Alright, scratch everything below the line. Let me present one cohesive question not marred by repeated edits.
The limit lim exists iff for every \epsilon>0 there is a \delta>0 such that |f(x)-L|<\epsilon when 0<|x-a|<\delta.
Thus, \lim_{x\to0}\sin\left(\frac1x\right) does not exist because, being that it oscillates infinitely near 0, there is no \epsilon,\delta.
On the other hand, with the limit\lim_{x\to0}\frac{\sin\left(x\sin\left(\frac1x\right)\right)}{x\sin\left(\frac1x\right)}\\\lim_{x\to0}x\sin\left(\frac1x\right)=0\\y=x\sin\left(\frac1x\right)\\\lim_{y\to0}\frac{\sin y}{y}=1\\\lim_{x\to0}\frac{\sin\left(x\sin\left(\frac1x\right)\right)}{x\sin\left(\frac1x\right)}=1
this proof can be shown. However, since \sin\left(\frac1x\right) oscillates infinitely, by the same definition of limit we used to show the above, the limit does not exist. How do I resolve this discrepancy?
Answer
A useful thing to know about limits, is that if you are evaluating limit of the form \lim_{x \to a} f(g(x)), and you know that \lim_{x \to a} g(x) = b then \lim_{x \to a} f(g(x)) = \lim_{y \to b} f(y) (assuming everything is nice and continuous). So, because you have already worked out the limit \lim_{x\to 0} x \sin\frac{1}{x} = 0, you get:
\lim_{x \to 0} \frac{\sin(x \sin\frac{1}{x})}{x \sin\frac{1}{x}} = \lim_{y\to 0}\frac{\sin y}{y} = 1
Edit
Let me be a little more precise. Suppose you know that \lim_{y \to b} f(y) = L (so for \varepsilon you have \delta_f(\varepsilon) such that if |y -b| < \delta_f(\varepsilon) you have |f(y) - L| < \varepsilon) and that \lim_{x \to a} g(x) = b (so for \varepsilon you have \delta_g(\varepsilon) such that if |x -a| < \delta_g(\varepsilon) you have |g(x) - b| < \varepsilon). I claim that then, with no extra assumption \lim_{x \to a} f(g(x)) = L. With g(x) = x \sin\frac{1}{x} and f(y) = \frac{1}{y}\sin y, this solves your problem.
The reasoning is as follows: Take \varepsilon > 0, and define \delta := \delta_g(\delta_f). I claim that if |x-a| < \delta then |f(g(x))-L| < \varepsilon. First, because |x-a| < \delta_g(\delta_f(\varepsilon)), you have |g(x)-b| < \delta_f(\varepsilon). Next, because |g(x)-b| < \delta_f(\varepsilon), you have |f(g(x)) - L| < \varepsilon, as promised.
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