For a car moving along a circular path without skidding outwards, the centripetal force required is provided by the frictional force between the tires and the road.
The maximum frictional force is given by \( f_{max} = \mu N \), where \( \mu \) is the coefficient of friction and \( N \) is the normal force.
On a level road, the normal force \( N \) is equal to the gravitational force \( mg \), where \( m \) is the mass of the car and \( g \) is the acceleration due to gravity.
So, \( f_{max} = \mu mg \).
The centripetal force required for circular motion with velocity \( v \) and radius \( r \) is \( F_c = \frac{mv^2}{r} \).
For the car not to skid, the centripetal force must be less than or equal to the maximum frictional force:
\( \frac{mv^2}{r} \le \mu mg \)
\( v^2 \le \mu gr \)
The maximum velocity \( v_{max} \) is given by:
\( v_{max} = \sqrt{\mu gr} \)
Given:
Coefficient of friction \( \mu = 0.
5 \)
Radius of curvature \( r = 16.
2 \) m
Acceleration due to gravity \( g = 10 \) ms\(^{-2} \)
Substitute the values:
\( v_{max} = \sqrt{0.
5 \times 10 \times 16.
2} \)
\( v_{max} = \sqrt{5 \times 16.
2} \)
\( v_{max} = \sqrt{81} \)
\( v_{max} = 9 \) ms\(^{-1} \)
Now, convert the velocity from ms\(^{-1} \) to kmh\(^{-1} \):
\( v_{max} = 9 \frac{\text{m}}{\text{s}} \times \frac{3600 \text{ s}}{1 \text{ hour}} \times \frac{1 \text{ km}}{1000 \text{ m}} \)
\( v_{max} = 9 \times 3.
6 \) kmh\(^{-1} \)
\( v_{max} = 32.
4 \) kmh\(^{-1} \)