$$\begin {aligned}\pi^{-s/2}\Gamma(s/2)\zeta(s)=&\pi^{-(1-s)/2}\Gamma((1-s)/2)\zeta(1-s) \\ \zeta(0) =&\frac{\pi^{-1/2}\Gamma(1/2)\zeta(1)}{\pi^{0}\Gamma(0)}=\frac{\zeta(1)}{\Gamma(0)}\end {aligned}$$
so that $\zeta(0)$ is the ratio of the residues of $\zeta(s)$ at $s=1$ end $\Gamma(s)$ at $s=0$. The latter is just $1$ since
$$\lim_{s\rightarrow 0} s\Gamma(s) = \Gamma(1)=1.$$
To calculate the residue of $\zeta(s)$ at $s=1$, I simply used the expression, proved in Stein & Shakarchi Complex Analysis p. 171
$$\pi^{-s/2}\Gamma(s/2)\zeta(s) = \frac 1{s-1} -\frac1s +\frac12\int_1^\infty(u^{(-s/2)-1/2}+u^{s/2-1})[\theta(u)-1]du$$
I argued that since the integral on the RHS is holomorphic at $s=1$, the residue of the LHS at $s=1$ must be $1$ (the coefficient of the first fraction). Since $\pi^{-1/2}\Gamma(1/2)$ cancel each other, it should be the case that $\operatorname {res}_{s=1} \zeta(s)=1$, but then my argument says that $\zeta(0) = 1$. Where did I miss the $-\frac12$?