INTEGRALS 5. 5.3 The Fundamental Theorem of Calculus INTEGRALS In this section, we will learn about: The Fundamental Theorem of Calculus and its significance.

Slides:



Advertisements
Similar presentations
The Fundamental Theorem of Calculus Some books have the First and Second Fundamental Theorem of Calculus switched. They are switched in this PowerPoint,
Advertisements

TECHNIQUES OF INTEGRATION
3 DERIVATIVES.
INFINITE SEQUENCES AND SERIES
APPLICATIONS OF DIFFERENTIATION Maximum and Minimum Values In this section, we will learn: How to find the maximum and minimum values of a function.
MULTIPLE INTEGRALS MULTIPLE INTEGRALS Recall that it is usually difficult to evaluate single integrals directly from the definition of an integral.
INTEGRALS Areas and Distances INTEGRALS In this section, we will learn that: We get the same special type of limit in trying to find the area under.
APPLICATIONS OF DIFFERENTIATION
INTEGRALS 5. INTEGRALS We saw in Section 5.1 that a limit of the form arises when we compute an area.  We also saw that it arises when we try to find.
APPLICATIONS OF DIFFERENTIATION The Mean Value Theorem APPLICATIONS OF DIFFERENTIATION In this section, we will learn about: The significance of.
FURTHER APPLICATIONS OF INTEGRATION 9. In chapter 6, we looked at some applications of integrals:  Areas  Volumes  Work  Average values.
Chapter 5: INTEGRAL CALCULUS In Chapter 2 we used the tangent and velocity problems to introduce the derivative, which is the central idea in differential.
Copyright © Cengage Learning. All rights reserved. 3 Differentiation Rules.
Copyright © Cengage Learning. All rights reserved. 5 Integrals.
APPLICATIONS OF DIFFERENTIATION 4. In Sections 2.2 and 2.4, we investigated infinite limits and vertical asymptotes.  There, we let x approach a number.
5.5 The Substitution Rule In this section, we will learn: To substitute a new variable in place of an existing expression in a function, making integration.
Example We can also evaluate a definite integral by interpretation of definite integral. Ex. Find by interpretation of definite integral. Sol. By the interpretation.
5.3 The Fundamental Theorem of Calculus INTEGRALS In this section, we will learn about: The Fundamental Theorem of Calculus and its significance.
INTEGRALS The Fundamental Theorem of Calculus INTEGRALS In this section, we will learn about: The Fundamental Theorem of Calculus and its significance.
LIMITS AND DERIVATIVES
The importance of sequences and infinite series in calculus stems from Newton’s idea of representing functions as sums of infinite series.  For instance,
INTEGRALS Areas and Distances INTEGRALS In this section, we will learn that: We get the same special type of limit in trying to find the area under.
LIMITS AND DERIVATIVES 2. In Sections 2.2 and 2.4, we investigated infinite limits and vertical asymptotes.  There, we let x approach a number.  The.
APPLICATIONS OF DIFFERENTIATION 4. A polynomial behaves near infinity as its term of highest degree. The polynomial behaves like the polynomial Near infinity.
Integrals 5. The Fundamental Theorem of Calculus 5.4.
3 DERIVATIVES. In this section, we will learn about: Differentiating composite functions using the Chain Rule. DERIVATIVES 3.5 The Chain Rule.
Integration 4 Copyright © Cengage Learning. All rights reserved.
INTEGRALS The Fundamental Theorem of Calculus INTEGRALS In this section, we will learn about: The Fundamental Theorem of Calculus and its significance.
INTEGRALS 5. Suumary 1. Definite Integral 2.FTC1,If, then g’(x) = f(x). 3. FTC2,, where F is any antiderivative of f, that is, F’ = f.
