lesson 22: areas and distances (handout)

10
Section 5.1 Areas and Distances V63.0121.006/016, Calculus I New York University April 13, 2010 Announcements I Quiz April 16 on §§4.1–4.4 I Final Exam: Monday, May 10, 12:00noon Announcements I Quiz April 16 on §§4.1–4.4 I Final Exam: Monday, May 10, 12:00noon V63.0121.006/016, Calculus I (NYU) Section 5.1 Areas and Distances April 13, 2010 2 / 30 Objectives I Compute the area of a region by approximating it with rectangles and letting the size of the rectangles tend to zero. I Compute the total distance traveled by a particle by approximating it as distance = (rate)(time) and letting the time intervals over which one approximates tend to zero. V63.0121.006/016, Calculus I (NYU) Section 5.1 Areas and Distances April 13, 2010 3 / 30 Notes Notes Notes 1 Section 5.1 : Areas and Distances V63.0121.006/016, Calculus I April 13, 2010

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We trace the computation of area through the centuries. The process known known as Riemann Sums has applications to not just area but many fields of science. (Handout version of slideshow from class)

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Page 1: Lesson 22: Areas and Distances (handout)

Section 5.1Areas and Distances

V63.0121.006/016, Calculus I

New York University

April 13, 2010

Announcements

I Quiz April 16 on §§4.1–4.4

I Final Exam: Monday, May 10, 12:00noon

Announcements

I Quiz April 16 on §§4.1–4.4

I Final Exam: Monday, May10, 12:00noon

V63.0121.006/016, Calculus I (NYU) Section 5.1 Areas and Distances April 13, 2010 2 / 30

Objectives

I Compute the area of aregion by approximating itwith rectangles and lettingthe size of the rectanglestend to zero.

I Compute the total distancetraveled by a particle byapproximating it as distance= (rate)(time) and lettingthe time intervals over whichone approximates tend tozero.

V63.0121.006/016, Calculus I (NYU) Section 5.1 Areas and Distances April 13, 2010 3 / 30

Notes

Notes

Notes

1

Section 5.1 : Areas and DistancesV63.0121.006/016, Calculus I April 13, 2010

Page 2: Lesson 22: Areas and Distances (handout)

Outline

Area through the CenturiesEuclidArchimedesCavalieri

Generalizing Cavalieri’s methodAnalogies

DistancesOther applications

V63.0121.006/016, Calculus I (NYU) Section 5.1 Areas and Distances April 13, 2010 4 / 30

Easy Areas: Rectangle

Definition

The area of a rectangle with dimensions ` and w is the product A = `w .

`

w

It may seem strange that this is a definition and not a theorem but wehave to start somewhere.

V63.0121.006/016, Calculus I (NYU) Section 5.1 Areas and Distances April 13, 2010 5 / 30

Easy Areas: Parallelogram

By cutting and pasting, a parallelogram can be made into a rectangle.

b b

h

So

Fact

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

A = bh

V63.0121.006/016, Calculus I (NYU) Section 5.1 Areas and Distances April 13, 2010 6 / 30

Notes

Notes

Notes

2

Section 5.1 : Areas and DistancesV63.0121.006/016, Calculus I April 13, 2010

Page 3: Lesson 22: Areas and Distances (handout)

Easy Areas: Triangle

By copying and pasting, a triangle can be made into a parallelogram.

b

h

So

Fact

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

A =1

2bh

V63.0121.006/016, Calculus I (NYU) Section 5.1 Areas and Distances April 13, 2010 7 / 30

Easy Areas: Other Polygons

Any polygon can be triangulated, so its area can be found by summing theareas of the triangles:

V63.0121.006/016, Calculus I (NYU) Section 5.1 Areas and Distances April 13, 2010 8 / 30

Hard Areas: Curved Regions

???

V63.0121.006/016, Calculus I (NYU) Section 5.1 Areas and Distances April 13, 2010 9 / 30

Notes

Notes

Notes

3

Section 5.1 : Areas and DistancesV63.0121.006/016, Calculus I April 13, 2010

Page 4: Lesson 22: Areas and Distances (handout)

Meet the mathematician: Archimedes

I Greek (Syracuse), 287 BC –212 BC (after Euclid)

I Geometer

I Weapons engineer

V63.0121.006/016, Calculus I (NYU) Section 5.1 Areas and Distances April 13, 2010 10 / 30

118

18

164

164

164

164

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

A = 1 + 2 · 1

8+ 4 · 1

64+ · · ·

= 1 +1

4+

1

16+ · · ·+ 1

4n+ · · ·

V63.0121.006/016, Calculus I (NYU) Section 5.1 Areas and Distances April 13, 2010 11 / 30

We would then need to know the value of the series

1 +1

4+

1

16+ · · ·+ 1

4n+ · · ·

But for any number r and any positive integer n,

(1− r)(1 + r + · · ·+ rn) = 1− rn+1

So

1 + r + · · ·+ rn =1− rn+1

1− r

Therefore

1 +1

4+

1

16+ · · ·+ 1

4n=

1− (1/4)n+1

1− 1/4→ 1

3/4=

4

3

as n→∞.

