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Litecoin is an extremely interesting altcoin which was created in 2011 by a group of people who were dissatisfied with the way Bitcoin was functioning. Their major issue with Bitcoin was that it was too slow, as transactions were taking a long time to be verified.

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Instead of a maximum supply of 21 million coins, Litecoin has a maximum supply of 84 million, which gives Litecoin a much faster block time, some think it could be as fast as 2 minutes.

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Because of its fast block time, Litecoin is a very popular currency for quick transactions. It is also a very stable currency as it is very regulated by community involvement. There are many people who have committed to the Litecoin blockchain, which means it’s a strong currency.

There is also a huge community, as well as an active development team. It is an exciting time for Litecoin as it is really showing that it is very different and is here to stay in the crypto space.

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Litecoin has a lot of parallels with Bitcoin. You can be introduced to both sides using these Litecoin facts.

Litecoin seems to follow the path that Bitcoin has been on. After Bitcoin, Litecoin is another successful crypto currency. It has been successful because it is easy

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DiskDigger crackQ:

Uniform distribution on circular sector for poles (special case of Bessel)

I would like to get $\phi$ uniformly distributed over the solid $0 \leq \phi \leq 2\pi$ and $0 \leq r \leq 1$. It is easy to prove that when $a$ is the length of the arc $r \leq r \leq 1$, we obtain the arcs of equal length, which means that the $r$ of $\phi$ varies within the radius of the inner circle.
I would like to obtain the uniform distribution, $\phi$ at the beginning (when $r=0$) of the specific case of $a = \pi/2$ (Bessel $\text{J}_{0}$). I know that the distribution of $\phi$ when $r=0$ is obtained by the uniform distribution on the solid $0 \leq \phi \leq 2\pi$ and the variable $r$, through $r=0$. But for the inner circle I have problems.
I would like to obtain the formula of the density function for the $\phi$ of the Bessel, that is $\text{J}_{0}(2r)$ for $0 \leq \phi \leq 2\pi$.
I have tried calculating $F(h)$, where $h=\phi$, the density function, which is:
$$F(h)=\int\limits_{0}^{2\pi} 2\pi F(h) \, d\phi = \int\limits_{0}^{2\pi} 2\pi \, h \, r \, dr = \pi \int\limits_{0}^{2\pi} h^2 r^2 dr.$$
Therefore, the distribution for $\phi$ is:
$$F(h) = \frac{\pi}{6} h^3,\, 0 \leq h \leq 2\pi.$$
However, I do not know how to integrate.
What should be done with the above integral? Also, I have the same problem for \$\text{J
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