8.4 Integration by trigonometric and other substitutions 473
we look at itand generate the idea that we should try setting x = a sec 8.
Then x' = a sec 0 tan B, so
(8.474)
- 1 ('sec0d8
f
J=
1 J (sin 8)-2 cos 8 d8
a2
J 1 - a sec 0 tan B do
J (a2 t^1
8
_ 1 (sin 8)-i
a'- -1 + c
x
a2
a2 + C.
x2-
It is not implied that we know in advance that the integrand should be
written in terms of sines and cosines, but trying this possibility and seeing
that the power formula can be applied is all a part of the game.
Our last problem has a lengthy solution. We can bravely start to
evaluate the integral in
(8.48) J2=j x2-a2dx
by setting x = a sec 8. Then x' = a sec 0 tan 0 and
J2 = f a2 tan2 0 a sec 0 tan 8 do
so
(8.481) J2 = a2f tang 8 sec 0 do.
It happens that this integral is an elementary function, but there is no
simple direct way of discovering the facts. Authors and teachers, as
well as students, can work for hours on this problem unless they remember
how to solve it or (and this much better) have a guiding principle. The
principle is the following. If we want to learn something about an
integral and other methods fail to be helpful, we try integration by parts.
By this we mean that we try to determine two functions u and v of the
variable of integration in such a way that the integral we are studying
will be the left member of the formula
(8.482) fu(8)v'(8) d8 = u(8)v(8) - fv(8)u'(6) d8
and, moreover, the "parts" on the right side enable us to make progress
with our problem. Assuming that u and v have continuous derivatives
over intervals where we use the formula,differentiation shows that the
formula is correct. The trick is to use it effectively. Naturally, we
want the functions u, v, u', v' to be as simple aspossible, and it is quite
easy to discover that the best way to convertJ2 into the left member of
(8.482) is to set
(8.483)
{ 1'( )=
aa' tan 0,
2 sec 0, vv(0) = sec
8.tan 8