Copyright © Cengage Learning. All rights reserved. 4 Integrals.
Section 5.4a FUNDAMENTAL THEOREM OF CALCULUS. Deriving the Theorem Let Apply the definition of the derivative: Rule for Integrals!
DIFFERENTIATION RULES
INTEGRALS 5. INTEGRALS In Chapter 2, we used the tangent and velocity problems to introduce the derivative—the central idea in differential calculus.
Integrals  In Chapter 2, we used the tangent and velocity problems to introduce the derivative—the central idea in differential calculus.  In much the.
Copyright © Cengage Learning. All rights reserved. 4 Integrals.
Chapter 5 Integrals 机动 目录 上页 下页 返回 结束 5.2 Area 5.3 The Definite Integral 5.4 The Fundamental Theorem of Calculus 5.5 The Substitution Rule.
Integration Copyright © Cengage Learning. All rights reserved.
INTEGRALS 5. The Fundamental Theorem of Calculus INTEGRALS In this section, we will learn about: The Fundamental Theorem of Calculus and its significance.
3. Fundamental Theorem of Calculus. Fundamental Theorem of Calculus We’ve learned two different branches of calculus so far: differentiation and integration.
In section 11.9, we were able to find power series representations for a certain restricted class of functions. Here, we investigate more general problems.
INTEGRALS The Substitution Rule In this section, we will learn: To substitute a new variable in place of an existing expression in a function,
Applications of Differentiation Section 4.2 The Mean Value Theorem
APPLICATIONS OF DIFFERENTIATION 4. We will see that many of the results of this chapter depend on one central fact—the Mean Value Theorem.
TECHNIQUES OF INTEGRATION Due to the Fundamental Theorem of Calculus (FTC), we can integrate a function if we know an antiderivative, that is, an indefinite.
Copyright © Cengage Learning. All rights reserved.
APPLICATIONS OF DIFFERENTIATION 4. We will see that many of the results of this chapter depend on one central fact—the Mean Value Theorem.
3 DIFFERENTIATION RULES. We have:  Seen how to interpret derivatives as slopes and rates of change  Seen how to estimate derivatives of functions given.
8 TECHNIQUES OF INTEGRATION. Due to the Fundamental Theorem of Calculus (FTC), we can integrate a function if we know an antiderivative, that is, an indefinite.
DOUBLE INTEGRALS OVER RECTANGLES
Applications of Differentiation Section 4.9 Antiderivatives
In Chapters 6 and 8, we will see how to use the integral to solve problems concerning:  Volumes  Lengths of curves  Population predictions  Cardiac.
INTEGRALS We saw in Section 5.1 that a limit of the form arises when we compute an area. We also saw that it arises when we try to find the distance traveled.
5 INTEGRALS.
The Fundamental Theorem of Calculus is appropriately named because it establishes connection between the two branches of calculus: differential calculus.
APPLICATIONS OF DIFFERENTIATION 4. EXTREME VALUE THEOREM If f is continuous on a closed interval [a, b], then f attains an absolute maximum value f(c)
INTEGRALS 5. INTEGRALS In Chapter 3, we used the tangent and velocity problems to introduce the derivative—the central idea in differential calculus.
Copyright © Cengage Learning. All rights reserved.
5.3 The Fundamental Theorem of Calculus
MATH 318: MATHEMATICAL ANALYSIS II Chapter 7: INTEGRAL CALCULUS
Copyright © Cengage Learning. All rights reserved.
Chapter 5: INTEGRAL CALCULUS
Chapter 5: INTEGRAL CALCULUS
5 INTEGRALS.
Copyright © Cengage Learning. All rights reserved.
The Fundamental Theorem of Calculus
Copyright © Cengage Learning. All rights reserved.
Copyright © Cengage Learning. All rights reserved.
APPLICATIONS OF DIFFERENTIATION
Presentation transcript:

