Sunday, 9 September 2018

calculus - Why "$limlimits_{xrightarrow infty} frac{x+sin x}{x}$ does not exist" is not an acceptable answer?



Find the limits:



$\lim\limits_{x\rightarrow \infty} \frac{x+\sin x}{x}$



Since the numerator and denominator tends to infinity as $x$ tends to infinity, then applying Lhopital's rule:




$\lim\limits_{x\rightarrow \infty} \frac{x+\sin x}{x} = \lim\limits_{x\rightarrow \infty} \frac{1 + \cos x}{1}$



since $\cos x$ has no limit as $x$ tend to infinity ($\cos x$ oscillates between $-1$ and $1$), I conclude that the limit of $\frac{x + \sin x }{x}$ as $x$ tends to infinity does not exist too.



Why is this answer wrong (the correct answer is 1) and at what point should I have realized that I made a mistake and abort this solution and try something else? Is $\frac{1 + \cos x}{1}$ considered an indeterminate form?


Answer



L'Hospital rule says that if $\lim_{x \to \infty} f(x)=\lim_{x \to \infty}g(x)= \infty$ and $\lim_{x \to \infty} \frac{f'(x)}{g'(x)}$ exists then $\lim_{x \to \infty} \frac{f(x)}{g(x)}$ exists and is the same thing.



L'Hospital doesn't say anything about what happens if $\lim_{x \to \infty} \frac{f'(x)}{g'(x)}$ doesn't exists, and the converse of L'H is not true.




To understand why this happens, you have to look at the proof of L'H. The proof of L'H uses the mean value theorem to deduce that there exists some $c_x$ which depends on $x$ such that
$c_x \to \infty$ and
$$\frac{f(x)}{g(x)}= \frac{f'(c_x)}{g'(c_x)}$$



Now, $\lim_x \frac{f'(x)}{g'(x)}$ calculates the limit using ALL $x$, while $\lim_x\frac{f'(c_x)}{g'(c_x)}$ calculates the limit using only SOME of the $x$. If the limit exists for all $x$, then it does exists for some of the $x$, but the other way around it is not true.



In your example, what happens most probably is that while
$$\lim\limits_{x\rightarrow \infty} \frac{1 + \cos x}{1}$$
does not exist, when you apply the MVT you get

$$\frac{x+\sin x}{x} =\frac{1 + \cos c_x}{1}$$
and each $c_x$ is very very close to some $\frac{\pi}{2}+2k \pi$. Moreover, when $x$ goes to infinity the approximation $c_x \sim \frac{\pi}{2}+2k \pi$ becomes better and better.


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