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CHAPTER XVII
INTEGRAL CALCULUS. STANDARD FORMS


1. In the preceding chapter we found that the process of integrais the converse of that of differentiation. In other words, that given f' (x) we have to find a function f (x) such that f' (x) is its first differential coefficient. The analogy with the process of finite integration is apparent and the remarks made in Chapter VII, 5, apply equally to the present case.
It may, therefore, be said again that the process of integration cannot be carried out for every function, that definite rules cannot be laid down to apply in every case, and that the student must look to applying the results of the differential calculus as a guide in
solving any problem presented by the function under consideration.
2. In the first place it is necessary to point out that the ordinary algebraic laws apply to the integrating symbol fdx in the same way as they have been shown to apply to the symbolic operations 0 and d
d- x. Thus:

and therefore


rudx+ fvdx+ fwdx+...=J(u+v+w+..•)dx ...(I).

if da=u,    d(cv)_cdv_cu,
dx    dv    dx
therefore    fcudx=cv_cludx     (2).
3. It should be added that the process of integration introduces a constant into every indefinite integral, for, if u = dx,
d (v + c) _ dv _
dx    dx    '

I

94    INTEGRAL CALCULUS
and therefore    fudx = v + c,
which result is, indeed, obvious from the consideration that a constant term disappears on differentiation.
STANDARD FORMS    95
3. The results are embodied in the following table. Their verifiis left as an exercise to the student.
Function Integral
rx"dx
!
1 dx
x
Jaxdx
f exdx
f cosxdx
yin x dx
f sec2xdx
Icosec2xdx
xn+i
n    1
log,x
ax
lug, a
ex
sinx
— cos x
tanx
—cotx

In each case the constant c has been omitted for the sake of simplicity, but its importance in the result must not be forgotten.
96    INTEGRAL CALCULUS
The series may be written as
1 rl    1    1    1    ' m
m 1    in+ tin++    m x
1+— 1+    l+x.
x    x    x
The terms in the denominator consist of values of a quantity, which
can be represented by y, increasing by equal increments of m. Also x
the sum of the series is multiplied by m, which is the increment x
in the value of the denominator.
Since the initial value of the denominator y is unity and the final value is 1 + m, from our definition of an integral we may write,
when x-.-co and therefore m-..O,
x
Lt 1 rl + 1 + 1 + ... +    1    m _ 1 I+m dy
_    _ _ f _
    nt 1 1+m l+ ~n    l+x.in x in    y
x    x    x,
1
= m [log i+m
= ma log 1 +m.