INTEGRALS 5

5.3 The Fundamental Theorem of Calculus INTEGRALS In this section, we will learn about: The Fundamental Theorem of Calculus and its significance.

The Fundamental Theorem of Calculus (FTC) is appropriately named.  It establishes a connection between the two branches of calculus—differential calculus and integral calculus. FUNDAMENTAL THEOREM OF CALCULUS

FTC Differential calculus arose from the tangent problem. Integral calculus arose from a seemingly unrelated problem—the area problem.

Newton’s mentor at Cambridge, Isaac Barrow (1630–1677), discovered that these two problems are actually closely related.  In fact, he realized that differentiation and integration are inverse processes. FTC

The FTC gives the precise inverse relationship between the derivative and the integral. FTC

It was Newton and Leibniz who exploited this relationship and used it to develop calculus into a systematic mathematical method.  In particular, they saw that the FTC enabled them to compute areas and integrals very easily without having to compute them as limits of sums—as we did in Sections 5.1 and 5.2 FTC

The first part of the FTC deals with functions defined by an equation of the form where f is a continuous function on [a, b] and x varies between a and b. Equation 1 FTC

 Observe that g depends only on x, which appears as the variable upper limit in the integral.  If x is a fixed number, then the integral is a definite number.  If we then let x vary, the number also varies and defines a function of x denoted by g(x). FTC

If f happens to be a positive function, then g(x) can be interpreted as the area under the graph of f from a to x, where x can vary from a to b.  Think of g as the ‘area so far’ function, as seen here. FTC Figure 5.3.1, p. 314

If f is the function whose graph is shown and, find the values of: g(0), g(1), g(2), g(3), g(4), and g(5).  Then, sketch a rough graph of g. Example 1 FTC Figure 5.3.2, p. 314

First, we notice that: FTC Example 1

From the figure, we see that g(1) is the area of a triangle: Example 1 FTC Figure 5.3.3a, p. 314

To find g(2), we add to g(1) the area of a rectangle: Example 1 FTC Figure 5.3.3b, p. 314

We estimate that the area under f from 2 to 3 is about 1.3. So, Example 1 FTC Figure 5.3.3c, p. 314

Thus, FTC Example 1 Figure 5.3.3d, p. 314Figure 5.3.3e, p. 314

We use these values to sketch the graph of g.  Notice that, because f(t) is positive for t < 3, we keep adding area for t < 3.  So, g is increasing up to x = 3, where it attains a maximum value.  For x > 3, g decreases because f(t) is negative. Example 1 FTC Figure 5.3.4, p. 314

If we take f(t) = t and a = 0, then, using Exercise 27 in Section 5.2, we have: FTC

Notice that g’(x) = x, that is, g’ = f.  In other words, if g is defined as the integral of f by Equation 1, g turns out to be an antiderivative of f—at least in this case. FTC

If we sketch the derivative of the function g, as in the first figure, by estimating slopes of tangents, we get a graph like that of f in the second figure.  So, we suspect that g’ = f in Example 1 too. FTC Figure 5.3.4, p. 314 Figure 5.3.2, p. 314

To see why this might be generally true, we consider a continuous function f with f(x) ≥ 0.  Then, can be interpreted as the area under the graph of f from a to x. FTC Figure 5.3.1, p. 314

To compute g’(x) from the definition of derivative, we first observe that, for h > 0, g(x + h) – g(x) is obtained by subtracting areas.  It is the area under the graph of f from x to x + h (the gold area). FTC Figure 5.3.5, p. 315

For small h, you can see that this area is approximately equal to the area of the rectangle with height f(x) and width h: So, FTC Figure 5.3.5, p. 315

Intuitively, we therefore expect that:  The fact that this is true, even when f is not necessarily positive, is the first part of the FTC (FTC1). FTC

FTC1 If f is continuous on [a, b], then the function g defined by is continuous on [a, b] and differentiable on (a, b), and g’(x) = f(x).

If x and x + h are in (a, b), then Proof FTC1

So, for h ≠ 0, Proof—Equation 2 FTC1

For now, let us assume that h > 0.  Since f is continuous on [x, x + h], the Extreme Value Theorem says that there are numbers u and v in [x, x + h] such that f(u) = m and f(v) = M.  m and M are the absolute minimum and maximum values of f on [x, x + h]. Proof FTC1 Figure 5.3.6, p. 316

By Property 8 of integrals, we have: That is, Proof FTC1

Since h > 0, we can divide this inequality by h: FTC1 Proof

Now, we use Equation 2 to replace the middle part of this inequality:  Inequality 3 can be proved in a similar manner for the case h < 0. Proof—Equation 3 FTC1

Now, we let h → 0. Then, u → x and v → x, since u and v lie between x and x + h.  Therefore, and because f is continuous at x. Proof FTC1

From Equation 3 and the Squeeze Theorem, we conclude that: Proof—Equation 4 FTC1

Using Leibniz notation for derivatives, we can write the FTC1 as when f is continuous.  Roughly speaking, Equation 5 says that, if we first integrate f and then differentiate the result, we get back to the original function f. Equation 5 FTC1

Find the derivative of the function  As is continuous, the FTC1 gives: Example 2 FTC1

FRESNEL FUNCTION For instance, consider the Fresnel function  It is named after the French physicist Augustin Fresnel (1788–1827), famous for his works in optics.  It first appeared in Fresnel’s theory of the diffraction of light waves.  More recently, it has been applied to the design of highways. Example 3

