Calculus: Analytic Geometry and Calculus, with Vectors

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9.5 Integration by parts 521

We could feel that integration by parts would not enableus to simplify
f log x dx, but we can set


u=logx, dv=ldx


du=1dx, v=x
x

to obtain
f logxdx=xlogx- f1dx=xlogx-x+c.


This result is easily checked by differentiation.


Problems 9.59


1 Derive the following formulas by one or more integrations by parts

(a) f xea: dx =(x-^1
(a az) a°x + c
x2 x2
(b) f x log x dx = 2 log x- 4+ c
xn+l 1
(c) f x" log x dx =
;T_+_1

(logx - n +1) -{-c

(d) f x2eaa dx = (-X^2 - 2 + a3) eaz + c2x^2
' a a2

(e) f xsec2xdx=xtanx+logcosx+c

(f) f (log x)n dx = x(log x)n - n f (log x)n-1 dx

(g) f(x+1), dx = z1+1 log (x -} i) + c

(h) f sin-' xdx =xsin'x-1 1 -x2+c

(i) f tan' x dx = x tan' x - log (1 + x2) + c

2 Setting u = iP, dv = (1 - t)4 dt, derive the formula

fol i (1 - t)4 dt =

q+^1

fo1 t-1(1 - t)4+1 dt.

Observe the fact that the result agrees with the beta integral formula


i
fo tP(1 - t)4 dt

p !q!
= (p +q + 1)1

and the formula r! = r[(r - 1)!]. Remark: In Problems 18 and 19 of Problems
13.49, we shall introduce the Euler gamma integral formula

z! = fo0 t=e t dt (z > -1)


and show how it is used to derive the Euler beta integral formula.
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