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

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Section 5.5 The Substitution Rule 417

Therefore

y 4

s2x 1 1 dx − y 9 1

2 su du

0 1

− 1 2 ? 2 3 u 3y2 g 1

9

− 1 3 s93y2 2 1 3y2 d − 26

3

Observe that when using (6) we do not return to the variable x after integrating. We

simply evaluate the expression in u between the appropriate values of u.

n

The integral given in Example 8 is an

abbreviation for

y 2 1

1 s3 2 5xd dx 2

Example 8 Evaluate y 2

1

dx

s3 2 5xd 2 .

SOLUtion Let u − 3 2 5x. Then du − 25 dx, so dx − 2 1 5 du. When x − 1, u − 22

and when x − 2, u − 27. Thus

y 2

1

dx

s3 2 5xd 2

− 2 1 5 y27 22

du

u 2

27

− 2 1 F2 1 − 1

5 uG22

27

5uG22

− 1 5

S2 1 7 1 1 2D − 1 14

n

Since the function f sxd − sln xdyx

in Example 9 is positive for x . 1,

the integral represents the area of the

shaded region in Figure 2.

y

0.5

y= ln x

x

Example 9 Calculate y e

1

ln x

x

dx.

SOLUtion We let u − ln x because its differential du − dxyx occurs in the integral.

When x − 1, u − ln 1 − 0; when x − e, u − ln e − 1. Thus

y e

1

ln x

x

dx − y 1

u du − u 2

0

1

2G0

− 1 2

n

0

FIGURE 2

1 e

x

Symmetry

The next theorem uses the Substitution Rule for Definite Integrals (6) to simplify the

calculation of integrals of functions that possess symmetry properties.

7 Integrals of Symmetric Functions Suppose f is continuous on f2a, ag.

(a) If f is even f f s2xd − f sxdg, then y a f sxd dx − 2 2a ya f sxd dx.

0

(b) If f is odd f f s2xd − 2f sxdg, then y a 2a

f sxd dx − 0.

Proof We split the integral in two:

8

y a 2a

f sxd dx − y 0 f sxd dx 1 y a

2a

0

f sxd dx − 2y 2a

0

f sxd dx 1 y a

f sxd dx

0

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