(iii) When we make a substitution, we can change the limits too – then
we don’t have to return to the original variables.
In
∫ 1
0
x^2
x^3 + 1
dxthe numerator is the derivative of the denomi-
nator (almost), so putu=x^3 +1.
Thendu= 3 x^2 dxorx^2 dx=
du
3
The limits onuare obtained from the substitution
whenx= 0 ,u= 03 + 1 = 1
whenx= 2 ,u= 23 + 1 = 9
So ∫ 2
0
x^2
x^3 + 1
dx=
1
3
∫ 9
1
du
u
=
1
3
[lnu]^91
=
1
3
(ln 9−ln 1)
=
1
3
ln 9
remembering that ln 1=0.
(iv) This sort of integral is very important in the theory of Fourier
series (see Chapter 17). Using the double angle formula we have
∫ 2 π
0
cosxsinxdx=
1
2
∫ 2 π
0
sin 2xdx
=−
1
4
[cos 2x]^20 π= 0
B.
∫ 2
0
dx
x^2 − 1
=
∫ 2
0
dx
(x− 1 )(x+ 1 )
The integrand doesn’t exist (‘becomes singular’) atx=1, which
is within the range of integration.
9.3 Reinforcement
9.3.1 Definition of integration
➤➤
251 253
➤
A.Differentiate the following functions:
(i) 3x^3 (ii)
√
3 x (iii)
2
x^4
(iv) x^2 /^5