Well, a simple asymptotic is (by probability) $\sqrt{m/3}$
This can be obtained by considering that we want the expectation of
$w = \sqrt{x_1^2 +... x_m^2} = \sqrt{y_1 +... y_2}$
with $y_i = x_i^2$, so that $\displaystyle f_y(y) = \frac{y^{1/2}}{2}$, and $E(y)=1/3$, $\sigma^2(y)=4/45$.
Then, the variable $z = (y_1 +... y_2)/m$ will approach a gaussian with $\mu_z = 1/3$, $\sigma^2_z=\frac{4}{m 45}$.
And $E(w) = \sqrt{m} E(\sqrt{z})$ which in first approximation is $E(w) \approx \sqrt{m} \sqrt{\mu_z} = \sqrt{m/3}$
One can get better aproximations with the higher moments, for example:
$E(w) \approx \mu_z^{1/2} - \frac{1}{8}\mu_z^{-3/2}\sigma_z^2 =
\sqrt{\frac{m}{3}} - \frac{1}{30}\sqrt{\frac{3}{m}} = \sqrt{\frac{m}{3}}\Bigl(1 - \frac{1}{10 m}\Bigr)$
(errors aside).
Are you looking for something more precise?
UPDATE: By a similar reasoning, the additional problem (if I understand it right) gives $\displaystyle \sqrt{\frac{4}{3 m}}$
UPDATE2: About the second order approximation:
In general, when we want to find moments of $Y=g(X)$ with $g(.)$ nonlinear but smooth, we can do a Taylor expansion around its media:
$Y = g(\mu_x) + g'(\mu_x)(X-\mu_x) + \frac{1}{2!} g''(\mu_x)(X-\mu_x)^2 + ...$
So that
$\displaystyle \mu_y = E(Y) = g(\mu_x) + g''(\mu_x)\frac{\sigma_x^2}{2} +...$
This, BTW, justifies the intuitive notion that $E(g(.)) \approx g(E(.))$ if the variance is small (equality applies only if $g(.)$ is linear, of course) and allows to estimate (and to some extent correct) the error of the approximation.