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In circular motion:
1. velocity remains constant.
2. acceleration remains constant.
3. speed remains constant.
4. none of above

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Correct Answer - Option 3 : speed remains constant.

Explanation:

Circular motion:

  • The motion of a body moving around a fixed point in a circular path is known as circular motion.

Example:

  1. The motion of the moon around the earth.
  2. The motion of a satellite around its planet.
  • The direction of motion changes continuously in a circular motion, therefore the circular motion is an accelerated motion.

Uniform circular motion:

  • If the angular velocity of the body remains constant during circular motion then it is called uniform circular motion. 
  • Speed of body is constant with change in direction.
  • Uniform circular motion is an accelerated motion because the direction of motion of the body continuously changes.


Non-Uniform circular motion:

  • If the angular velocity of the body changes during circular motion then it is called non-uniform circular motion.

Linear acceleration:

  • The acceleration involved in linear motion is called linear acceleration.
  • Here the acceleration is only due to the change in speed and no acceleration due to change in direction, therefore no radial component of acceleration.

Circular acceleration:

  • The acceleration involved in a circular motion is called angular acceleration.
  • In a circular motion, the acceleration experienced by the body towards the centre is called the centripetal acceleration which can be resolved into two-component.
  • A radial component and a tangential component depending upon the type of motion.

Radial acceleration (ar):  The acceleration of the object along the radius, directed towards the centre is called radial acceleration.

\(a_r=\frac{v^2}{r}=ω^2r\)

Where ar = radial acceleration, v = speed, r = radius of circular motion, ω = angular velocity

Tangential acceleration (at): The tangential component is defined as the component of angular acceleration tangential to the circular path.

\(a_t=\alpha r\)

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