Topic-2-The Fundamental Theorem of Calculus

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Dr. Gizem SEYHAN Γ–ZTEPE

Topic-2-The Fundamental Theorem of Calculus

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The Fundamental Theorem of Calculus is appropriately named because itestablishes a connection between the two branches of calculus: differential calculusand integral calculus.

Differential calculus arose from the tangent problem, whereas integral calculusarose from a seemingly unrelated problem, the area problem. Newton’s teacher atCambridge, Isaac Barrow (1630–1677), discovered that these two problems areactually closely related. In fact, he realized that differentiation and integration areinverse processes.

The Fundamental Theorem of Calculus gives the precise inverse relationshipbetween the derivative and the integral. It was Newton and Leibniz who exploitedthis relationship and used it to develop calculus into a systematic mathematicalmethod.

In particular, they saw that the Fundamental Theorem enabled them to computeareas and integrals very easily without having to compute them as limits of sumsas we did in Sections 1.1 and 1.2.

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The first part of the Fundamental Theorem deals withfunctions defined by an equation of the form

where 𝑓 is a continuous function on [π‘Ž, 𝑏] and π‘₯ variesbetween π‘Ž and 𝑏. Observe that 𝑔 depends only on π‘₯,which appears as the variable upper limit in the integral.

If π‘₯ is a fixed number, then the integral π‘Ž

π‘₯𝑓 𝑑 𝑑𝑑 is a

definite number. If we then let π‘₯ vary, the number

π‘Ž

π‘₯𝑓 𝑑 𝑑𝑑 also varies and defines a function of π‘₯ denoted

by 𝑔 π‘₯ .

𝑔 π‘₯ = ΰΆ±π‘Ž

π‘₯

𝑓 𝑑 𝑑𝑑 (1)

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If 𝑓 happens to be a positive function, then𝑔(π‘₯) can be interpreted as the area underthe graph of 𝑓 from π‘Ž to π‘₯, where π‘₯ can varyfrom π‘Ž to 𝑏. (Think of as the β€œarea so far”function; see Figure 1.)

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If 𝑓 is continuous on [π‘Ž, 𝑏], then the function𝑔 defined by

is continuous on [π‘Ž, 𝑏], and differentiable on (π‘Ž, 𝑏), and 𝑔′ π‘₯ = 𝑓 π‘₯ .

This theorem says that the derivative of a definite integralwith respect to its upper limit is the integrand evaluated atthe upper limit.

𝑔 π‘₯ = ΰΆ±π‘Ž

π‘₯

𝑓 𝑑 𝑑𝑑 , π‘Ž ≀ π‘₯ ≀ 𝑏

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Example-1

Find the derivative of the function 𝑔 π‘₯ = 0

π‘₯1 + 𝑑2𝑑𝑑.

Solution

Since 𝑓 𝑑 = 1 + 𝑑2 is continuous by using FTC1,

𝑔′ π‘₯ = 1 + π‘₯2

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Example-2

Although a formula of the form 𝑔 π‘₯ = π‘Ž

π‘₯𝑓 𝑑 𝑑𝑑 may seem

like a strange way of defining a function, books on physics,chemistry, and statistics are full of such functions.

For instance, the Fresnel function

𝑆 π‘₯ = ΰΆ±0

π‘₯

sin( ΰ΅—πœ‹π‘‘2

2)𝑑𝑑

is named after the French physicist Augustin Fresnel (1788–1827), who is famous for his works in optics. This functionfirst appeared in Fresnel’s theory of the diffraction of light

waves, but more recently it has been applied to the design ofhighways.

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Part 1 of the Fundamental Theorem tells us how to differentiate the Fresnel function:

𝑆′ π‘₯ = sin( ΰ΅—πœ‹π‘₯2

2)

This means that we can apply all the methods of differential calculus to analyze 𝑆.

Figure 2 shows the graphs of 𝑓 π‘₯ = sin( ΰ΅—πœ‹π‘₯2

2) and the Fresnel function 𝑆 π‘₯ =

0

π‘₯sin( ΰ΅—πœ‹π‘‘2

2)𝑑𝑑

Figure 3 shows a larger part of the graph of .

Figure-2 Figure-3

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In Section 1.2 we computed integrals from the

definition as a limit of Riemann sums and we

saw that this procedure is sometimes long and difficult.

The second part of the Fundamental Theorem of Calculus,which follows easily from the first part, provides us with amuch simpler method for the evaluation of integrals.

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If 𝑓 is continuous on [π‘Ž, 𝑏], then

where 𝐹 is any antiderivative of 𝑓, that is, a functionsuch that 𝐹′ = 𝑓.

