MadViolinist said:
Thanks for the answer!
However, I do not get the step where ln(limn→∞ un)=limn→∞ ( ln(un)). How did you change the order of the natural log and the limit?
If ##f## is any function that is continuous at ##L##, and ##\lim_{n \rightarrow \infty} u_n = L##, then ##\lim_{n \rightarrow \infty} f(u_n) = f(\lim_{n \rightarrow \infty} u_n) = f(L)##. You can prove this quite easily using the epsilon-delta definition of continuity.
Assuming that theorem, all you need is the fact that ##\ln## is continuous at ##L##, where ##L## is any real positive number. (By the way, positivity of ##L## is another assumption that needs to be added to the problem statement, otherwise the equation makes no sense.)
How to prove that ##\ln## is continuous depends on how you defined ##\ln##. One standard definition is
$$\ln(x) = \int_{1}^{x} \frac{1}{t} dt$$
If we use that definition, then
$$\begin{align}
|\ln(x+h) - \ln(x)| &= \left|\int_{1}^{x+h} \frac{1}{t} dt - \int_{1}^{x} \frac{1}{t}\right|\\
&= \left|\int_{x}^{x+h}\frac{1}{t} dt\right|\\
\end{align}$$
If ##h > 0## then we have the bound
$$\left|\int_{x}^{x+h}\frac{1}{t} dt\right| \leq \left|\int_{x}^{x+h}\frac{1}{x} dt\right| = \left| \frac{h}{x} \right|$$
which we can make as small as we like as ##h \rightarrow 0##. A similar argument holds for ##h < 0##.