Circular motion is a motion in which a body travels a definite distance along a circular path. Let’s learn about the meaning of motion, circular motion, the types of circular motion, its properties, and how to derive a velocity of a body performing the circular motion.
Motion can be defined as any object or body changing its position in its surroundings concerning time. When an object is moved from its initial position in a particular interval of time, it is said to be under motion.
Motion is a very common concept that we come across in day-to-day life. It can be said that every component of the universe performs some form of motion. Some examples can be cars moving on the road, boats sailing in the ocean, birds flying in the sky, and the earth moving around the sun. All these bodies can be said to be performing a motion.
Speed = DistanceTime
The SI unit of speed is ‘m/s.’ It is a scalar quantity.
Velocity (v) = DisplacementTime
The SI unit of velocity is ‘m/s’.
Acceleration (a) = VelocityTime
The SI unit of acceleration is ‘m/s2’.
Force= m x a (mass x acceleration)
The SI unit of force is ‘N’ (Newton).
Momentum (P) = m x v (Mass x Velocity)
The SI unit of Momentum is ‘Kg m/s.’
A body is said to be in Circular Motion when the body moves at a definite distance from a fixed point along a circular path. The fixed point acts as the centre, and the fixed distance acts as the radius of the circular path the body is travelling.
A body performing Circular Motion constantly changes its direction of movement, which is tangent to the circular path at that point. For any body performing a circular motion, centripetal force is a must, which acts along the radius towards the centre.
This force providing the acceleration to the object/body is,
Fc(Centripetal force) = mv2R
Here m is mass of object
v is the linear velocity of particle
R is radius of circular path
The motion of a car on a level road:
Let us assume a car is moving on a level road, with mass ‘m’ and ‘g’ as the acceleration due to gravity acting upon it.
When the car is taking a turn on the road, a total of three forces act simultaneously on the car:
The car is moving in the horizontal plane, so there is no vertical movement which means there is no acceleration in the vertical direction (Along X-Axis).
Therefore,
N – mg = 0
N = mg (i)
When a car moves along the curved road, centripetal force is required to perform this circular motion. This centripetal force is provided by the frictional force (f) between the wheels of the car and the surface of the road.
Since the centripetal acceleration is only produced in the case of static friction, and as we know, static friction opposes the motion.
According to this analogy,
f = mv2R μsN
∴ v2 μsNRm= μsRg (N=mg)
∴ v = μsRg
We can conclude that velocity is independent of the car’s mass according to this derived equation.
Based on the direction and rate of rotation of the body, Circular Motion can be further subdivided into two types:
When the rate of rotation of the object/body remains constant concerning time, it is said to be performing Uniform Circular Motion. In other words, the speed of rotation remains constant along the circular path. For every object performing Circular Motion, some acceleration is provided by the centripetal force, which acts along the path of radius towards the centre. Hence, the acceleration is perpendicular to the direction of velocity at every point of motion.
When the rate of rotation of the object/body changes concerning time, it is said to be performing Non-Uniform Circular Motion. The speed of the rotation changes at every point in the circular path.
Angular Displacement (Δθ) =ΔSR
Angular Velocity (Δω) = Δθt
Angular Acceleration (Δ) = Δωt
Let us see a few Uniform Circular Motion examples.
Hope this gives you an understanding of circular motion, its properties, and various terms related to it.