Step 1: Write the standard equation of trajectory.
The trajectory of a projectile is given by
\[
y=x\tan\theta-\frac{gx^2}{2u^2\cos^2\theta}
\]
where
\[
u=\text{velocity of projection}
\]
and
\[
\theta=\text{angle of projection}
\]
Step 2: Compare the given equation with the standard form.
Given equation:
\[
y=\frac{x}{\sqrt{3}}-\frac{x^2}{60}
\]
Comparing the coefficient of \(x\),
\[
\tan\theta=\frac{1}{\sqrt{3}}
\]
Hence,
\[
\theta=30^\circ
\]
Now,
\[
\cos30^\circ=\frac{\sqrt{3}}{2}
\]
Therefore,
\[
\cos^2 30^\circ=\frac{3}{4}
\]
Step 3: Compare the coefficient of \(x^2\).
From the trajectory equation,
\[
\frac{g}{2u^2\cos^2\theta}=\frac{1}{60}
\]
Substituting
\[
g=10
\]
and
\[
\cos^2\theta=\frac{3}{4},
\]
we get
\[
\frac{10}{2u^2\left(\frac{3}{4}\right)}=\frac{1}{60}
\]
\[
\frac{10}{\frac{3u^2}{2}}=\frac{1}{60}
\]
\[
\frac{20}{3u^2}=\frac{1}{60}
\]
Cross multiplying,
\[
20\times 60=3u^2
\]
\[
1200=3u^2
\]
\[
u^2=400
\]
\[
u=20\ \text{ms}^{-1}
\]
Step 4: Final conclusion.
Hence, the velocity of projection is
\[
\boxed{20\ \text{ms}^{-1}}
\]