Consider a vehicle of weight mg moving on circular level road of radius r with constant velocity v. While taking the round, the tyres of the car tend to leave the road and move away from the centre of curve. In such case, forces of friction f1 and f2 will act inward towards the two tyres. If R1 and R2 are the normal reactions of ground on the tyres, then
f1 = μs R1 and f2 = μs R2
where μs = coefficient of static friction
Now total frictional force,
f = μs R1 + μs R2
f = μs (R1 + R2)
f = μs R
where R = reaction of ground on the vehicle.
As total frictional force f cannot exceed μs R, hence f ≤ μs R
This frictional force will provide the necessary centripetal force f = mv2/r
Hence the maximum speed, vmax = √μsrg
If the vehicle is driven at a speed greater than vmax, then it will skid and goes off the road in a circle of radius greater than r as the maximum available friction is inadequate to give required centripetal force.