FRESNEL FUNCTION The FTC1 tells us how to differentiate the Fresnel function: S’(x) = sin(πx 2 /2)  This means that we can apply all the methods of differential calculus to analyze S. Example 3

The figure shows the graphs of f(x) = sin(πx 2 /2) and the Fresnel function  A computer was used to graph S by computing the value of this integral for many values of x. Example 3 FRESNEL FUNCTION Figure 5.3.7, p. 317

It does indeed look as if S(x) is the area under the graph of f from 0 to x (until x ≈ 1.4, when S(x) becomes a difference of areas). Example 3 FRESNEL FUNCTION Figure 5.3.7, p. 317

The other figure shows a larger part of the graph of S. Example 3 FRESNEL FUNCTION Figure 5.3.7, p. 317 Figure 5.3.8, p. 317

If we now start with the graph of S here and think about what its derivative should look like, it seems reasonable that S’(x) = f(x).  For instance, S is increasing when f(x) > 0 and decreasing when f(x) < 0. Example 3 FRESNEL FUNCTION Figure 5.3.7, p. 317

Find  Here, we have to be careful to use the Chain Rule in conjunction with the FTC1. Example 4 FTC1

Let u = x 4. Then, Example 4 FTC1

FTC2 If f is continuous on [a, b], then where F is any antiderivative of f, that is, a function such that F’ = f.

FTC2 Let We know from the FTC1 that g’(x) = f(x), that is, g is an antiderivative of f. Proof

FTC2 If F is any other antiderivative of f on [a, b], then we know from Corollary 7 in Section 4.2 that F and g differ by a constant: F(x) = g(x) + C for a < x < b. Proof—Equation 6

FTC2 However, both F and g are continuous on [a, b]. Thus, by taking limits of both sides of Equation 6 (as x → a + and x → b - ), we see it also holds when x = a and x = b. Proof

FTC2 If we put x = a in the formula for g(x), we get: Proof

FTC2 So, using Equation 6 with x = b and x = a, we have: Proof

FTC2 Evaluate the integral  The function f(x) = x 3 is continuous on [-2, 1] and we know from Section 4.9 that an antiderivative is F(x) = ¼x 4.  So, the FTC2 gives: Example 5

FTC2  Notice that the FTC2 says that we can use any antiderivative F of f.  So, we may as well use the simplest one, namely F(x) = ¼x 4, instead of ¼x or ¼x 4 + C. Example 5

FTC2 We often use the notation So, the equation of the FTC2 can be written as:  Other common notations are and.

FTC2 Find the area under the parabola y = x 2 from 0 to 1.  An antiderivative of f(x) = x 2 is F(x) = (1/3)x 3.  The required area is found using the FTC2: Example 6

FTC2 Find the area under the cosine curve from 0 to b, where 0 ≤ b ≤ π/2.  Since an antiderivative of f(x) = cos x is F(x) = sin x, we have: Example 7

FTC2 In particular, taking b = π/2, we have proved that the area under the cosine curve from 0 to π/2 is sin(π/2) =1. Example 7 Figure 5.3.9, p. 319

FTC2 What is wrong with this calculation? Example 8

FTC2 To start, we notice that the calculation must be wrong because the answer is negative but f(x) = 1/x 2 ≥ 0 and Property 6 of integrals says that when f ≥ 0. Example 9

FTC2 The FTC applies to continuous functions.  It can’t be applied here because f(x) = 1/x 2 is not continuous on [-1, 3].  In fact, f has an infinite discontinuity at x = 0.  So, does not exist. Example 9

FTC Suppose f is continuous on [a, b]. 1.If, then g’(x) = f(x). 2., where F is any antiderivative of f, that is, F’ = f.

INVERSE PROCESSES We noted that the FTC1 can be rewritten as:  This says that, if f is integrated and then the result is differentiated, we arrive back at the original function f.

INVERSE PROCESSES As F’(x) = f(x), the FTC2 can be rewritten as:  This version says that, if we take a function F, first differentiate it, and then integrate the result, we arrive back at the original function F.  However, it’s in the form F(b) - F(a).

SUMMARY Before it was discovered—from the time of Eudoxus and Archimedes to that of Galileo and Fermat—problems of finding areas, volumes, and lengths of curves were so difficult that only a genius could meet the challenge.

SUMMARY Now, armed with the systematic method that Newton and Leibniz fashioned out of the theorem, we will see in the chapters to come that these challenging problems are accessible to all of us.