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James Stewart-Calculus_ Early Transcendentals-Cengage Learning (2015)

A five star textbook for college calculus

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Section 5.3 The Fundamental Theorem of Calculus 397

Although the theorem may be surprising at first glance, it becomes plausible if we

interpret it in physical terms. If vstd is the velocity of an object and sstd is its position at

time t, then vstd − s9std, so s is an antiderivative of v. In Section 5.1 we considered an

object that always moves in the positive direction and made the guess that the area under

the velocity curve is equal to the distance traveled. In symbols:

y b

vstd dt − ssbd 2 ssad

a

That is exactly what FTC2 says in this context.

Example 5 Evaluate the integral y 3

e x dx.

1

Compare the calculation in Example 5

with the much harder one in Example

5.2.3.

SOLUTION The function f sxd − e x is continuous everywhere and we know that an antiderivative

is Fsxd − e x , so Part 2 of the Fundamental Theorem gives

y 3

e x dx − Fs3d 2 Fs1d − e 3 2 e

1

Notice that FTC2 says we can use any antiderivative F of f. So we may as well use

the simplest one, namely Fsxd − e x , instead of e x 1 7 or e x 1 C.

n

We often use the notation

So the equation of FTC2 can be written as

Fsxdg a

b

− Fsbd 2 Fsad

y b

b

f sxd dx − Fsxdg

a

a

where

F9− f

b

Other common notations are Fsxd

|a

and fFsxdg ab .

Example 6 Find the area under the parabola y − x 2 from 0 to 1.

SOLUTION An antiderivative of f sxd − x 2 is Fsxd − 1 3 x 3 . The required area A is found

using Part 2 of the Fundamental Theorem:

In applying the Fundamental Theorem

we use a particular antiderivative F

of f . It is not necessary to use the

most general antiderivative.

A − y 1

x 2 dx − x 3

0

3G0

1

− 13

3 2 03

3 − 1 3

If you compare the calculation in Example 6 with the one in Example 5.1.2, you will

see that the Fundamental Theorem gives a much shorter method.

n

Example 7 Evaluate y 6 dx

3 x .

SOLUTION The given integral is an abbreviation for

y 6

3

1

x dx

An antiderivative of f sxd − 1yx is Fsxd − ln | x |

Fsxd − ln x. So

y 6

3

1

x dx − ln xg 6 3 − ln 6 2 ln 3 − ln 6 3 − ln 2

and, because 3 < x < 6, we can write

n

Copyright 2016 Cengage Learning. All Rights Reserved. May not be copied, scanned, or duplicated, in whole or in part. Due to electronic rights, some third party content may be suppressed from the eBook and/or eChapter(s).

Editorial review has deemed that any suppressed content does not materially affect the overall learning experience. Cengage Learning reserves the right to remove additional content at any time if subsequent rights restrictions require it.

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