
274 integration by substitution
du
––
dx
du
––
dx
√x3–1
du
––
dx
du
––
dx
Then:
The integration-by-parts formula can be applied more
than once to complete an integration problem. For
example, to evaluate ∫excos(x)dx, one application of
the technique yields:
∫excos(x)dx = exsin(x) – ∫exsin(x)dx
Applying the integration-by-parts technique to the sec-
ond integral yields:
∫excos(x)dx = exsin(x) – ∫exsin(x)dx
= exsin(x) – [–excos(x) – ∫ex(–cos(x))dx]
= ex(sin(x) + cos(x)) – ∫excos(x)dx
Algebra now shows that the integral we seek is given by:
The method of integration by parts was discovered by
English mathematician B
ROOK
T
AYLOR
(1685–1731).
See also
ANTIDIFFERENTIATION
;
INTEGRAL CAL
-
CULUS
;
INTEGRATION BY SUBSTITUTION
;
RECURRENCE
RELATION
.
integration by substitution (change of variable, sub-
stitution rule for integration) This technique of inte-
gration is used to find the integral of a function easily
recognized as a
COMPOSITION
of two simpler functions.
It is essentially the
CHAIN RULE
for differentiation
employed in reverse. Specifically, the chain rule states:
Integrating both sides yields:
Noting that, since fis the antiderivative of f′, the right-
hand side of this formula can be thought of as the
indefinite integral of f′evaluated with uas the variable.
Thus it is valid to write:
This equation is the change-of-variables equation for
integration. For example, we can use it to evaluate
∫2x(1 + x2)4dx. Setting u(x) = 1 + x2, giving = 2x,
the integral reads:
Notice that the notation we used here mimics the prop-
erties of fractions: we are permitted to replace a term
dx under an integral sign by the term dx.
When using this technique, one typically chooses
u(x) to be a function that simplifies a complicated part
of the
INTEGRAND
, and then adjusts matters so that the
factor appears explicitly. For example, to evaluate
∫x2dx, it is natural to set u(x) = x3– 1. Then
= 3x3, and we have:
x x dx x u dx
xudx
udu
dx dx
udu
uC
xC
23 2
2
3
2
3
3
2
1
1
33
1
3
1
3
1
3
2
3
2
91
−=
=
=
=
=⋅ +
=−
()
+
∫∫
∫
∫
∫
21
1
5
1
51
244
4
5
24
x x dx u du
dx dx
udu
uC
xC
+
()
=
=
=+
=+
()
+
∫∫
∫
′=′
∫∫
fuxdu
dx dx f u du(()) ()
′=+
∫fuxdu
dx dx f u x C(()) (())
d
dx fux f ux du
dx
( ( )) ( ( ))=′
exdxex xC
xx
cos( ) sin( ) cos( )=+
()
+
∫1
2
ln( ) ln( ) ln( )xdx x x xxdx x x x C=−⋅=−+
∫∫ 1
ux x v x
ux xvx x
( ) ln( ) ( )
() ()
=′=
′==
1
1