (r+ r2 + r3 · · ·+ rn + rn+1)

= 1− rn+1

Page 27: Lesson 24: Areas and Distances, The Definite Integral (slides)

Summing a geometric seriesFactFor any number r and any posi ve integer n,

(1− r)(1+ r+ r2 + · · ·+ rn) = 1− rn+1.

Proof.

(1− r)(1+ r+ r2 + · · ·+ rn)= (1+ r+ r2 + · · ·+ rn)− r(1+ r+ r2 + · · ·+ rn)= (1+ r+ r2 + · · ·+ rn)− (r+ r2 + r3 · · ·+ rn + rn+1)

= 1− rn+1

Page 28: Lesson 24: Areas and Distances, The Definite Integral (slides)

Summing a geometric seriesFactFor any number r and any posi ve integer n,

(1− r)(1+ r+ r2 + · · ·+ rn) = 1− rn+1.

Corollary

1+ r+ · · ·+ rn =1− rn+1

1− r

Page 29: Lesson 24: Areas and Distances, The Definite Integral (slides)

Summing the series

We need to know the value of the series

1+14+

116

+ · · ·+ 14n

+ · · ·

Using the corollary,

1+14+

116

+ · · ·+ 14n

=1− (1/4)n+1

1− 1/4

→ 13/4

=43as n → ∞.

Page 30: Lesson 24: Areas and Distances, The Definite Integral (slides)

Summing the series

We need to know the value of the series

1+14+

116

+ · · ·+ 14n

+ · · ·

Using the corollary,

1+14+

116

+ · · ·+ 14n

=1− (1/4)n+1

1− 1/4→ 1

3/4=

43as n → ∞.

Page 31: Lesson 24: Areas and Distances, The Definite Integral (slides)

Cavalieri

I Italian,1598–1647

I Revisitedthe areaproblemwith adifferentperspec ve

Page 32: Lesson 24: Areas and Distances, The Definite Integral (slides)

Cavalieri’s method

..

y = x2

..0..

1

..12

Divide up the interval into pieces andmeasure the area of the inscribedrectangles:

L2 =18

L3 =

127

+427

=527

L4 =

164

+464

+964

=1464

L5 =

1125

+4

125+

9125

+16125

=30125

Ln =?

Page 33: Lesson 24: Areas and Distances, The Definite Integral (slides)

Cavalieri’s method

..

y = x2

..0..

1..

12

Divide up the interval into pieces andmeasure the area of the inscribedrectangles:

L2 =18

L3 =

127

+427

=527

L4 =

164

+464

+964

=1464

L5 =

1125

+4

125+

9125

+16125

=30125

Ln =?

Page 34: Lesson 24: Areas and Distances, The Definite Integral (slides)

Cavalieri’s method

..

y = x2

..0..

1

..12

..13

..23

Divide up the interval into pieces andmeasure the area of the inscribedrectangles:

L2 =18

L3 =

127

+427

=527

L4 =

164

+464

+964

=1464

L5 =

1125

+4

125+

9125

+16125

=30125

Ln =?

Page 35: Lesson 24: Areas and Distances, The Definite Integral (slides)

Cavalieri’s method

..

y = x2

..0..

1

..12

..13

..23

Divide up the interval into pieces andmeasure the area of the inscribedrectangles:

L2 =18

L3 =127

+427

=527

L4 =

164

+464

+964

=1464

L5 =

1125

+4

125+

9125

+16125

=30125

Ln =?

Page 36: Lesson 24: Areas and Distances, The Definite Integral (slides)

Cavalieri’s method

..

y = x2

..0..

1

..12

..14

..24

..34

Divide up the interval into pieces andmeasure the area of the inscribedrectangles:

L2 =18

L3 =127

+427

=527

L4 =

164

+464

+964

=1464

L5 =

1125

+4

125+

9125

+16125

=30125

Ln =?

Page 37: Lesson 24: Areas and Distances, The Definite Integral (slides)

Cavalieri’s method

..

y = x2

..0..

1

..12

..14

..24

..34

Divide up the interval into pieces andmeasure the area of the inscribedrectangles:

L2 =18

L3 =127

+427

=527

L4 =164

+464

+964

=1464

L5 =

1125

+4

125+

9125

+16125

=30125

Ln =?

Page 38: Lesson 24: Areas and Distances, The Definite Integral (slides)

Cavalieri’s method

..

y = x2

..0..

1

..12

..15

..25

..35

..45

Divide up the interval into pieces andmeasure the area of the inscribedrectangles:

L2 =18

L3 =127

+427

=527

L4 =164

+464

+964

=1464

L5 =

1125

+4

125+

9125

+16125

=30125

Ln =?

Page 39: Lesson 24: Areas and Distances, The Definite Integral (slides)

Cavalieri’s method

..

y = x2

..0..

1

..12

..15

..25

..35

..45

Divide up the interval into pieces andmeasure the area of the inscribedrectangles:

L2 =18

L3 =127

+427

=527

L4 =164

+464

+964

=1464

L5 =1

125+

4125

+9

125+

16125

=30125

Ln =?

Page 40: Lesson 24: Areas and Distances, The Definite Integral (slides)

Cavalieri’s method

..

y = x2

..0..

1

..12

..

Divide up the interval into pieces andmeasure the area of the inscribedrectangles:

L2 =18

L3 =127

+427

=527

L4 =164

+464

+964

=1464

L5 =1

125+

4125

+9

125+

16125

=30125

Ln =?

Page 41: Lesson 24: Areas and Distances, The Definite Integral (slides)

What is Ln?Divide the interval [0, 1] into n pieces. Then each has width

1n.

Therectangle over the ith interval and under the parabola has area

1n·(i− 1n

)2

=(i− 1)2

n3.

So

Ln =1n3

+22

n3+ · · ·+ (n− 1)2

n3=

1+ 22 + 32 + · · ·+ (n− 1)2

n3

SoLn =

n(n− 1)(2n− 1)6n3

→ 13

as n → ∞.

Page 42: Lesson 24: Areas and Distances, The Definite Integral (slides)

What is Ln?Divide the interval [0, 1] into n pieces. Then each has width

1n. The

rectangle over the ith interval and under the parabola has area

1n·(i− 1n

)2

=(i− 1)2

n3.

So

Ln =1n3

+22

n3+ · · ·+ (n− 1)2

n3=

1+ 22 + 32 + · · ·+ (n− 1)2

n3

SoLn =

n(n− 1)(2n− 1)6n3

→ 13

as n → ∞.

Page 43: Lesson 24: Areas and Distances, The Definite Integral (slides)

What is Ln?Divide the interval [0, 1] into n pieces. Then each has width

1n. The

rectangle over the ith interval and under the parabola has area

1n·(i− 1n

)2

=(i− 1)2

n3.

So

Ln =1n3

+22

n3+ · · ·+ (n− 1)2

n3=

1+ 22 + 32 + · · ·+ (n− 1)2

n3

SoLn =

n(n− 1)(2n− 1)6n3

→ 13

as n → ∞.

Page 44: Lesson 24: Areas and Distances, The Definite Integral (slides)

The Square Pyramidial Numbers

FactLet n be a posi ve integer. Then

1+ 22 + 32 + · · ·+ (n− 1)2 =n(n− 1)(2n− 1)

6

This formula was known to the Arabs and discussed by Fibonacci inhis book Liber Abaci.

Page 45: Lesson 24: Areas and Distances, The Definite Integral (slides)

What is Ln?Divide the interval [0, 1] into n pieces. Then each has width

1n. The

rectangle over the ith interval and under the parabola has area

1n·(i− 1n

)2

=(i− 1)2

n3.

So

Ln =1n3

+22

n3+ · · ·+ (n− 1)2

n3=

1+ 22 + 32 + · · ·+ (n− 1)2

n3

SoLn =

n(n− 1)(2n− 1)6n3

→ 13

as n → ∞.

Page 46: Lesson 24: Areas and Distances, The Definite Integral (slides)

What is Ln?Divide the interval [0, 1] into n pieces. Then each has width

1n. The

rectangle over the ith interval and under the parabola has area

1n·(i− 1n

)2

=(i− 1)2

n3.