V63.0121.006/016, Calculus I (NYU) Section 5.1 Areas and Distances April 13, 2010 12 / 30

Notes

Notes

Notes

4

Section 5.1 : Areas and DistancesV63.0121.006/016, Calculus I April 13, 2010

Page 5: Lesson 22: Areas and Distances (handout)

Cavalieri

I Italian,1598–1647

I Revisited thearea problemwith adifferentperspective

V63.0121.006/016, Calculus I (NYU) Section 5.1 Areas and Distances April 13, 2010 13 / 30

Cavalieri’s method

y = x2

0 1

1

2

Divide up the interval into piecesand measure the area of theinscribed rectangles:

L2 =1

8

L3 =1

27+

4

27=

5

27

L4 =1

64+

4

64+

9

64=

14

64

L5 =1

125+

4

125+

9

125+

16

125=

30

125Ln =?

V63.0121.006/016, Calculus I (NYU) Section 5.1 Areas and Distances April 13, 2010 14 / 30

What is Ln?

Divide the interval [0, 1] into n pieces. Then each has width1

n. The

rectangle over the ith interval and under the parabola has area

1

n·(

i − 1

n

)2

=(i − 1)2

n3.

So

Ln =1

n3+

22

n3+ · · ·+ (n − 1)2

n3=

1 + 22 + 32 + · · ·+ (n − 1)2

n3

The Arabs knew that

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

6

So

Ln =n(n − 1)(2n − 1)

6n3→ 1

3as n→∞.V63.0121.006/016, Calculus I (NYU) Section 5.1 Areas and Distances April 13, 2010 15 / 30

Notes

Notes

Notes

5

Section 5.1 : Areas and DistancesV63.0121.006/016, Calculus I April 13, 2010

Page 6: Lesson 22: Areas and Distances (handout)

Cavalieri’s method for different functions

Try the same trick with f (x) = x3. We have

Ln =1

n· f(

1

n

)+

1

n· f(

2

n

)+ · · ·+ 1

n· f(

n − 1

n

)=

1

n· 1

n3+

1

n· 23

n3+ · · ·+ 1

n· (n − 1)3

n3

=1 + 23 + 33 + · · ·+ (n − 1)3

n4

The formula out of the hat is

1 + 23 + 33 + · · ·+ (n − 1)3 =[12n(n − 1)

]2So

Ln =n2(n − 1)2

4n4→ 1

4as n→∞.

V63.0121.006/016, Calculus I (NYU) Section 5.1 Areas and Distances April 13, 2010 16 / 30

Cavalieri’s method with different heights

Rn =1

n· 13

n3+

1

n· 23

n3+ · · ·+ 1

n· n3

n3

=13 + 23 + 33 + · · ·+ n3

n4

=1

n4

[12n(n + 1)

]2=

n2(n + 1)2

4n4→ 1

4

as n→∞.So even though the rectangles overlap, we still get the same answer.

V63.0121.006/016, Calculus I (NYU) Section 5.1 Areas and Distances April 13, 2010 17 / 30

Outline

Area through the CenturiesEuclidArchimedesCavalieri

Generalizing Cavalieri’s methodAnalogies

DistancesOther applications

V63.0121.006/016, Calculus I (NYU) Section 5.1 Areas and Distances April 13, 2010 18 / 30

Notes

Notes

Notes

6

Section 5.1 : Areas and DistancesV63.0121.006/016, Calculus I April 13, 2010

Page 7: Lesson 22: Areas and Distances (handout)

Cavalieri’s method in general

Let f be a positive function defined on the interval [a, b]. We want to find the areabetween x = a, x = b, y = 0, and y = f (x).

For each positive integer n, divide up the interval into n pieces. Then ∆x =b − a

n.

For each i between 1 and n, let xi be the nth step between a and b. So

a bx0 x1 x2 . . . xixn−1xn

x0 = a

x1 = x0 + ∆x = a +b − a

n

x2 = x1 + ∆x = a + 2 · b − a

n· · · · · ·

xi = a + i · b − a

n· · · · · ·

xn = a + n · b − a

n= b

V63.0121.006/016, Calculus I (NYU) Section 5.1 Areas and Distances April 13, 2010 19 / 30

Forming Riemann sums

We have many choices of how to approximate the area:

Ln = f (x0)∆x + f (x1)∆x + · · ·+ f (xn−1)∆x

Rn = f (x1)∆x + f (x2)∆x + · · ·+ f (xn)∆x

Mn = f

(x0 + x1

2

)∆x + f

(x1 + x2

2

)∆x + · · ·+ f

(xn−1 + xn

2

)∆x

In general, 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

V63.0121.006/016, Calculus I (NYU) Section 5.1 Areas and Distances April 13, 2010 20 / 30

Theorem of the Day

Theorem

If f is a continuous function orhas finitely many jumpdiscontinuities on [a, b], then

limn→∞

Sn = limn→∞

n∑i=1

f (ci )∆x

exists and is the same value nomatter what choice of ci wemade.

