Definition
Now recall that
is said to be an antiderivative of f if
. However,
is not the only antiderivative. We can add any constant to
without changing the derivative. With this, we define the indefinite integral as follows:
where
satisfies
and
is any constant.
The function
, the function being integrated, is known as the integrand. Note that the indefinite integral yields a family of functions.
Example
Since the derivative of
is
, the general antiderivative of
is
plus a constant. Thus,

Example: Finding antiderivatives
Let's take a look at
. How would we go about finding the integral of this function? Recall the rule from differentiation that

In our circumstance, we have:

This is a start! We now know that the function we seek will have a power of 3 in it. How would we get the constant of 6? Well,

Thus, we say that
is an antiderivative of
.
Indefinite integral identities
Basic Properties of Indefinite Integrals
Constant Rule for indefinite integrals
If
is a constant then
Sum/Difference Rule for indefinite integrals


Indefinite integrals of Polynomials
Say we are given a function of the form,
, and would like to determine the antiderivative of
. Considering that

we have the following rule for indefinite integrals:
Power rule for indefinite integrals
for all
Integral of the Inverse function
To integrate
, we should first remember

Therefore, since
is the derivative of
we can conclude that
Note that the polynomial integration rule does not apply when the exponent is
. This technique of integration must be used instead. Since the argument of the natural logarithm function must be positive (on the real line), the absolute value signs are added around its argument to ensure that the argument is positive.
Integral of the Exponential function
Since

we see that
is its own antiderivative. This allows us to find the integral of an exponential function:
Integral of Sine and Cosine
Recall that


So
is an antiderivative of
and
is an antiderivative of
. Hence we get the following rules for integrating
and

We will find how to integrate more complicated trigonometric functions in the chapter on integration techniques.
Example
Suppose we want to integrate the function
. An application of the sum rule from above allows us to use the power rule and our rule for integrating
as follows,
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The Substitution Rule
The substitution rule is a valuable asset in the toolbox of any integration greasemonkey. It is essentially the chain rule (a differentiation technique you should be familiar with) in reverse. First, let's take a look at an example:
Preliminary Example
Suppose we want to find
. That is, we want to find a function such that its derivative equals
. Stated yet another way, we want to find an antiderivative of
. Since
differentiates to
, as a first guess we might try the function
. But by the Chain Rule,

Which is almost what we want apart from the fact that there is an extra factor of 2 in front. But this is easily dealt with because we can divide by a constant (in this case 2). So,

Thus, we have discovered a function,
, whose derivative is
. That is,
is an antiderivative of
. This gives us

Generalization
In fact, this technique will work for more general integrands. Suppose
is a differentiable function. Then to evaluate
we just have to notice that by the Chain Rule

As long as
is continuous we have that

Now the right hand side of this equation is just the integral of
but with respect to
. If we write
instead of
this becomes
So, for instance, if
we have worked out that

General Substitution Rule
Now there was nothing special about using the cosine function in the discussion above, and it could be replaced by any other function. Doing this gives us the substitution rule for indefinite integrals:
Substitution rule for indefinite integrals
Assume
is differentiable with continuous derivative and that
is continuous on the range of
. Then
Notice that it looks like you can "cancel" in the expression
to leave just a
. This does not really make any sense because
is not a fraction. But it's a good way to remember the substitution rule.
Examples
The following example shows how powerful a technique substitution can be. At first glance the following integral seems intractable, but after a little simplification, it's possible to tackle using substitution.
Example
We will show that

First, we re-write the integral:
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Now we perform the following substitution:


Which yields:







Integration by Parts
Integration by parts is another powerful tool for integration. It was mentioned above that one could consider integration by substitution as an application of the chain rule in reverse. In a similar manner, one may consider integration by parts as the product rule in reverse.
Preliminary Example
General Integration by Parts
Integration by parts for indefinite integrals
Suppose
and
are differentiable and their derivatives are continuous. Then

it is also very important to notice that

is not equal to
to set the
and
we need to follow the rule called I.L.A.T.E.
ILATE defines the order in which we must set the 
- I for inverse trigonometric function
- L for log functions
- A for algebraic functions
- T for trigonometric functions
- E for exponential function
f(x) and g(x) must be in the order of ILATE
or else your final answers will not match with the main key
Examples
Example
Find
Here we let:
, so that
,
, so that
.
Then:
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Example
Find
In this example we will have to use integration by parts twice.
Here we let
, so that
,
, so that
.
Then:
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Now to calculate the last integral we use integration by parts again. Let
, so that
,
, so that 
and integrating by parts gives

So, finally we obtain

Example
Find
The trick here is to write this integral as

Now let
so
,
so
.
Then using integration by parts,
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Example
Find
Again the trick here is to write the integrand as
. Then let
so 
so 
so using integration by parts,
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Example
Find
This example uses integration by parts twice. First let,
so 
so 
so

Now, to evaluate the remaining integral, we use integration by parts again, with
so 
so 
Then
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Putting these together, we have

Notice that the same integral shows up on both sides of this equation, but with opposite signs. The integral does not cancel; it doubles when we add the integral to both sides to get


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