So

Ln =1n3

+22

n3+ · · ·+ (n− 1)2

n3=

1+ 22 + 32 + · · ·+ (n− 1)2

n3

SoLn =

n(n− 1)(2n− 1)6n3

→ 13

as n → ∞.

Page 47: Lesson 24: Areas and Distances, The Definite Integral (slides)

Cavalieri’s method for different functionsTry the same trick with f(x) = x3. We have

Ln =1n· f(1n

)+

1n· f(2n

)+ · · ·+ 1

n· f(n− 1n

)

=1n· 1n3

+1n· 2

3

n3+ · · ·+ 1

n· (n− 1)3

n3

=1+ 23 + 33 + · · ·+ (n− 1)3

n4

=n2(n− 1)2

4n4→ 1

4as n → ∞.

Page 48: Lesson 24: Areas and Distances, The Definite Integral (slides)

Cavalieri’s method for different functionsTry the same trick with f(x) = x3. We have

Ln =1n· f(1n

)+

1n· f(2n

)+ · · ·+ 1

n· f(n− 1n

)=

1n· 1n3

+1n· 2

3

n3+ · · ·+ 1

n· (n− 1)3

n3

=1+ 23 + 33 + · · ·+ (n− 1)3

n4

=n2(n− 1)2

4n4→ 1

4as n → ∞.

Page 49: Lesson 24: Areas and Distances, The Definite Integral (slides)

Cavalieri’s method for different functionsTry the same trick with f(x) = x3. We have

Ln =1n· f(1n

)+

1n· f(2n

)+ · · ·+ 1

n· f(n− 1n

)=

1n· 1n3

+1n· 2

3

n3+ · · ·+ 1

n· (n− 1)3

n3

=1+ 23 + 33 + · · ·+ (n− 1)3

n4

=n2(n− 1)2

4n4→ 1

4as n → ∞.

Page 50: Lesson 24: Areas and Distances, The Definite Integral (slides)

Nicomachus’s Theorem

Fact (Nicomachus 1st c. CE, Aryabhata 5th c., Al-Karaji 11th c.)

1+ 23 + 33 + · · ·+ (n− 1)3 = [1+ 2+ · · ·+ (n− 1)]2

=[12n(n− 1)

]2

Page 51: Lesson 24: Areas and Distances, The Definite Integral (slides)

Cavalieri’s method for different functionsTry the same trick with f(x) = x3. We have

Ln =1n· f(1n

)+

1n· f(2n

)+ · · ·+ 1

n· f(n− 1n

)=

1n· 1n3

+1n· 2

3

n3+ · · ·+ 1

n· (n− 1)3

n3

=1+ 23 + 33 + · · ·+ (n− 1)3

n4

=n2(n− 1)2

4n4

→ 14

as n → ∞.

Page 52: Lesson 24: Areas and Distances, The Definite Integral (slides)

Cavalieri’s method for different functionsTry the same trick with f(x) = x3. We have

Ln =1n· f(1n

)+

1n· f(2n

)+ · · ·+ 1

n· f(n− 1n

)=

1n· 1n3

+1n· 2

3

n3+ · · ·+ 1

n· (n− 1)3

n3

=1+ 23 + 33 + · · ·+ (n− 1)3

n4

=n2(n− 1)2

4n4→ 1

4as n → ∞.

Page 53: Lesson 24: Areas and Distances, The Definite Integral (slides)

Cavalieri’s method with different heights

.

Rn =1n· 1

3

n3+

1n· 2

3

n3+ · · ·+ 1

n· n

3

n3

=13 + 23 + 33 + · · ·+ n3

n4

=1n4

[12n(n+ 1)

]2=

n2(n+ 1)2

4n4→ 1

4as n → ∞.

So even though the rectangles overlap, we s ll get the same answer.

Page 54: Lesson 24: Areas and Distances, The Definite Integral (slides)

Cavalieri’s method with different heights

.

Rn =1n· 1

3

n3+

1n· 2

3

n3+ · · ·+ 1

n· n

3

n3

=13 + 23 + 33 + · · ·+ n3

n4

=1n4

[12n(n+ 1)

]2=

n2(n+ 1)2

4n4→ 1

4as n → ∞.

So even though the rectangles overlap, we s ll get the same answer.

Page 55: Lesson 24: Areas and Distances, The Definite Integral (slides)

OutlineArea through the Centuries

EuclidArchimedesCavalieri

Generalizing Cavalieri’s methodAnalogies

DistancesOther applica ons

The definite integral as a limitEs ma ng the Definite IntegralProper es of the integralComparison Proper es of the Integral

Page 56: Lesson 24: Areas and Distances, The Definite Integral (slides)

Cavalieri’s method in generalProblem

.. x..x0..x1

..xi

..xn−1

..xn

.. . .

.. . .

Let f be a posi ve func on definedon the interval [a, b]. Find thearea between x = a, x = b, y = 0,and y = f(x).

Page 57: Lesson 24: Areas and Distances, The Definite Integral (slides)

Cavalieri’s method in generalFor each posi ve integer n, divide up the interval into n pieces. Then∆x =

b− an

. For each i between 1 and n, let xi be the ith stepbetween a and b.

.. x..x0..x1

..xi

..xn−1

..xn

.. . .

.. . .

x0 = a

x1 = x0 +∆x = a+b− an

x2 = x1 +∆x = a+ 2 · b− an

. . .

xi = a+ i · b− an

. . .

xn = a+ n · b− an

= b

Page 58: Lesson 24: Areas and Distances, The Definite Integral (slides)

Forming Riemann Sums

Choose ci to be a point in the ith interval [xi−1, xi]. Form theRiemann sum

Sn = f(c1)∆x+ f(c2)∆x+ · · ·+ f(cn)∆x =n∑

i=1

f(ci)∆x

Thus we approximate area under a curve by a sum of areas ofrectangles.

Page 59: Lesson 24: Areas and Distances, The Definite Integral (slides)

Forming Riemann sumsWe have many choices of representa ve points to approximate thearea in each subinterval.

le endpoints…

Ln =n∑

i=1

f(xi−1)∆x

.. x.......

Page 60: Lesson 24: Areas and Distances, The Definite Integral (slides)

Forming Riemann sumsWe have many choices of representa ve points to approximate thearea in each subinterval.

right endpoints…

Rn =n∑

i=1

f(xi)∆x

.. x.......

Page 61: Lesson 24: Areas and Distances, The Definite Integral (slides)

Forming Riemann sumsWe have many choices of representa ve points to approximate thearea in each subinterval.

midpoints…

Mn =n∑

i=1

f(xi−1 + xi

2

)∆x

.. x.......

Page 62: Lesson 24: Areas and Distances, The Definite Integral (slides)

Forming Riemann sumsWe have many choices of representa ve points to approximate thearea in each subinterval.

the maximum value on theinterval…

Un =n∑

i=1

maxxi−1≤x≤xi

{f(x)}∆x

.. x.......

Page 63: Lesson 24: Areas and Distances, The Definite Integral (slides)

Forming Riemann sumsWe have many choices of representa ve points to approximate thearea in each subinterval.

the minimum value on theinterval…

Ln =n∑

i=1

minxi−1≤x≤xi

{f(x)}∆x

.. x.......

Page 64: Lesson 24: Areas and Distances, The Definite Integral (slides)

Forming Riemann sumsWe have many choices of representa ve points to approximate thearea in each subinterval.

…even random points!

.. x.......

Page 65: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.

Page 66: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.

Page 67: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.le endpoints.

L1 = 3.0

Page 68: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.le endpoints.

L2 = 5.25

Page 69: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.le endpoints.

L3 = 6.0

Page 70: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.le endpoints.

L4 = 6.375

Page 71: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.le endpoints.

L5 = 6.59988

Page 72: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.le endpoints.

L6 = 6.75

Page 73: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.le endpoints.

L7 = 6.85692

Page 74: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.le endpoints.

L8 = 6.9375

Page 75: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.le endpoints.

L9 = 6.99985

Page 76: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.le endpoints.

L10 = 7.04958

Page 77: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.le endpoints.

