If you remove all of the parts involving $\delta$ from the epsilon-delta definition, then you indeed get something like the first proposition:
For every $\varepsilon > 0$, $\lvert f(x) - L \rvert < \varepsilon$.
This would imply (by the first proposition) that $f(x) = L$.
(It would not imply that $\lvert f(x) - L \rvert = \varepsilon$. Think again: how is that equation relevant to anything else in the question?)
If $f(x) = L$ for all $x$ then $x$ is a constant function. So a definition like this would only be useful for finding the limit of a constant function, which is hardly even worth defining.
That's why we need $\delta$. Moreover, it's why we need to introduce "some" $\delta$ and why we need to write "some" $\delta$ after we write "for all $\varepsilon$",
because when it is written that way it allows us to specify a different $\delta$ for each $\varepsilon$ whenever we want to.
In the epsilon-delta definition, therefore,
there is never a time when we choose two particular numbers $a$ and $b$, such as
$a = f(x)$ for some $x$ and $b = L$,
and say that $\lvert a - b \rvert < \varepsilon$, that is,
$\lvert f(x) - L \rvert < \varepsilon$, for every $\varepsilon$.
We always have $\delta$ getting in the way of that notion.
Remember that in the definition of a limit,
$\lvert f(x) - L \rvert < \varepsilon$ only has to be true when
$0 < \lvert x - a \rvert < \delta$.
This implies that no matter what $x$ you might want to choose at which to evaluate $f(x)$, there is always a $\delta$ that forbids you to use that $x$.
Obviously, $x = a$ is ruled out, and if you choose any other $x$,
then $\delta = \frac12\lvert x - a \rvert$ will rule out that $x$ too.
Indeed, in a typical proof of a limit by the epsilon-delta definition,
we are always looking at an ever-shrinking set of values of $x$
for smaller and smaller values of $\varepsilon$,
there is no value of $x$ that is always in that set,
and there is no particular $f(x)$ that needs to satisfy
$\lvert f(x) - L \rvert < \varepsilon$ for every $\varepsilon$.