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Now to
This can be done using various substitutions. We will look at a hyperbolic substitution at the end of this page. It can also be done using the substitution
But that is begging the question because it feels like we have to know the answer to come up with that idea. We could also do the substitution
But that will require us to know or figure out, that
which is quite easy to find. You can get it from
in a couple of steps. Worse is that after the substitution we end up with the necessity to find the integral of sec θ, and that is not all too straightforward.
The above can be found in various sources, so we will not go through that here, but instead, we will find the answer to our integral using (simple) complex analysis.
Using complex analysis
We will use complex analysis, or rather just complex numbers and a bit of calculus in a rather straightforward way. Let us first pull out a factor of -1 from the square root, and then the rule from the previous page, to get
Technically we are done, but it is in a not all too useful form. To fix this we need to look at the arcsine part. We want it to be able to “absorb” the i.
To start with, if
then
(We put the constant of integration back later on.) From a previous section, we have that
So
or
where
this gives us
or
This we can solve using the quadratic formula to get
Substituting back eI and adding back the constant of integration will give us
Here we let the constant absorb the ln(i). Next comes the question of which sign to use. We may start by noting that
and thus that
If z is larger than one the logarithm is not negative, since
and we can also see that this function is increasing, but less and less fast. The function
should be the derivative of the above logarithmic expression. We can see that is s positive, and decreasing as x>0, and the only option is thus that the integral is the positive variant of the logarithm. So we get
For symmetry reasons we also have
as shown in the graph below.
The inverse of the answer
Let us look at the inverse function
We get
and thus
This is one of the hyperbolic functions. You can find more on those here. So this means that
so
Using hyperbolic functions directly
If we happen to know our hyperbolic functions we can do the substitution
We also have that
This gives us
The above generalized a bit
Now, we get
or
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