L11 = 7.09064

Page 78: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.le endpoints.

L12 = 7.125

Page 79: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.le endpoints.

L13 = 7.15332

Page 80: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.le endpoints.

L14 = 7.17819

Page 81: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.le endpoints.

L15 = 7.19977

Page 82: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.le endpoints.

L16 = 7.21875

Page 83: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.le endpoints.

L17 = 7.23508

Page 84: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.le endpoints.

L18 = 7.24927

Page 85: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.le endpoints.

L19 = 7.26228

Page 86: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.le endpoints.

L20 = 7.27443

Page 87: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.le endpoints.

L21 = 7.28532

Page 88: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.le endpoints.

L22 = 7.29448

Page 89: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.le endpoints.

L23 = 7.30406

Page 90: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.le endpoints.

L24 = 7.3125

Page 91: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.le endpoints.

L25 = 7.31944

Page 92: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.le endpoints.

L26 = 7.32559

Page 93: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.le endpoints.

L27 = 7.33199

Page 94: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.le endpoints.

L28 = 7.33798

Page 95: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.le endpoints.

L29 = 7.34372

Page 96: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.le endpoints.

L30 = 7.34882

Page 97: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.right endpoints.

R1 = 12.0

Page 98: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.right endpoints.

R2 = 9.75

Page 99: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.right endpoints.

R3 = 9.0

Page 100: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.right endpoints.

R4 = 8.625

Page 101: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.right endpoints.

R5 = 8.39969

Page 102: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.right endpoints.

R6 = 8.25

Page 103: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.right endpoints.

R7 = 8.14236

Page 104: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.right endpoints.

R8 = 8.0625

Page 105: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.right endpoints.

R9 = 7.99974

Page 106: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.right endpoints.

R10 = 7.94933

Page 107: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.right endpoints.

R11 = 7.90868

Page 108: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.right endpoints.

R12 = 7.875

Page 109: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.right endpoints.

R13 = 7.84541

Page 110: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.right endpoints.

R14 = 7.8209

Page 111: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.right endpoints.

R15 = 7.7997

Page 112: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.right endpoints.

R16 = 7.78125

Page 113: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.right endpoints.

R17 = 7.76443

Page 114: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.right endpoints.

R18 = 7.74907

Page 115: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.right endpoints.

R19 = 7.73572

Page 116: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.right endpoints.

R20 = 7.7243

Page 117: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.right endpoints.

R21 = 7.7138

Page 118: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.right endpoints.

R22 = 7.70335

Page 119: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.right endpoints.

R23 = 7.69531

Page 120: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.right endpoints.

R24 = 7.6875

Page 121: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.right endpoints.

R25 = 7.67934

Page 122: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.right endpoints.

R26 = 7.6715

Page 123: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.right endpoints.

R27 = 7.66508

Page 124: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.right endpoints.

R28 = 7.6592

Page 125: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.right endpoints.

R29 = 7.65388

Page 126: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.right endpoints.

R30 = 7.64864

Page 127: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.midpoints

.

M1 = 7.5

Page 128: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.midpoints

.

M2 = 7.5

Page 129: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.midpoints

.

M3 = 7.5

Page 130: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.midpoints

.

M4 = 7.5

Page 131: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.midpoints

.

M5 = 7.4998

Page 132: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.midpoints

.

M6 = 7.5

Page 133: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.midpoints

.

M7 = 7.4996

Page 134: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.midpoints

.

M8 = 7.5

Page 135: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.midpoints

.

M9 = 7.49977

Page 136: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.midpoints

.

M10 = 7.49947

Page 137: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.midpoints

.

M11 = 7.49966

Page 138: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.midpoints

.

M12 = 7.5

Page 139: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.midpoints

.

M13 = 7.49937

Page 140: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.midpoints

.

M14 = 7.49954

Page 141: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.midpoints

.

M15 = 7.49968

Page 142: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.midpoints

.

M16 = 7.49988

Page 143: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.midpoints

.

M17 = 7.49974

Page 144: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.midpoints

.

M18 = 7.49916

Page 145: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.midpoints

.

M19 = 7.49898

Page 146: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.midpoints

.

M20 = 7.4994

Page 147: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.midpoints

.

M21 = 7.49951

Page 148: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.midpoints

.

M22 = 7.49889

Page 149: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.midpoints

.

M23 = 7.49962

Page 150: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.midpoints

.

M24 = 7.5

Page 151: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.midpoints

.

M25 = 7.49939

Page 152: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.midpoints

.

M26 = 7.49847

Page 153: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.midpoints

.

M27 = 7.4985

Page 154: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.midpoints

.

M28 = 7.4986

Page 155: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.midpoints

.

M29 = 7.49878

Page 156: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.midpoints

.

M30 = 7.49872

Page 157: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.maximum points.

U1 = 12.0

Page 158: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.maximum points.

U2 = 10.55685

Page 159: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.maximum points.

U3 = 10.0379

Page 160: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.maximum points.

U4 = 9.41515

Page 161: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.maximum points.

U5 = 8.96004

Page 162: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.maximum points.

U6 = 8.76895

Page 163: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.maximum points.

U7 = 8.6033

Page 164: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.maximum points.

U8 = 8.45757

Page 165: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.maximum points.

U9 = 8.34564

Page 166: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.maximum points.

U10 = 8.27084

Page 167: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.maximum points.

U11 = 8.20132

Page 168: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.maximum points.

U12 = 8.13838

Page 169: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.maximum points.

U13 = 8.0916

Page 170: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.maximum points.

U14 = 8.05139

Page 171: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.maximum points.

U15 = 8.01364

Page 172: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.maximum points.

U16 = 7.98056

Page 173: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.maximum points.

U17 = 7.9539

Page 174: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.maximum points.

U18 = 7.92815

Page 175: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.maximum points.

U19 = 7.90414

Page 176: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.maximum points.

U20 = 7.88504

Page 177: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.maximum points.

U21 = 7.86737

Page 178: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.maximum points.

U22 = 7.84958

Page 179: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.maximum points.

U23 = 7.83463

Page 180: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.maximum points.

U24 = 7.82187

Page 181: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.maximum points.

U25 = 7.80824

Page 182: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.maximum points.

U26 = 7.79504

Page 183: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.maximum points.

U27 = 7.78429

Page 184: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.maximum points.

U28 = 7.77443

Page 185: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.maximum points.

U29 = 7.76495

Page 186: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.maximum points.

U30 = 7.7558

Page 187: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.minimum points.

L1 = 3.0

Page 188: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.minimum points.

L2 = 4.44312

Page 189: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.minimum points.

L3 = 4.96208

Page 190: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.minimum points.

L4 = 5.58484

Page 191: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.minimum points.

L5 = 6.0395

Page 192: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.minimum points.

L6 = 6.23103

Page 193: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.minimum points.

L7 = 6.39577

Page 194: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.minimum points.

L8 = 6.54242

Page 195: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.minimum points.

L9 = 6.65381

Page 196: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.minimum points.

L10 = 6.72797

Page 197: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.minimum points.

L11 = 6.7979

Page 198: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.minimum points.

L12 = 6.8616

Page 199: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.minimum points.

L13 = 6.90704

Page 200: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.minimum points.

L14 = 6.94762

Page 201: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.minimum points.

L15 = 6.98575

Page 202: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.minimum points.

L16 = 7.01942

Page 203: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.minimum points.

L17 = 7.04536

Page 204: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.minimum points.

L18 = 7.07005

Page 205: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.minimum points.

L19 = 7.09364

Page 206: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.minimum points.

L20 = 7.1136

Page 207: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.minimum points.

L21 = 7.13155

Page 208: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.minimum points.

L22 = 7.14804

Page 209: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.minimum points.

L23 = 7.16441

Page 210: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.minimum points.

L24 = 7.17812

Page 211: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.minimum points.

L25 = 7.19025

Page 212: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.minimum points.

L26 = 7.2019

Page 213: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.minimum points.

L27 = 7.21265

Page 214: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.minimum points.

L28 = 7.22269

Page 215: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.minimum points.

