First, technically speaking, given only $X \sim N(\mu_1, \sigma_1^2), Y \sim N(\mu_2, \sigma_2^2)$ and $\operatorname{Corr}(X, Y) = \rho$ does not imply the joint distribution of $(X, Y)$ is bivariate normal $N_2(\mu_1, \mu_2, \sigma_1^2, \sigma_2^2, \rho)$. Check this answer for many counterexamples. Therefore, the accepted answer actually imposed additional conditions that were not originally posted in the question.
Secondly, if we do have $(X, Y) \sim N_2(\mu_1, \mu_2, \sigma_1^2, \sigma_2^2, \rho)$, then $E[\max(X, Y)]$ indeed admits a closed-form expression, which is deduced below.
Write $E[\max(X, Y)] = \frac{1}{2}E[(X + Y) + |X - Y|]$. Under the joint normality condition, we have
\begin{align}
& X + Y \sim N(\mu_1 + \mu_2, \sigma_1^2 + \sigma_2^2 + 2\rho\sigma_1\sigma_2), \\
& X - Y \sim N(\mu_1 - \mu_2, \sigma_1^2 + \sigma_2^2 - 2\rho\sigma_1\sigma_2).
\end{align}
It thus suffices to compute $E[Z]$ and $E[|Z|]$ for a univariate r.v. $Z \sim N(\mu, \sigma^2)$. Clearly, $E[Z] = \mu$, while $E[|Z|] = \sigma E[|Z'|]$ with $Z' \sim N(\mu\sigma^{-1}, 1)$, and
\begin{align}
& E[|Z'|] = \int_{-\infty}^\infty |x|\frac{1}{\sqrt{2\pi}}e^{-\frac{1}{2}(x - \mu\sigma^{-1})^2}dx \\
=& \frac{1}{\sqrt{2\pi}}\int_0^\infty xe^{-\frac{1}{2}(x - \mu\sigma^{-1})^2}dx -
\frac{1}{\sqrt{2\pi}}\int_{-\infty}^0 xe^{-\frac{1}{2}(x - \mu\sigma^{-1})^2}dx \\
=& \left[\frac{1}{\sqrt{2\pi}}e^{-\mu^2\sigma^{-2}/2} + \mu\sigma^{-1}\Phi(\mu\sigma^{-1})\right] -
\left[-\frac{1}{\sqrt{2\pi}}e^{-\mu^2\sigma^{-2}/2} + \mu\sigma^{-1}\Phi(-\mu\sigma^{-1})\right] \\
=& \frac{2}{\sqrt{2\pi}}e^{-\mu^2\sigma^{-2}/2} + \mu\sigma^{-1}(2\Phi(\mu\sigma^{-1}) - 1).
\end{align}
Denote $\sqrt{\sigma_1^2 + \sigma_2^2 - 2\rho\sigma_1\sigma_2}$ by $\sigma_0$, then
\begin{align*}
E[|X - Y|] = \sigma_0
\left(\frac{2}{\sqrt{2\pi}}e^{-(\mu_1 - \mu_2)^2\sigma_0^{-2}/2} + (\mu_1 - \mu_2)\sigma_0^{-1}(2\Phi((\mu_1 - \mu_2)\sigma_0^{-1}) - 1)\right)
\end{align*}
and
\begin{align}
& E[\max(X, Y)] \\
=& \frac{1}{2}E[X + Y] + \frac{1}{2}E[|X - Y|] \\
=& \frac{\mu_1 + \mu_2}{2} + \frac{\sigma_0}{\sqrt{2\pi}}e^{-(\mu_1 - \mu_2)^2\sigma_0^{-2}/2} + \frac{1}{2}(\mu_1 - \mu_2)(2\Phi((\mu_1 - \mu_2)\sigma_0^{-1}) - 1) \\
=& \mu_2 + \frac{\sigma_0}{\sqrt{2\pi}}e^{-\frac{(\mu_1 - \mu_2)^2}{2\sigma_0^2}} + (\mu_1 - \mu_2)\Phi\left(\frac{\mu_1 - \mu_2}{\sigma_0}\right).
\end{align}