This proof and others I've looked up for $$ \lim_{x\to c}\frac{1}{g(x)} = \frac{1}{L} \quad\text{assuming $L$ and $\lim_{x\to c}g(x) \neq 0$ }$$
pick $\epsilon$ at $\frac{|L|}{2}$
$$0<|x−a|<\delta_1 \rightarrow |g(x)−L|<\frac{|L|}{2}$$
and at $\frac{|L|^2\epsilon}{2}$
$$0<|x−a|<\delta_2 \rightarrow |g(x)−L|<\frac{|L|^2\epsilon}{2}$$
This works out later in the proof when we are able to multiply $\frac{1}{|L|}$ by the reciprocal of the first equation, $\frac{2}{|L|}$, by the second equation $\frac{|L|^2\epsilon}{2}$ giving us $\epsilon$:
My question is, why do we pick epsilon at $\frac{|L|}{2}$ and $\frac{|L|^2\epsilon}{2}$, when we could (I think) pick them at $|L|$ and $|L|^2\epsilon$, which should later provide:
$$\frac{1}{|L|} \cdot \frac{1}{|L|} \cdot |L|^2\epsilon = \epsilon.$$
My understanding is the $\epsilon$ can be any real number greater than 0, and, $|L|$ must be a positive number, so why not use the combo above.. what rule is being broken or ignored?
Is it possibly because of this step? If we choose $\epsilon$ at $|L|$ instead of $|L/2|$ it seems impossible to complete this step:
This would imply though that there are an infinite number of epsilons, different recripocal fractions you could take to prove so long as you avoid the $|L|$ cancelling situation here. $\frac{|L|}{2}$ is the simplest fraction that works, so it makes sense they chose that.