L29 = 7.23251

Page 216: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.minimum points.

L30 = 7.24162

Page 217: Lesson 24: Areas and Distances, The Definite Integral (slides)

AnalogiesThe Tangent Problem(Ch. 2–4)

I Want the slope of a curveI Only know the slope oflines

I Approximate curve with aline

I Take limit over be er andbe er approxima ons

The Area Problem (Ch. 5)

I Want the area of a curvedregion

I Only know the area ofpolygons

I Approximate region withpolygons

I Take limit over be er andbe er approxima ons

Page 218: Lesson 24: Areas and Distances, The Definite Integral (slides)

AnalogiesThe Tangent Problem(Ch. 2–4)

I Want the slope of a curve

I Only know the slope oflines

I Approximate curve with aline

I Take limit over be er andbe er approxima ons

The Area Problem (Ch. 5)

I Want the area of a curvedregion

I Only know the area ofpolygons

I Approximate region withpolygons

I Take limit over be er andbe er approxima ons

Page 219: Lesson 24: Areas and Distances, The Definite Integral (slides)

AnalogiesThe Tangent Problem(Ch. 2–4)

I Want the slope of a curve

I Only know the slope oflines

I Approximate curve with aline

I Take limit over be er andbe er approxima ons

The Area Problem (Ch. 5)I Want the area of a curvedregion

I Only know the area ofpolygons

I Approximate region withpolygons

I Take limit over be er andbe er approxima ons

Page 220: Lesson 24: Areas and Distances, The Definite Integral (slides)

AnalogiesThe Tangent Problem(Ch. 2–4)

I Want the slope of a curveI Only know the slope oflines

I Approximate curve with aline

I Take limit over be er andbe er approxima ons

The Area Problem (Ch. 5)I Want the area of a curvedregion

I Only know the area ofpolygons

I Approximate region withpolygons

I Take limit over be er andbe er approxima ons

Page 221: Lesson 24: Areas and Distances, The Definite Integral (slides)

AnalogiesThe Tangent Problem(Ch. 2–4)

I Want the slope of a curveI Only know the slope oflines

I Approximate curve with aline

I Take limit over be er andbe er approxima ons

The Area Problem (Ch. 5)I Want the area of a curvedregion

I Only know the area ofpolygons

I Approximate region withpolygons

I Take limit over be er andbe er approxima ons

Page 222: Lesson 24: Areas and Distances, The Definite Integral (slides)

AnalogiesThe Tangent Problem(Ch. 2–4)

I Want the slope of a curveI Only know the slope oflines

I Approximate curve with aline

I Take limit over be er andbe er approxima ons

The Area Problem (Ch. 5)I Want the area of a curvedregion

I Only know the area ofpolygons

I Approximate region withpolygons

I Take limit over be er andbe er approxima ons

Page 223: Lesson 24: Areas and Distances, The Definite Integral (slides)

AnalogiesThe Tangent Problem(Ch. 2–4)

I Want the slope of a curveI Only know the slope oflines

I Approximate curve with aline

I Take limit over be er andbe er approxima ons

The Area Problem (Ch. 5)I Want the area of a curvedregion

I Only know the area ofpolygons

I Approximate region withpolygons

I Take limit over be er andbe er approxima ons

Page 224: Lesson 24: Areas and Distances, The Definite Integral (slides)

AnalogiesThe Tangent Problem(Ch. 2–4)

I Want the slope of a curveI Only know the slope oflines

I Approximate curve with aline

I Take limit over be er andbe er approxima ons

The Area Problem (Ch. 5)I Want the area of a curvedregion

I Only know the area ofpolygons

I Approximate region withpolygons

I Take limit over be er andbe er approxima ons

Page 225: Lesson 24: Areas and Distances, The Definite Integral (slides)

OutlineArea through the Centuries

EuclidArchimedesCavalieri

Generalizing Cavalieri’s methodAnalogies

DistancesOther applica ons

The definite integral as a limitEs ma ng the Definite IntegralProper es of the integralComparison Proper es of the Integral

Page 226: Lesson 24: Areas and Distances, The Definite Integral (slides)

Distances

Just like area = length× width, we have

distance = rate× me.

So here is another use for Riemann sums.

Page 227: Lesson 24: Areas and Distances, The Definite Integral (slides)

Application: Dead Reckoning

Page 228: Lesson 24: Areas and Distances, The Definite Integral (slides)

Computing position by Dead ReckoningExampleA sailing ship is cruising back and forth along a channel (in a straightline). At noon the ship’s posi on and velocity are recorded, butshortly therea er a storm blows in and posi on is impossible tomeasure. The velocity con nues to be recorded at thirty-minuteintervals.

Page 229: Lesson 24: Areas and Distances, The Definite Integral (slides)

Computing position by Dead ReckoningExample

Time 12:00 12:30 1:00 1:30 2:00Speed (knots) 4 8 12 6 4Direc on E E E E WTime 2:30 3:00 3:30 4:00Speed 3 3 5 9Direc on W E E E

Es mate the ship’s posi on at 4:00pm.

Page 230: Lesson 24: Areas and Distances, The Definite Integral (slides)

SolutionSolu onWe es mate that the speed of 4 knots (nau cal miles per hour) ismaintained from 12:00 un l 12:30. So over this me interval theship travels (

4 nmihr

)(12hr)

= 2 nmi

We can con nue for each addi onal half hour and get

distance = 4× 1/2 + 8× 1/2 + 12× 1/2

+ 6× 1/2 − 4× 1/2 − 3× 1/2 + 3× 1/2 + 5× 1/2 = 15.5

So the ship is 15.5 nmi east of its original posi on.

Page 231: Lesson 24: Areas and Distances, The Definite Integral (slides)

Analysis

I This method of measuring posi on by recording velocity wasnecessary un l global-posi oning satellite technology becamewidespread

I If we had velocity es mates at finer intervals, we’d get be eres mates.

I If we had velocity at every instant, a limit would tell us ourexact posi on rela ve to the last me we measured it.

Page 232: Lesson 24: Areas and Distances, The Definite Integral (slides)

Other uses of Riemann sums

Anything with a product!I Area, volumeI Anything with a density: Popula on, massI Anything with a “speed:” distance, throughput, powerI Consumer surplusI Expected value of a random variable

Page 233: Lesson 24: Areas and Distances, The Definite Integral (slides)

OutlineArea through the Centuries

EuclidArchimedesCavalieri

Generalizing Cavalieri’s methodAnalogies

DistancesOther applica ons

The definite integral as a limitEs ma ng the Definite IntegralProper es of the integralComparison Proper es of the Integral

Page 234: Lesson 24: Areas and Distances, The Definite Integral (slides)

The definite integral as a limit

Defini onIf f is a func on defined on [a, b], the definite integral of f from a tob is the number ∫ b

af(x) dx = lim

∆x→0

n∑i=1

f(ci)∆x

Page 235: Lesson 24: Areas and Distances, The Definite Integral (slides)

Notation/Terminology∫ b

af(x) dx = lim

∆x→0

n∑i=1

f(ci)∆x

I

∫— integral sign (swoopy S)

I f(x)— integrandI a and b— limits of integra on (a is the lower limit and b theupper limit)

I dx— ??? (a parenthesis? an infinitesimal? a variable?)I The process of compu ng an integral is called integra on orquadrature

Page 236: Lesson 24: Areas and Distances, The Definite Integral (slides)

Notation/Terminology∫ b

af(x) dx = lim

∆x→0

n∑i=1

f(ci)∆x

I

∫— integral sign (swoopy S)

I f(x)— integrandI a and b— limits of integra on (a is the lower limit and b theupper limit)

I dx— ??? (a parenthesis? an infinitesimal? a variable?)I The process of compu ng an integral is called integra on orquadrature

Page 237: Lesson 24: Areas and Distances, The Definite Integral (slides)

Notation/Terminology∫ b

af(x) dx = lim

∆x→0

n∑i=1

f(ci)∆x

I

∫— integral sign (swoopy S)

I f(x)— integrand

I a and b— limits of integra on (a is the lower limit and b theupper limit)

I dx— ??? (a parenthesis? an infinitesimal? a variable?)I The process of compu ng an integral is called integra on orquadrature

Page 238: Lesson 24: Areas and Distances, The Definite Integral (slides)

Notation/Terminology∫ b

af(x) dx = lim

∆x→0

n∑i=1

f(ci)∆x

I

∫— integral sign (swoopy S)

I f(x)— integrandI a and b— limits of integra on (a is the lower limit and b theupper limit)

I dx— ??? (a parenthesis? an infinitesimal? a variable?)I The process of compu ng an integral is called integra on orquadrature

Page 239: Lesson 24: Areas and Distances, The Definite Integral (slides)

Notation/Terminology∫ b

af(x) dx = lim

∆x→0

n∑i=1

f(ci)∆x

I

∫— integral sign (swoopy S)

I f(x)— integrandI a and b— limits of integra on (a is the lower limit and b theupper limit)

I dx— ??? (a parenthesis? an infinitesimal? a variable?)

