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082-Engineering-Mathematics-Anthony-Croft-Robert-Davison-Martin-Hargreaves-James-Flint-Edisi-5-2017

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432 Chapter 13 Integration

(f) TheindependentvariableiszbutfromTable13.1wecandeduce ∫ e az dz = eaz

a +c.

Hence, takinga = −3 we obtain

e −3z dz = e−3z

−3 +c=−e−3z 3 +c

(g) Since 1 x 2 =x−2 ,wefind

∫ 1

x 2 dx = ∫

x −2 dx = x−1

−1 +c=−1 x +c

(h) Whenintegratingcos100nπt withrespecttot,notethat100nπisaconstant.Hence,

usingpart (b)wefind

cos100nπt dt = sin100nπt

100nπ +c

13.2.1 Integrationasalinearoperator

Integration, like differentiation, is a linear operator. If f and g are two functions of x,

then

∫ ∫ ∫

f+gdx= fdx+ gdx

This states that the integral of a sum of functions is the sum of the integrals of the individual

functions.IfAisaconstant and f a functionofx, then

Afdx=A

f dx

Thus,constantfactors can betakenthroughthe integral sign.

IfAandBareconstants,and f andgarefunctions ofx, then

Af+Bgdx=A

fdx+B

gdx

These three properties are all consequences of the fact that integration is a linear operator.

Note that the first two are special cases of the third. The properties are used in

Example 13.4.

Example13.4 Use Table 13.1 and the properties of a linear operator to integrate the following

expressions:

(a) x 2 +9 (d) (t +2) 2 (g) 3sin4t

(b) 3t 4 − √ t

(c)

1

x

(e)

(f) 4e 2z

1

+z (h) 4cos(9x +2)

z

(i) 3e 2z

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