In fact, we can say slightly more almost immediately. First, let's codify the result that we used in the proof of the theorem above.
First, we'll show Euler's (ingenious but rather iffy) argument to highlight points where we need to drive deeper. To begin, Euler knew that
\begin{equation*}
\sin x = x - \frac{x^3}{3!} + \frac{x^5}{5!} - \ldots,
\end{equation*}
and so
\begin{equation*}
\frac{\sin x}{x} = 1 - \frac{x^2}{3!} + \frac{x^4}{5!} - \ldots.
\end{equation*}
He wants to factor this “polynomial” using the fundamental theorem of algebra as
\begin{equation*}
\frac{\sin x}{x} = (x - \pi)(x+\pi)(x - 2\pi)(x + 2\pi)\ldots,
\end{equation*}
but he can't, as this has no hope of converging in the infinite product. Instead, he defines terms of the form \((1 \pm \frac{x}{k\pi})\) - after all, these terms vanish at the same set of zeros. Making the rather large leap that the function is determined by its zeros and a single value (as in the case of a polynomial), Euler writes
\begin{align*}
\frac{\sin x}{x} \amp= (1 - \frac{x}{\pi})(1 + \frac{x}{\pi})(1 - \frac{x}{2\pi})(1 + \frac{x}{2\pi})\ldots\\
\amp= (1 - \frac{x^2}{\pi^2})(1 - \frac{x^2}{4\pi^2})(1 - \frac{x^2}{9\pi^2})\ldots
\end{align*}
which at least has a shot of converging. He then notices that a pattern emerges as you start formally multiplying out this product.
\begin{equation*}
(1 - \frac{x^2}{\pi^2})(1 - \frac{x^2}{4\pi^2}) = 1 - (\frac{1}{\pi^2} + \frac{1}{2^2 \pi^2}) x^2 + O(x^4),
\end{equation*}
and
\begin{equation*}
(1 - \frac{x^2}{\pi^2})(1 - \frac{x^2}{4\pi^2})(1 - \frac{x^2}{9\pi^2}) =1 - (\frac{1}{\pi^2} + \frac{1}{2^2 \pi^2} + \frac{1}{3^2 \pi^2}) x^2 + O(x^4).
\end{equation*}
He makes the leap that
\begin{equation*}
\prod_{n=1}^\infty (1 - \frac{x^2}{k^2 \pi^2}) = 1 - (\sum_{k=1}^\infty \frac{1}{k^2 \pi^2})x^2 + O(x^4).
\end{equation*}
Now, still with the underlying assumption that all of this converges and makes sense, he compares the coefficients of \(x^2\) in his two power series to get
\begin{equation*}
- (\sum_{k=1}^\infty \frac{1}{k^2 \pi^2}) = \frac{-1}{3!},
\end{equation*}
which is just
\begin{equation*}
\zeta(2) = \sum_{k=1}^\infty \frac{1}{k^2} = \frac{\pi^2}{6}.
\end{equation*}