I The process of compu ng an integral is called integra on orquadrature

Page 240: Lesson 24: Areas and Distances, The Definite Integral (slides)

Notation/Terminology∫ b

af(x) dx = lim

∆x→0

n∑i=1

f(ci)∆x

I

∫— integral sign (swoopy S)

I f(x)— integrandI a and b— limits of integra on (a is the lower limit and b theupper limit)

I dx— ??? (a parenthesis? an infinitesimal? a variable?)I The process of compu ng an integral is called integra on orquadrature

Page 241: Lesson 24: Areas and Distances, The Definite Integral (slides)

The limit can be simplified

TheoremIf f is con nuous on [a, b] or if f has only finitely many jumpdiscon nui es, then f is integrable on [a, b]; that is, the definite

integral∫ b

af(x) dx exists.

So we can find the integral by compu ng the limit of any sequenceof Riemann sums that we like,

Page 242: Lesson 24: Areas and Distances, The Definite Integral (slides)

The limit can be simplified

TheoremIf f is con nuous on [a, b] or if f has only finitely many jumpdiscon nui es, then f is integrable on [a, b]; that is, the definite

integral∫ b

af(x) dx exists.

So we can find the integral by compu ng the limit of any sequenceof Riemann sums that we like,

Page 243: Lesson 24: Areas and Distances, The Definite Integral (slides)

Example

Find∫ 3

0x dx

Solu on

For any n we have∆x =3nand for each i between 0 and n, xi =

3in.

For each i, take xi to represent the func on on the ith interval. So∫ 3

0x dx = lim

n→∞Rn = lim

n→∞

n∑i=1

f(xi)∆x = limn→∞

n∑i=1

(3in

) (3n

)= lim

n→∞

9n2

n∑i=1

i = limn→∞

9n2

· n(n+ 1)2

=92· 1

Page 244: Lesson 24: Areas and Distances, The Definite Integral (slides)

Example

Find∫ 3

0x dx

Solu on

For any n we have∆x =3nand for each i between 0 and n, xi =

3in.

For each i, take xi to represent the func on on the ith interval. So∫ 3

0x dx = lim

n→∞Rn = lim

n→∞

n∑i=1

f(xi)∆x = limn→∞

n∑i=1

(3in

) (3n

)= lim

n→∞

9n2

n∑i=1

i = limn→∞

9n2

· n(n+ 1)2

=92· 1

Page 245: Lesson 24: Areas and Distances, The Definite Integral (slides)

Example

Find∫ 3

0x dx

Solu on

For any n we have∆x =3nand for each i between 0 and n, xi =

3in.

For each i, take xi to represent the func on on the ith interval.

So∫ 3

0x dx = lim

n→∞Rn = lim

n→∞

n∑i=1

f(xi)∆x = limn→∞

n∑i=1

(3in

) (3n

)= lim

n→∞

9n2

n∑i=1

i = limn→∞

9n2

· n(n+ 1)2

=92· 1

Page 246: Lesson 24: Areas and Distances, The Definite Integral (slides)

Example

Find∫ 3

0x dx

Solu on

For any n we have∆x =3nand for each i between 0 and n, xi =

3in.

For each i, take xi to represent the func on on the ith interval. So∫ 3

0x dx = lim

n→∞Rn

= limn→∞

n∑i=1

f(xi)∆x = limn→∞

n∑i=1

(3in

) (3n

)= lim

n→∞

9n2

n∑i=1

i = limn→∞

9n2

· n(n+ 1)2

=92· 1

Page 247: Lesson 24: Areas and Distances, The Definite Integral (slides)

Example

Find∫ 3

0x dx

Solu on

For any n we have∆x =3nand for each i between 0 and n, xi =

3in.

For each i, take xi to represent the func on on the ith interval. So∫ 3

0x dx = lim

n→∞Rn = lim

n→∞

n∑i=1

f(xi)∆x

= limn→∞

n∑i=1

(3in

) (3n

)= lim

n→∞

9n2

n∑i=1

i = limn→∞

9n2

· n(n+ 1)2

=92· 1

Page 248: Lesson 24: Areas and Distances, The Definite Integral (slides)

Example

Find∫ 3

0x dx

Solu on

For any n we have∆x =3nand for each i between 0 and n, xi =

3in.

For each i, take xi to represent the func on on the ith interval. So∫ 3

0x dx = lim

n→∞Rn = lim

n→∞

n∑i=1

f(xi)∆x = limn→∞

n∑i=1

(3in

) (3n

)

= limn→∞

9n2

n∑i=1

i = limn→∞

9n2

· n(n+ 1)2

=92· 1

Page 249: Lesson 24: Areas and Distances, The Definite Integral (slides)

Example

Find∫ 3

0x dx

Solu on

For any n we have∆x =3nand for each i between 0 and n, xi =

3in.

For each i, take xi to represent the func on on the ith interval. So∫ 3

0x dx = lim

n→∞Rn = lim

n→∞

n∑i=1

f(xi)∆x = limn→∞

n∑i=1

(3in

) (3n

)

= limn→∞

9n2

n∑i=1

i = limn→∞

9n2

· n(n+ 1)2

=92· 1

Page 250: Lesson 24: Areas and Distances, The Definite Integral (slides)

Example

Find∫ 3

0x dx

Solu on

For any n we have∆x =3nand for each i between 0 and n, xi =

3in.

For each i, take xi to represent the func on on the ith interval. So∫ 3

0x dx = lim

n→∞Rn = lim

n→∞

n∑i=1

f(xi)∆x = limn→∞

n∑i=1

(3in

) (3n

)= lim

n→∞

9n2

n∑i=1

i

= limn→∞

9n2

· n(n+ 1)2

=92· 1

Page 251: Lesson 24: Areas and Distances, The Definite Integral (slides)

Example

Find∫ 3

0x dx

Solu on

For any n we have∆x =3nand for each i between 0 and n, xi =

3in.

For each i, take xi to represent the func on on the ith interval. So∫ 3

0x dx = lim

n→∞Rn = lim

n→∞

n∑i=1

f(xi)∆x = limn→∞

n∑i=1

(3in

) (3n

)= lim

n→∞

9n2

n∑i=1

i = limn→∞

9n2

· n(n+ 1)2

=92· 1

Page 252: Lesson 24: Areas and Distances, The Definite Integral (slides)

Example

Find∫ 3

0x dx

Solu on

For any n we have∆x =3nand for each i between 0 and n, xi =

3in.

