We know that the functions f(x)and f−^1 (x)are symmetric about the line y=x
as illustrated in the figure 12-1. Examine the figure 12-1 and note that one can
express the area A=
∫b
af(x)dx as
A=
∫b
a
f(x)dx = (b−a)d
︸ ︷︷ ︸
orange+green area
−
∫d
c
[f−^1 (x)−a]dx
︸ ︷︷ ︸
green area
= (b−a)d−
∫d
c
f−^1 (x)dx + (d−c)a
(12.1)
which shows that the area A is given by the rectangular area (orange plus green
area) minus the area under the inverse curve (green plus grey area) corrected by the
rectangular grey area. Hence, if you know
∫b
a
f(x)dx , then you can find
∫d
c
f−^1 (x)dx
and vice-versa.
The use of integration to sum infinite series
There is a definite relation between certain infinite series and definite integrals.
For example, consider the relationship between the problem of finding the sum of
the alternating infinite series
1
a
−^1
a+b
+^1
a+ 2 b
−^1
a+ 3b
+^1
a+ 4 b
−···+ (−1)n^1
a+nb
+··· (12.2)
where a > 0 ,b > 0 and the associated problem of evaluating the definite integral
∫ 1
0
ta−^1
1 + tbdt (12.3)
Use the well known series expansion
1
1 + x= 1 −x+x
(^2) +x (^3) −x (^4) +··· (12.4)
with xreplaced by tbto write the equation (12.3) in the form
∫ 1
0
ta−^1
1 + tb
dt =
∫ 1
0
ta−^1
[
1 −tb+t^2 b−t^3 b+t^4 b−···
]
dt (12.5)
and then integrate each term to produce the result
∫ 1
0
ta−^1
1 + tbdt =
[ta
a−
ta+b
a+b+
ta+2b
a+ 2 b+···+ (−1)
nta+nb
a+nb +···
] 1
∫^0
1
0
ta−^1
1 + tbdt =
1
a−
1
a+b+
1
a+ 2 b+···+ (−1)
n^1
a+nb +···
(12.6)