Free NEET Physics resource
Circular Motion: Kinematics
A particle can move at constant speed and still accelerate because its velocity changes direction. Understand the picture first; use the equations after that.
1. Start with the picture
For a circle of radius r, the arc length covered through an angle θ (in radians) is s = rθ. Displacement is the straight-line chord, not the arc. After one complete revolution, distance is 2πr but displacement is zero.
Teacher's checkpoint: On the same rigid rotating disc, all points have the same angular speed. Points farther from the axis have greater linear speed.
At every instant, velocity is tangent to the circle; centripetal acceleration points towards the centre. The direction of the velocity changes even when its magnitude stays constant.
2. Acceleration: radial and tangential
In uniform circular motion (UCM), the acceleration is radially inward. After a turn through angle Δθ at constant speed v, the magnitude of the change in velocity is:
Quarter turn: |Δv| = √2v. Half turn: |Δv| = 2v. Full turn: |Δv| = 0.
Average is not instantaneous: Over a full revolution, average velocity and average acceleration are both zero, although instantaneous acceleration is nonzero.
When speed changes in non-uniform circular motion, radial acceleration changes the direction of velocity, while tangential acceleration changes its magnitude.
Common mistake: Centripetal acceleration is the inward component of acceleration. The net inward force comes from real forces such as friction, tension or gravity; centripetal force is not an additional force to add.
3. Five worked examples
01 · Frequency to acceleration
Radius 0.50 m, frequency 2 Hz. Find ω, v and ac.
Reasoning: ω = 2πf = 4π rad/s; v = rω = 2π m/s; ac = ω²r = 8π² m/s².
02 · Changing direction
At a constant speed of 10 m/s, find |Δv| after a 90° turn.
Reasoning: |Δv| = 2(10)sin45° = 10√2 m/s. Constant speed does not mean constant velocity.
03 · Average versus instantaneous
Half a revolution at speed π m/s around a circle of radius 2 m.
Reasoning: Time = 2 s; displacement magnitude = 4 m. Average velocity magnitude = 2 m/s. |Δv| = 2π m/s, so average acceleration magnitude = π m/s². Compare instantaneous ac = π²/2 ≈ 4.93 m/s².
04 · Two perpendicular components
At an instant, r = 2 m, v = 6 m/s, at = 4 m/s². Find net acceleration.
Reasoning: ac = 36/2 = 18 m/s². Net magnitude = √(18² + 4²) = √340 ≈ 18.44 m/s².
05 · Points on the same disc
One point at 25 cm from the axis moves at 5 m/s. Find the speed at 10 cm.
Reasoning: ω = 5/0.25 = 20 rad/s. The second speed is 20 × 0.10 = 2 m/s.
4. Practice: 10 NEET-style questions
Choose one answer for each question. The final two use statement-based and assertion-reason formats.
- After a complete revolution in UCM, which quantity is zero?
- A particle moves in a circle of radius 0.50 m with a period of 2 s. Its speed is:
- At constant speed v, |Δv| after a quarter-turn is:
- Two points are at radii 2r and 5r on one rigid rotating disc. Their linear speed ratio is:
- At fixed radius, doubling the speed multiplies centripetal acceleration by:
- Over a complete UCM revolution, average acceleration magnitude is:
- If ac = 18 m/s² and at = 4 m/s², net acceleration magnitude is:
- Viewed face-on, a wheel spins anticlockwise. Its angular-velocity vector points:
- Statements: For UCM, I: speed is constant. II: acceleration vector is constant.
- Assertion: UCM has nonzero acceleration despite constant speed. Reason: Velocity direction changes continuously.
Reveal answers with reasons
- A — Net displacement is zero.
- A — v = 2πr/T.
- B — Vector change after 90° is √2v.
- C — At common ω, v ∝ r.
- B — ac ∝ v² at fixed r.
- A — Final velocity equals initial velocity.
- B — Radial and tangential components are perpendicular.
- D — Right-hand rule for a face-on view.
- B — In UCM, inward acceleration changes direction.
- A — Changing velocity direction causes acceleration.
What should you study next?
Move from kinematics to the forces behind circular motion: centripetal force, banking of roads, and vertical circles.