For each i, take xi to represent the func on on the ith interval. So∫ 3

0x dx = lim

n→∞Rn = lim

n→∞

n∑i=1

f(xi)∆x = limn→∞

n∑i=1

(3in

) (3n

)= lim

n→∞

9n2

n∑i=1

i = limn→∞

9n2

· n(n+ 1)2

=92· 1

Page 253: Lesson 24: Areas and Distances, The Definite Integral (slides)

Example

Find∫ 3

0x2 dx

Solu on

For any n and i we have∆x =3nand xi =

3in. So∫ 3

0x2 dx = lim

n→∞Rn = lim

n→∞

n∑i=1

f(xi)∆x = limn→∞

n∑i=1

(3in

)2(3n

)= lim

n→∞

27n3

n∑i=1

i2 = limn→∞

27n3

· n(n+ 1)(2n+ 1)6

=273

= 9

Page 254: Lesson 24: Areas and Distances, The Definite Integral (slides)

Example

Find∫ 3

0x2 dx

Solu on

For any n and i we have∆x =3nand xi =

3in. So∫ 3

0x2 dx = lim

n→∞Rn = lim

n→∞

n∑i=1

f(xi)∆x = limn→∞

n∑i=1

(3in

)2(3n

)= lim

n→∞

27n3

n∑i=1

i2 = limn→∞

27n3

· n(n+ 1)(2n+ 1)6

=273

= 9

Page 255: Lesson 24: Areas and Distances, The Definite Integral (slides)

Example

Find∫ 3

0x2 dx

Solu on

For any n and i we have∆x =3nand xi =

3in.

So∫ 3

0x2 dx = lim

n→∞Rn = lim

n→∞

n∑i=1

f(xi)∆x = limn→∞

n∑i=1

(3in

)2(3n

)= lim

n→∞

27n3

n∑i=1

i2 = limn→∞

27n3

· n(n+ 1)(2n+ 1)6

=273

= 9

Page 256: Lesson 24: Areas and Distances, The Definite Integral (slides)

Example

Find∫ 3

0x2 dx

Solu on

For any n and i we have∆x =3nand xi =

3in. So∫ 3

0x2 dx = lim

n→∞Rn

= limn→∞

n∑i=1

f(xi)∆x = limn→∞

n∑i=1

(3in

)2(3n

)= lim

n→∞

27n3

n∑i=1

i2 = limn→∞

27n3

· n(n+ 1)(2n+ 1)6

=273

= 9

Page 257: Lesson 24: Areas and Distances, The Definite Integral (slides)

Example

Find∫ 3

0x2 dx

Solu on

For any n and i we have∆x =3nand xi =

3in. So∫ 3

0x2 dx = lim

n→∞Rn = lim

n→∞

n∑i=1

f(xi)∆x

= limn→∞

n∑i=1

(3in

)2(3n

)= lim

n→∞

27n3

n∑i=1

i2 = limn→∞

27n3

· n(n+ 1)(2n+ 1)6

=273

= 9

Page 258: Lesson 24: Areas and Distances, The Definite Integral (slides)

Example

Find∫ 3

0x2 dx

Solu on

For any n and i we have∆x =3nand xi =

3in. So∫ 3

0x2 dx = lim

n→∞Rn = lim

n→∞

n∑i=1

f(xi)∆x = limn→∞

n∑i=1

(3in

)2(3n

)

= limn→∞

27n3

n∑i=1

i2 = limn→∞

27n3

· n(n+ 1)(2n+ 1)6

=273

= 9

Page 259: Lesson 24: Areas and Distances, The Definite Integral (slides)

Example

Find∫ 3

0x2 dx

Solu on

For any n and i we have∆x =3nand xi =

3in. So∫ 3

0x2 dx = lim

n→∞Rn = lim

n→∞

n∑i=1

f(xi)∆x = limn→∞

n∑i=1

(3in

)2(3n

)

= limn→∞

27n3

n∑i=1

i2 = limn→∞

27n3

· n(n+ 1)(2n+ 1)6

=273

= 9

Page 260: Lesson 24: Areas and Distances, The Definite Integral (slides)

Example

Find∫ 3

0x2 dx

Solu on

For any n and i we have∆x =3nand xi =

3in. So∫ 3

0x2 dx = lim

n→∞Rn = lim

n→∞

n∑i=1

f(xi)∆x = limn→∞

n∑i=1

(3in

)2(3n

)

= limn→∞

27n3

n∑i=1

i2 = limn→∞

27n3

· n(n+ 1)(2n+ 1)6

=273

= 9

Page 261: Lesson 24: Areas and Distances, The Definite Integral (slides)

Example

Find∫ 3

0x2 dx

Solu on

For any n and i we have∆x =3nand xi =

3in. So∫ 3

0x2 dx = lim

n→∞Rn = lim

n→∞

n∑i=1

f(xi)∆x = limn→∞

n∑i=1

(3in

)2(3n

)= lim

n→∞

27n3

n∑i=1

i2

= limn→∞

27n3

· n(n+ 1)(2n+ 1)6

=273

= 9

Page 262: Lesson 24: Areas and Distances, The Definite Integral (slides)

Example

Find∫ 3

0x2 dx

Solu on

For any n and i we have∆x =3nand xi =

3in. So∫ 3

0x2 dx = lim

n→∞Rn = lim

n→∞

n∑i=1

f(xi)∆x = limn→∞

n∑i=1

(3in

)2(3n

)= lim

n→∞

27n3

n∑i=1

i2 = limn→∞

27n3

· n(n+ 1)(2n+ 1)6

=273

= 9

Page 263: Lesson 24: Areas and Distances, The Definite Integral (slides)

Example

Find∫ 3

0x2 dx

Solu on

For any n and i we have∆x =3nand xi =

3in. So∫ 3

0x2 dx = lim

n→∞Rn = lim

n→∞

n∑i=1

f(xi)∆x = limn→∞

n∑i=1

(3in

)2(3n

)= lim

n→∞

27n3

n∑i=1

i2 = limn→∞

27n3

· n(n+ 1)(2n+ 1)6

=273

= 9

Page 264: Lesson 24: Areas and Distances, The Definite Integral (slides)

Example

Find∫ 3

0x3 dx

Solu on

For any n we have∆x =3nand xi =

3in. So

Rn =n∑

i=1

f(xi)∆x =n∑

i=1

(3in

)3(3n

)=

81n4

n∑i=1

i3

=81n4

· n2(n+ 1)2

4−→ 81

4

So∫ 3

0x3 dx =

814

= 20.25

Page 265: Lesson 24: Areas and Distances, The Definite Integral (slides)

Example

Find∫ 3

0x3 dx

Solu on

For any n we have∆x =3nand xi =

3in. So

Rn =n∑

i=1

f(xi)∆x =n∑

i=1

(3in

)3(3n

)=

81n4

n∑i=1

i3

=81n4

· n2(n+ 1)2

4−→ 81

4

So∫ 3

0x3 dx =

814

= 20.25

Page 266: Lesson 24: Areas and Distances, The Definite Integral (slides)

OutlineArea through the Centuries

EuclidArchimedesCavalieri

Generalizing Cavalieri’s methodAnalogies

DistancesOther applica ons

The definite integral as a limitEs ma ng the Definite IntegralProper es of the integralComparison Proper es of the Integral

Page 267: Lesson 24: Areas and Distances, The Definite Integral (slides)

Estimating the Definite IntegralExample

Es mate∫ 1

0

41+ x2

dx usingM4.

Solu on

Page 268: Lesson 24: Areas and Distances, The Definite Integral (slides)

Estimating the Definite IntegralExample

Es mate∫ 1

0

41+ x2

dx usingM4.

Solu on

We have x0 = 0, x1 =14, x2 =

12, x3 =

34, x4 = 1.

So c1 =18, c2 =

38, c3 =

58, c4 =

78.

Page 269: Lesson 24: Areas and Distances, The Definite Integral (slides)

Estimating the Definite IntegralExample

Es mate∫ 1

0

41+ x2

dx usingM4.

Solu on

M4 =14

(4

1+ (1/8)2+

41+ (3/8)2

+4

1+ (5/8)2+

41+ (7/8)2

)

=14

(4

65/64+

473/64

+4

89/64+

4113/64

)=

6465

+6473

+6489

+64113

≈ 3.1468

Page 270: Lesson 24: Areas and Distances, The Definite Integral (slides)

Estimating the Definite IntegralExample

Es mate∫ 1

0

41+ x2

dx usingM4.

Solu on

M4 =14

(4

1+ (1/8)2+

41+ (3/8)2

+4

1+ (5/8)2+

41+ (7/8)2

)=

14

(4

65/64+

473/64

+4

89/64+

4113/64

)

=6465

+6473

+6489

+64113

≈ 3.1468

Page 271: Lesson 24: Areas and Distances, The Definite Integral (slides)

Estimating the Definite IntegralExample

Es mate∫ 1

0

41+ x2

dx usingM4.

