4. Theory of the Integral 4.1 Antidifferentiation 4.2 The Definite - - PowerPoint PPT Presentation

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4. Theory of the Integral 4.1 Antidifferentiation 4.2 The Definite - - PowerPoint PPT Presentation

4. Theory of the Integral 4.1 Antidifferentiation 4.2 The Definite Integral 4.3 Riemann Sums 4.4 The Fundamental Theorem of Calculus 4.5 Fundamental Integration Rules 4.6 U-Substitutions 4.1 Antidifferentiation We will begin our study


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  • 4. Theory of the Integral
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4.1 Antidifferentiation 4.2 The Definite Integral 4.3 Riemann Sums

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4.4 The Fundamental Theorem of Calculus 4.5 Fundamental Integration Rules 4.6 U-Substitutions

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4.1 Antidifferentiation

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  • We will begin our study of the integral

by discussing antidifferentiation.

  • As you might expect, this is the

process of undoing a derivative. Let f(x) be a function. A function F(x) is an antiderivative of f(x) if F 0(x) = f(x).

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Let f(x) = 1. Find an antiderivative of f(x).

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Let f(x) = sin(x). Find an antiderivative of f(x).

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Let f(x) = e2x. Find an antiderivative of f(x).

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  • Notice that I am asking to

find an antiderivative, not the antiderivative.

  • That is because

antiderivatives are not unique!

  • Indeed, if is an

antiderivative for , then is also an antiderivative for any constant . F(x) f(x) F(x) + C C

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4.2 Definite Integral

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  • We will relate the

antiderivative to another important object: the definite integral.

  • This is a quantity that

depends on two endpoint values, , and a function,

  • It is written as

a, b f(x). Z b

a

f(x)dx.

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  • The definite integral has many

important interpretations.

  • The most significant for us is

area under the curve from to

  • It is not obvious how to

compute the area under the curve of a general function— this is the power of calculus!

  • Let’s start with simple things.

f(x) a b.

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Compute Z 2 3dx.

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Compute Z 1

−1

xdx.

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Compute Z 5 2xdx.

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4.3 Riemann Sums

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4.3.1 Riemman Sums Part I 4.3.2 Riemman Sums Part II

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4.3.1 Riemann Sums Part I

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  • We have seen how to

compute definite integrals

  • f functions with certain

simple properties, by exploiting well-known area formulas from geometry.

  • What can we do in general?

Not much yet.

  • We can, however,

approximate the area with Riemann sums.

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  • A Riemann sum

approximates an integral by covering the area beneath the curve with rectangles.

  • The areas of the these

rectangles are more easily computed.

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  • This is because the width of

these rectangles is fixed, and the height is given by the value of the function at a given point.

  • Programmers—try coding

this! It’s a classic.

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Estimate Z 4 x2dx with left and right Riemann sums of width 1.

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4.3.2 Riemann Sums Part II

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Estimate Z 2

−1

(1 − x)dx with left and right Riemann sums of width 1.

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4.4 The Fundamental Theorem of Calculus

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  • The fundamental theorem
  • f calculus is a classic

result.

  • It links the derivative and

the integral.

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  • We will not prove it,

though we will use it extensively to compute areas under curves.

  • Intuitively, definite

integrals can be computed by evaluating an antiderivative at the endpoints of integration.

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Suppose f has antiderivative F(x). Then Z b

a

f(x)dx = F(b) − F(a).

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Compute Z 2 x2dx.

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Compute Z 2π cos(x)dx.

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  • When no particular

endpoints are specified, the FTC suggests that we write

  • Here, is an arbitrary

constant. Z f(x) = F(x) + C C

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Compute Z e3xdx.

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Compute Z 2 xdx.

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  • Another way to interpret the

FTC is as stating that the derivative and integral undo each other.

  • More precisely,
  • This is valid for all likely

to appear on the CLEP exam. d dx Z f(x)dx = f(x) f(x)

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4.5 Basic Integral Rules

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4.5.1 Basic Integral Rules I 4.5.2 Basic Integral Rules II

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4.5.1 Basic Integral Rules I

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  • Using the FTC, we see that

all the basic derivative rules apply, in an inverted way, to integrals.

  • This means that to know

the basic rules for integrals, it suffices to know the basic rules for derivatives.

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For constants a, b, Z (af(x) + bg(x))dx = a Z f(x)dx + b Z g(x)dx

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If n 6= 1, Z xndx = 1 n + 1xn+1 + C If n = −1, Z xndx = ln(x) + C

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Compute Z (x3 + 2x − 3)dx

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Compute Z (x−1 + 1)dx

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Z exdx = ex + C

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Compute Z ✓−4 x + 2ex ◆ dx

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4.5.2 Basic Integral Rules II

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Compute Z (sin(x) + x2)dx

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Z sin(x)dx = − cos(x) + C Z cos(x)dx = sin(x) + C

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Z tan(x)dx = − ln | cos(x)| + C Z sec(x)dx = ln | tan(x) + sec(x)| + C

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Compute Z (tan(θ) − cos(θ))dθ

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Z dx √ 1 − x2 = arcsin(x) + C Z dx 1 + x2 = arctan(x) + C Z dx |x| √ x2 − 1 = sec−1(x) + C

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Compute Z −3dx √ 4 − 4x2

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Compute Z dy 2|y| p y2 − 1

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4.6 U-Substitutions

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  • There are many more

sophisticated types of integration methods.

  • These include those based
  • n the product rule

(integration by parts), special properties of trigonometric functions (trig. substitutions), and those based on tedious algebra (partial fraction decomposition).

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  • We focus on a method

based on the chain rule.

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  • Recall that to compute the

derivative of a composition of functions, we use the chain rule:

  • According to the FTC,
  • Hence,

d dxf(g(x)) = f 0(g(x)) · g0(x). Z f 0(g(x))g0(x)dx = f(g(x)) + C Z d dxf(g(x)) = f(g(x)) + C.

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Compute Z xex2dx

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Compute Z cos(4x + 1)dx

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Compute Z x3p x4 + 1dx

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Compute Z tan(x)dx