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To recap: to integrate is to find the antiderivative of a function, i.e. to find a function that, taking the derivative of it, gives our original function back. This means that we can find integration rules just by using the derivative rules in the opposite direction.
One of the derivative rules is the chain rule:
For example
Working backwards means that
The constant C since the derivative of an added constant is 0.
It might be hard to see how to do this, but happily, there is a method to do this. This trick can be useful when the integrand (the equation we want to integrate) is a factor of two expressions.
To start with we have to look at if the derivative of a function or inner function is equal to the other factor, i.e. if we have
or
We call the function f (…) the outer function and g(x) the inner function.
(The first case is just a special case of the second. The function f is just the identity function that does nothing.)
In our example above we have
As we will see we can be of by a constant factor, and the trick we will use will work.
The substitution
Let us do the substitution
Now let us take the derivative of this with respect to x. We get
Let us multiply this by dx. Can we do that? In this case, we will see that it will work. The proof is in the pudding as one says.
Now, this will give us
Finally, we replace the expression for u back:
In practice
Ok, let us try this on our original example.
Here we can see that the derivative of x3+2 is 3x2, so we are only off with a constant factor, but that is OK as we will see.
In the above, I indicate the whole process of the substitution with a vertical line, and then I continue with an “=” sign, indicating that we simply continue with the integral again. In the part with the vertical line, our goal is to get to something we could easily substitute away – in this case x2dx.
I would usually go directly from u=x3+2 to du=3x2dx (I would differentiate).
A few examples
Here it might be a bit harder to see what the outer function is, but it is 1 divided by something, i.e. the reciprocal function that has the integral ln(of the something).
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