Solu on

M4 =14

(4

1+ (1/8)2+

41+ (3/8)2

+4

1+ (5/8)2+

41+ (7/8)2

)=

14

(4

65/64+

473/64

+4

89/64+

4113/64

)=

6465

+6473

+6489

+64113

≈ 3.1468

Page 272: Lesson 24: Areas and Distances, The Definite Integral (slides)

Estimating the Definite IntegralExample

Es mate∫ 1

0

41+ x2

dx using L4 and R4

Answer

Page 273: Lesson 24: Areas and Distances, The Definite Integral (slides)

Estimating the Definite IntegralExample

Es mate∫ 1

0

41+ x2

dx using L4 and R4

Answer

L4 =14

(4

1+ (0)2+

41+ (1/4)2

+4

1+ (1/2)2+

41+ (3/4)2

)= 1+

1617

+45+

1625

≈ 3.38118

Page 274: Lesson 24: Areas and Distances, The Definite Integral (slides)

Estimating the Definite IntegralExample

Es mate∫ 1

0

41+ x2

dx using L4 and R4

Answer

R4 =14

(4

1+ (1/4)2+

41+ (1/2)2

+4

1+ (3/4)2+

41+ (1)2

)=

1617

+45+

1625

+12≈ 2.88118

Page 275: Lesson 24: Areas and Distances, The Definite Integral (slides)

OutlineArea through the Centuries

EuclidArchimedesCavalieri

Generalizing Cavalieri’s methodAnalogies

DistancesOther applica ons

The definite integral as a limitEs ma ng the Definite IntegralProper es of the integralComparison Proper es of the Integral

Page 276: Lesson 24: Areas and Distances, The Definite Integral (slides)

Properties of the integralTheorem (Addi ve Proper es of the Integral)

Let f and g be integrable func ons on [a, b] and c a constant. Then

1.∫ b

ac dx = c(b− a)

2.∫ b

a[f(x) + g(x)] dx =

∫ b

af(x) dx+

∫ b

ag(x) dx.

3.∫ b

acf(x) dx = c

∫ b

af(x) dx.

4.∫ b

a[f(x)− g(x)] dx =

∫ b

af(x) dx−

∫ b

ag(x) dx.

Page 277: Lesson 24: Areas and Distances, The Definite Integral (slides)

Properties of the integralTheorem (Addi ve Proper es of the Integral)

Let f and g be integrable func ons on [a, b] and c a constant. Then

1.∫ b

ac dx = c(b− a)

2.∫ b

a[f(x) + g(x)] dx =

∫ b

af(x) dx+

∫ b

ag(x) dx.

3.∫ b

acf(x) dx = c

∫ b

af(x) dx.

4.∫ b

a[f(x)− g(x)] dx =

∫ b

af(x) dx−

∫ b

ag(x) dx.

Page 278: Lesson 24: Areas and Distances, The Definite Integral (slides)

Properties of the integralTheorem (Addi ve Proper es of the Integral)

Let f and g be integrable func ons on [a, b] and c a constant. Then

1.∫ b

ac dx = c(b− a)

2.∫ b

a[f(x) + g(x)] dx =

∫ b

af(x) dx+

∫ b

ag(x) dx.

3.∫ b

acf(x) dx = c

∫ b

af(x) dx.

4.∫ b

a[f(x)− g(x)] dx =

∫ b

af(x) dx−

∫ b

ag(x) dx.

Page 279: Lesson 24: Areas and Distances, The Definite Integral (slides)

Properties of the integralTheorem (Addi ve Proper es of the Integral)

Let f and g be integrable func ons on [a, b] and c a constant. Then

1.∫ b

ac dx = c(b− a)

2.∫ b

a[f(x) + g(x)] dx =

∫ b

af(x) dx+

∫ b

ag(x) dx.

3.∫ b

acf(x) dx = c

∫ b

af(x) dx.

4.∫ b

a[f(x)− g(x)] dx =

∫ b

af(x) dx−

∫ b

ag(x) dx.

Page 280: Lesson 24: Areas and Distances, The Definite Integral (slides)

ProofsProofs.

I When integra ng a constant func on c, each Riemann sumequals c(b− a).

I A Riemann sum for f+ g equals a Riemann sum for f plus aRiemann sum for g. Using the sum rule for limits, the integralof a sum is the sum of the integrals.

I Di o for constant mul plesI Di o for differences

Page 281: Lesson 24: Areas and Distances, The Definite Integral (slides)

Example

Find∫ 3

0

(x3 − 4.5x2 + 5.5x+ 1

)dx

Solu on∫ 3

0(x3−4.5x2 + 5.5x+ 1) dx

=

∫ 3

0x3 dx− 4.5

∫ 3

0x2 dx+ 5.5

∫ 3

0x dx+

∫ 3

01 dx

= 20.25− 4.5 · 9+ 5.5 · 4.5+ 3 · 1 = 7.5

(This is the func on we were es ma ng the integral of before)

Page 282: Lesson 24: Areas and Distances, The Definite Integral (slides)

Example

Find∫ 3

0

(x3 − 4.5x2 + 5.5x+ 1

)dx

Solu on∫ 3

0(x3−4.5x2 + 5.5x+ 1) dx

=

∫ 3

0x3 dx− 4.5

∫ 3

0x2 dx+ 5.5

∫ 3

0x dx+

∫ 3

01 dx

= 20.25− 4.5 · 9+ 5.5 · 4.5+ 3 · 1 = 7.5

(This is the func on we were es ma ng the integral of before)

Page 283: Lesson 24: Areas and Distances, The Definite Integral (slides)

Example

Find∫ 3

0

(x3 − 4.5x2 + 5.5x+ 1

)dx

Solu on∫ 3

0(x3−4.5x2 + 5.5x+ 1) dx

=

∫ 3

0x3 dx− 4.5

∫ 3

0x2 dx+ 5.5

∫ 3

0x dx+

∫ 3

01 dx

= 20.25− 4.5 · 9+ 5.5 · 4.5+ 3 · 1 = 7.5

(This is the func on we were es ma ng the integral of before)

Page 284: Lesson 24: Areas and Distances, The Definite Integral (slides)

Theorem of the DayTheoremIf f is a con nuous func on on[a, b] or has finitely many jumpdiscon nui es, then

limn→∞

Sn = limn→∞

{n∑

i=1

f(ci)∆x

}

exists and is the same value noma er what choice of ci we make.

.... x.midpoints

.

M15 = 7.49968

Page 285: Lesson 24: Areas and Distances, The Definite Integral (slides)

More Properties of the IntegralConven ons: ∫ a

bf(x) dx = −

∫ b

af(x) dx∫ a

af(x) dx = 0

This allows us to haveTheorem

5.∫ c

af(x) dx =

∫ b

af(x) dx+

∫ c

bf(x) dx for all a, b, and c.

Page 286: Lesson 24: Areas and Distances, The Definite Integral (slides)

Illustrating Property 5Theorem

5.∫ c

af(x) dx =

∫ b

af(x) dx+

∫ c

bf(x) dx for all a, b, and c.

..x

.

y

..a

..b

..c

Page 287: Lesson 24: Areas and Distances, The Definite Integral (slides)

Illustrating Property 5Theorem

5.∫ c

af(x) dx =

∫ b

af(x) dx+

∫ c

bf(x) dx for all a, b, and c.

..x

.

y

..a

..b

..c

.

∫ b

af(x) dx

Page 288: Lesson 24: Areas and Distances, The Definite Integral (slides)

Illustrating Property 5Theorem

5.∫ c

af(x) dx =

∫ b

af(x) dx+

∫ c

bf(x) dx for all a, b, and c.

..x

.

y

..a

..b

..c

.

∫ b

af(x) dx

.

∫ c

bf(x) dx

Page 289: Lesson 24: Areas and Distances, The Definite Integral (slides)

Illustrating Property 5Theorem

5.∫ c

af(x) dx =

∫ b

af(x) dx+

∫ c

bf(x) dx for all a, b, and c.