x1x1 x2x1 x2 x3x1 x2 x3 x4x1 x2 x3 x4 x5x1 x2 x3 x4 x5 x6x1 x2 x3 x4 x5 x6 x7x1x2x3x4x5x6x7x8x1x2x3x4x5x6x7x8x9x1x2x3x4x5x6x7x8x9x10x1x2x3x4x5x6x7x8x9x10x11x1x2x3x4x5x6x7x8x9x10x11x12x1x2x3x4x5x6x7x8x9x10x11x12x13x1x2x3x4x5x6x7x8x9x10x11x12x13x14x1x2x3x4x5x6x7x8x9x10x11x12x13x14x15x1x2x3x4x5x6x7x8x9x10x11x12x13x14x15x16x1x2x3x4x5x6x7x8x9x10x11x12x13x14x15x16x17x1x2x3x4x5x6x7x8x9x10x11x12x13x14x15x16x17x18x1x2x3x4x5x6x7x8x9x10x11x12x13x14x15x16x17x18x19x1x2x3x4x5x6x7x8x9x10x11x12x13x14x15x16x17x18x19x20a b

V63.0121.006/016, Calculus I (NYU) Section 5.1 Areas and Distances April 13, 2010 21 / 30

Notes

Notes

Notes

7

Section 5.1 : Areas and DistancesV63.0121.006/016, Calculus I April 13, 2010

Page 8: Lesson 22: Areas and Distances (handout)

Analogies

The Tangent Problem(Ch. 2–4)

I Want the slope of a curve

I Only know the slope of lines

I Approximate curve with aline

I Take limit over better andbetter approximations

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 better andbetter approximations

V63.0121.006/016, Calculus I (NYU) Section 5.1 Areas and Distances April 13, 2010 22 / 30

Outline

Area through the CenturiesEuclidArchimedesCavalieri

Generalizing Cavalieri’s methodAnalogies

DistancesOther applications

V63.0121.006/016, Calculus I (NYU) Section 5.1 Areas and Distances April 13, 2010 23 / 30

Distances

Just like area = length× width, we have

distance = rate× time.

So here is another use for Riemann sums.

V63.0121.006/016, Calculus I (NYU) Section 5.1 Areas and Distances April 13, 2010 24 / 30

Notes

Notes

Notes

8

Section 5.1 : Areas and DistancesV63.0121.006/016, Calculus I April 13, 2010

Page 9: Lesson 22: Areas and Distances (handout)

Application: Dead Reckoning

V63.0121.006/016, Calculus I (NYU) Section 5.1 Areas and Distances April 13, 2010 25 / 30

Example

A sailing ship is cruising back and forth along a channel (in a straightline). At noon the ship’s position and velocity are recorded, but shortlythereafter a storm blows in and position is impossible to measure. Thevelocity continues to be recorded at thirty-minute intervals.

Time 12:00 12:30 1:00 1:30 2:00

Speed (knots) 4 8 12 6 4

Direction E E E E W

Time 2:30 3:00 3:30 4:00

Speed 3 3 5 9

Direction W E E E

Estimate the ship’s position at 4:00pm.

V63.0121.006/016, Calculus I (NYU) Section 5.1 Areas and Distances April 13, 2010 26 / 30

Solution

We estimate that the speed of 4 knots (nautical miles per hour) ismaintained from 12:00 until 12:30. So over this time interval the shiptravels (

4 nmi

hr

)(1

2hr

)= 2nmi

We can continue for each additional 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 position.

V63.0121.006/016, Calculus I (NYU) Section 5.1 Areas and Distances April 13, 2010 27 / 30

Notes

Notes

Notes

9

Section 5.1 : Areas and DistancesV63.0121.006/016, Calculus I April 13, 2010

Page 10: Lesson 22: Areas and Distances (handout)

Analysis

I This method of measuring position by recording velocity was necessaryuntil global-positioning satellite technology became widespread

I If we had velocity estimates at finer intervals, we’d get betterestimates.

I If we had velocity at every instant, a limit would tell us our exactposition relative to the last time we measured it.

V63.0121.006/016, Calculus I (NYU) Section 5.1 Areas and Distances April 13, 2010 28 / 30

Other uses of Riemann sums

Anything with a product!

I Area, volume

I Anything with a density: Population, mass

I Anything with a “speed:” distance, throughput, power

I Consumer surplus

I Expected value of a random variable

V63.0121.006/016, Calculus I (NYU) Section 5.1 Areas and Distances April 13, 2010 29 / 30

Summary

I We can compute the area of a curved region with a limit of Riemannsums

I We can compute the distance traveled from the velocity with a limitof Riemann sums

I Many other important uses of this process.

V63.0121.006/016, Calculus I (NYU) Section 5.1 Areas and Distances April 13, 2010 30 / 30

Notes

Notes

Notes

10

Section 5.1 : Areas and DistancesV63.0121.006/016, Calculus I April 13, 2010