I have a question concerning the proof of the continuity of f(x)=lnx.
I read in a comment by Pedro Tamaroff to ncmathsadist's answer to this question that this can be proved in two steps:
- first by proving that f(x) is continuous at 1,
- and then by using ln(xy)=ln(x)+ln(y).
However, I do not really see how to do it.
How does it actually work?
Answer
Assume you have shown that f=ln is continuous at 1.
We will use the following relation, that holds for any x0>0
ln(x0+h)=ln(x0(1+hx0))=lnx0+ln(1+hx0).
For an (ε,δ) proof: fix any x0>0, and choose any ε>0. Let δ1 be such that
|lnx−ln1|≤ε
whenever |x−1|≤δ1 (this exists by continuity of ln at 1). Now, set δdef=x0δ1.
For any x>0 such that |x−x0|≤δ, we have by (1)
\begin{align} \lvert \ln x - \ln x_0\rvert &= \lvert \ln (x_0+\underbrace{(x-x_0)}_{"h"}) - \ln x_0\rvert = \left\lvert \ln\left( 1+\frac{x-x_0}{x_0}\right)\right\rvert\\ &= \left\lvert \ln\left( 1+\frac{x-x_0}{x_0}\right) - \ln 1\right\rvert \leq \varepsilon \end{align}
the last inequality since \left\lvert\frac{x-x_0}{x_0}\right\rvert \leq \frac{\delta}{x_0} = \frac{x_0\delta_1}{x_0} = \delta_1.
So \ln is continuous at x_0.
No comments:
Post a Comment