The singular integrands I will ask about in this post about appear a lot in numerical integration so I would really like to understand theoretically what makes some of these integrands 'more integrable' (whatever that means) than others.
Question 1:
I experimented in Wolfram Alpha by inputing a command to calculate:
$$ \int_0^1 (\ln |x|)^a \bigg(\frac{1}{|x|}\bigg)^b dx, $$ where $a,b \in [0,1]$ and $a+b = 1$. I found that it was always possible to integrate as long as we didn't have $a = 0, \ b = 1$! So what exactly is the theory behind why this happens? Why is $\ln |x|$ integrable on $[0, 1]$ yet $\frac{1}{|x|}$ isn't, even though they are both singular at zero?
Question 2:
What can be said about the integrability of the following functions:
- $|x| \ln|x|$
- $|x|^2 \ln|x|$
These type of functions where $\ln|x|$ is multiplied by $|x|^k$ for some $k \in \mathbb{N}$ really show up a lot in boundary integral situations where we are integrating on a closed curve in $\mathbb{R}^2$. Are these integrands 'more integrable' than the original $\ln|x|$ case? What make these integrands nicer/worse than $\ln |x|$?
For $b \ne 1$, an antiderivative of $x^{-b}$ is $x^{-b+1}/(1-b)$, which goes to $\infty$ as $x \to 0+$ if $b > 1$ but not if $b < 1$. Thus $x^{-b}$ is integrable near $0$ if $b < 1$ but not if $b > 1$. The same goes for $\ln(x)^{a} x^{-b}$, as for every $\epsilon > 0$ we have $\ln(x) x^\epsilon \to 0$ as $x \to 0+$.
Now to deal with $b = 1$. For $a \ne -1$, an antiderivative of $(-\ln(x))^a x^{-1}$ is $(-\ln(x))^{a+1}/(a+1)$, which goes to $\infty$ as $x \to 0+$ if $a > -1$ but not if $a < -1$. So $(-\ln(x))^a x^{-1}$ is integrable near $0$ if $a < -1$ but not if $a > -1$.
Finally, an antiderivative of $(-\ln(x))^{-1} x^{-1}$ is $-\ln(-\ln(x))$, which goes to $\infty$ as $x \to 0+$, so $1/(x \ln(x))$ is not integrable near $0$.