Step 1: Forces acting on the vehicle.
For a vehicle moving on a banked curve, the forces acting are:
Gravitational force (\( mg \)).
Normal reaction force (\( N \)).
Frictional force (\( f \)).
The net force provides the necessary centripetal force for circular motion.
Step 2: Resolving forces.
The component of the normal reaction along the radius provides the centripetal force:
\[
N \sin \theta = \frac{m v^2}{r},
\]
where \( v \) is the speed, \( r \) is the radius of the curve, and \( \theta \) is the banking angle.
Step 3: Frictionless case (Safety speed).
For the safety speed, assume friction is negligible. The normal force's component balances the centripetal force:
\[
v^2 = r g \tan \theta.
\]
Solve for \( v \):
\[
v = \sqrt{r g \tan \theta}.
\]
Step 4: Final Answer.
The safety speed is:
\[
\boxed{V = \sqrt{r g \tan \theta}}.
\]