..x

.

y

..a

..b

..c

.

∫ b

af(x) dx

.

∫ c

bf(x) dx

.

∫ c

af(x) dx

Page 290: Lesson 24: Areas and Distances, The Definite Integral (slides)

Illustrating Property 5Theorem

5.∫ c

af(x) dx =

∫ b

af(x) dx+

∫ c

bf(x) dx for all a, b, and c.

..x

.

y

..a..

b..

c

Page 291: Lesson 24: Areas and Distances, The Definite Integral (slides)

Illustrating Property 5Theorem

5.∫ c

af(x) dx =

∫ b

af(x) dx+

∫ c

bf(x) dx for all a, b, and c.

..x

.

y

..a..

b..

c.

∫ b

af(x) dx

Page 292: Lesson 24: Areas and Distances, The Definite Integral (slides)

Illustrating Property 5Theorem

5.∫ c

af(x) dx =

∫ b

af(x) dx+

∫ c

bf(x) dx for all a, b, and c.

..x

.

y

..a..

b..

c.

∫ c

bf(x) dx =

−∫ b

cf(x) dx

Page 293: Lesson 24: Areas and Distances, The Definite Integral (slides)

Illustrating Property 5Theorem

5.∫ c

af(x) dx =

∫ b

af(x) dx+

∫ c

bf(x) dx for all a, b, and c.

..x

.

y

..a..

b..

c.

∫ c

bf(x) dx =

−∫ b

cf(x) dx

.

∫ c

af(x) dx

Page 294: Lesson 24: Areas and Distances, The Definite Integral (slides)

Using the PropertiesExampleSuppose f and g are func onswith

I

∫ 4

0f(x) dx = 4

I

∫ 5

0f(x) dx = 7

I

∫ 5

0g(x) dx = 3.

Find

(a)∫ 5

0[2f(x)− g(x)] dx

(b)∫ 5

4f(x) dx.

Page 295: Lesson 24: Areas and Distances, The Definite Integral (slides)

Solu onWe have

(a)

∫ 5

0[2f(x)− g(x)] dx = 2

∫ 5

0f(x) dx−

∫ 5

0g(x) dx

= 2 · 7− 3 = 11

(b)

∫ 5

4f(x) dx =

∫ 5

0f(x) dx−

∫ 4

0f(x) dx

= 7− 4 = 3

Page 296: Lesson 24: Areas and Distances, The Definite Integral (slides)

Solu onWe have

(a)

∫ 5

0[2f(x)− g(x)] dx = 2

∫ 5

0f(x) dx−

∫ 5

0g(x) dx

= 2 · 7− 3 = 11

(b)

∫ 5

4f(x) dx =

∫ 5

0f(x) dx−

∫ 4

0f(x) dx

= 7− 4 = 3

Page 297: Lesson 24: Areas and Distances, The Definite Integral (slides)

OutlineArea through the Centuries

EuclidArchimedesCavalieri

Generalizing Cavalieri’s methodAnalogies

DistancesOther applica ons

The definite integral as a limitEs ma ng the Definite IntegralProper es of the integralComparison Proper es of the Integral

Page 298: Lesson 24: Areas and Distances, The Definite Integral (slides)

Comparison Properties of the IntegralTheoremLet f and g be integrable func ons on [a, b].

6. If f(x) ≥ 0 for all x in [a, b], then∫ b

af(x) dx ≥ 0

7. If f(x) ≥ g(x) for all x in [a, b], then∫ b

af(x) dx ≥

∫ b

ag(x) dx

8. If m ≤ f(x) ≤ M for all x in [a, b], then

m(b− a) ≤∫ b

af(x) dx ≤ M(b− a)

Page 299: Lesson 24: Areas and Distances, The Definite Integral (slides)

Comparison Properties of the IntegralTheoremLet f and g be integrable func ons on [a, b].

6. If f(x) ≥ 0 for all x in [a, b], then∫ b

af(x) dx ≥ 0

7. If f(x) ≥ g(x) for all x in [a, b], then∫ b

af(x) dx ≥

∫ b

ag(x) dx

8. If m ≤ f(x) ≤ M for all x in [a, b], then

m(b− a) ≤∫ b

af(x) dx ≤ M(b− a)

Page 300: Lesson 24: Areas and Distances, The Definite Integral (slides)

Comparison Properties of the IntegralTheoremLet f and g be integrable func ons on [a, b].

6. If f(x) ≥ 0 for all x in [a, b], then∫ b

af(x) dx ≥ 0

7. If f(x) ≥ g(x) for all x in [a, b], then∫ b

af(x) dx ≥

∫ b

ag(x) dx

8. If m ≤ f(x) ≤ M for all x in [a, b], then

m(b− a) ≤∫ b

af(x) dx ≤ M(b− a)

Page 301: Lesson 24: Areas and Distances, The Definite Integral (slides)

Comparison Properties of the IntegralTheoremLet f and g be integrable func ons on [a, b].

6. If f(x) ≥ 0 for all x in [a, b], then∫ b

af(x) dx ≥ 0

7. If f(x) ≥ g(x) for all x in [a, b], then∫ b

af(x) dx ≥

∫ b

ag(x) dx

8. If m ≤ f(x) ≤ M for all x in [a, b], then

m(b− a) ≤∫ b

af(x) dx ≤ M(b− a)

Page 302: Lesson 24: Areas and Distances, The Definite Integral (slides)

Integral of a nonnegative function is nonnegativeProof.If f(x) ≥ 0 for all x in [a, b], then forany number of divisions n and choiceof sample points {ci}:

Sn =n∑

i=1

f(ci)︸︷︷︸≥0

∆x ≥n∑

i=1

0 ·∆x = 0

.. x.......Since Sn ≥ 0 for all n, the limit of {Sn} is nonnega ve, too:∫ b

af(x) dx = lim

n→∞Sn︸︷︷︸≥0

≥ 0

Page 303: Lesson 24: Areas and Distances, The Definite Integral (slides)

The integral is “increasing”Proof.Let h(x) = f(x)− g(x). If f(x) ≥ g(x)for all x in [a, b], then h(x) ≥ 0 for allx in [a, b]. So by the previousproperty ∫ b

ah(x) dx ≥ 0 .. x.

f(x)

.

g(x)

.

h(x)

This means that∫ b

af(x) dx−

∫ b

ag(x) dx =

∫ b

a(f(x)− g(x)) dx =

∫ b

ah(x) dx ≥ 0

Page 304: Lesson 24: Areas and Distances, The Definite Integral (slides)

Bounding the integralProof.Ifm ≤ f(x) ≤ M on for all x in [a, b], then bythe previous property∫ b

amdx ≤

∫ b

af(x) dx ≤

∫ b

aMdx

By Property 8, the integral of a constantfunc on is the product of the constant andthe width of the interval. So:

m(b− a) ≤∫ b

af(x) dx ≤ M(b− a)

.. x.

y

.

M

.

f(x)

.

m

..a

..b

Page 305: Lesson 24: Areas and Distances, The Definite Integral (slides)

Example

Es mate∫ 2

1

1xdx using the comparison proper es.

Solu onSince

12≤ x ≤ 1

1for all x in [1, 2], we have

12· 1 ≤

∫ 2

1

1xdx ≤ 1 · 1

Page 306: Lesson 24: Areas and Distances, The Definite Integral (slides)

Example

Es mate∫ 2

1

1xdx using the comparison proper es.

Solu onSince

12≤ x ≤ 1

1for all x in [1, 2], we have

12· 1 ≤

∫ 2

1

1xdx ≤ 1 · 1

Page 307: Lesson 24: Areas and Distances, The Definite Integral (slides)

Summary

I We can compute the area of a curved region with a limit ofRiemann sums

I We can compute the distance traveled from the velocity with alimit of Riemann sums

I Many other important uses of this process.

Page 308: Lesson 24: Areas and Distances, The Definite Integral (slides)

Summary

I The definite integral is a limit of Riemann SumsI The definite integral can be es mated with Riemann SumsI The definite integral can be distributed across sums andconstant mul ples of func ons

I The definite integral can be bounded using bounds for thefunc on