ΰΆ±π‘Ž

𝑏

𝑓 π‘₯ 𝑑π‘₯ = 𝐹 𝑏 βˆ’ 𝐹(π‘Ž)

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Part 2 of the Fundamental Theorem states that if we know

an antiderivative 𝐹 of 𝑓, then we can evaluate π‘Ž

𝑏𝑓 π‘₯ 𝑑π‘₯

simply by subtracting the values of 𝐹 at the endpoints of the

interval [π‘Ž, 𝑏]. It’s very surprising that π‘Ž

𝑏𝑓 π‘₯ 𝑑π‘₯, which was

defined by a complicated procedure involving all of the values of 𝑓(π‘₯) for π‘Ž ≀ π‘₯ ≀ 𝑏, can be found by knowing the values of 𝐹(π‘₯) at only two points, π‘Ž and 𝑏.

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Example-3

Evaluate the integral 1

3𝑒π‘₯dx.

Solution

The function 𝑓 π‘₯ = 𝑒π‘₯ is continuous everywhere and we know that an antiderivative is 𝐹(π‘₯) = 𝑒π‘₯, so Part 2 of the Fundamental Theorem gives

ΰΆ±1

3

𝑒π‘₯ 𝑑π‘₯ = 𝐹 3 βˆ’ 𝐹 1 = 𝑒3 βˆ’ 𝑒

Notice that FTC2 says we can use any antiderivative 𝐹 of 𝑓. So we may as well use the simplest one, namely 𝐹 π‘₯ = 𝑒π‘₯ instead of 𝑒π‘₯ + 7 π‘œπ‘Ÿ 𝑒π‘₯ + 𝐢.

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Note: We often use the notation

ΰΈ­ΰΆ±π‘Ž

𝑏

𝑓 π‘₯ 𝑑π‘₯ = 𝐹(π‘₯)

π‘Ž

𝑏

= 𝐹 𝑏 βˆ’ 𝐹(π‘Ž)

where 𝐹′ = 𝑓.

Example-4

Find the area under the parabola 𝑦 = π‘₯2 from 0 to 1.

OR

Evaluate the integral0

1π‘₯2𝑑π‘₯.

Example-5

Evaluate 3

6 𝑑π‘₯

π‘₯.

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Example-6

Find the area under the cosine curve from 0 to b , where 0 ≀

𝑏 β‰€πœ‹

2.

Example-7

What is wrong with the following calculation?

ΰΆ±βˆ’1

3 1

π‘₯2𝑑π‘₯ = ΰΈ­

π‘₯βˆ’1

βˆ’1βˆ’1

3

=βˆ’1

3βˆ’ 1 =

βˆ’4

3

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The Fundamental Theorem of Calculus say that differentiation andintegration are inverse processes. Each undoes what the other does.

The Fundamental Theorem of Calculus is unquestionably the mostimportant theorem in calculus and, indeed, it ranks as one of thegreat accomplishments of the human mind. Before it wasdiscovered, from the time of Eudoxus and Archimedes to the time ofGalileo and Fermat, problems of finding areas, volumes, and lengthsof curves were so difficult that only a genius could meet thechallenge. But now, armed with the systematic method that Newtonand Leibniz fashioned out of the Fundamental Theorem, we will seein the chapters to come that these challenging problems areaccessible to all of us.

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Theorem (Symmetry Rule)

Let 𝑓 be a continuous function defined on [βˆ’π‘Ž, π‘Ž]

(i) If 𝑓 is an odd function, then π‘Žβˆ’

π‘Žπ‘“ π‘₯ 𝑑π‘₯ = 0

(ii) If 𝑓 is an even function, then π‘Žβˆ’

π‘Žπ‘“ π‘₯ 𝑑π‘₯ = 2 0

π‘Žπ‘“ π‘₯ 𝑑π‘₯.

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If 𝑔′ is continuous on [π‘Ž, 𝑏] and 𝑓 is continuous on therange of 𝑒 = 𝑔(π‘₯), then

ΰΆ±π‘Ž

𝑏

𝑓 𝑔 π‘₯ 𝑔′ π‘₯ 𝑑π‘₯ = ࢱ𝑔(π‘Ž)

𝑔(𝑏)

𝑓 𝑒 𝑑𝑒

This rule says that when using a substitution in adefinite integral, we must put everything in terms ofthe new variable , not only and but also the limits ofintegration.

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Example-8

Evaluate the following integrals:

a) 0

42π‘₯ + 1 𝑑π‘₯

b) 0

πœ‹2

4sin π‘₯

π‘₯𝑑π‘₯

c) 0

πœ‹π‘₯ cos π‘₯2𝑑π‘₯

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Solution

a) 0

42π‘₯ + 1 𝑑π‘₯

The geometric interpretation of Example(8.a) is shown in Figure 2. The substitution𝑒 = 2π‘₯ + 1stretches the interval [0,4] by afactor of 2 and translates it to the right byunit. The Substitution Rule shows that thetwo areas are equal.

More examples will be solved in the class.

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Example

Find the average value of the function 𝑓 π‘₯ = 1 + π‘₯2on theinterval [βˆ’1,2].

Solution

With π‘Ž = βˆ’1 and 𝑏 = 2, we have

π‘“π‘Žπ‘£π‘’ =1

(2 βˆ’ (βˆ’1))ΰΆ±

βˆ’1

2

1 + π‘₯2 𝑑π‘₯ = 2

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