Now when the pendulum will be in a car moving on a circular track of radius R with a uniform speed v, the effective acceleration on it will change which was earlier only acceleration due to gravity and now there is acceleration due to gravity and centripetal acceleration both acting perpendicular to each other so net acceleration and its direction also will change, the mean position will also change and the new mean position or equilibrium position of bob of pendulum will be in direction of acceleration as shown in the figure

Now centripetal acceleration on a body moving in circular path with uniform speed is given as

a_c = v²/R

where v is the uniform speed of the body and R is the radius of circular path

acceleration due to gravity g is acting in downward direction so net acceleration is

or

i.e.

we know time period of oscillation of a pendulum is given as

Where T is the time period l is the length of the pendulum and g is acceleration due to gravity

Since here now effective acceleration acting on pendulum has changed the equation will become

Where a is the effective acceleration acting on bob of pendulum

Putting value of a we get time period of oscillation of pendulum

Where T is the time period l is the length of the pendulum which is in a car which is moving on a circular track of radius R with a uniform speed v and g is acceleration due to gravity.