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Centripetal Acceleration , Centripetal Force

Sujoy Das
15 Feb 0 0

Definition:

Centripetal acceleration is the acceleration of a particle moving in a circle, directed towards the center of the circle.

  • Even if speed is constant, velocity changes because direction changes.

  • Acceleration points toward the center (radially inward).


🔹 Formula:

ac=v2r=rω2a_c = \frac{v^2}{r} = r \omega^2ac=rv2=rω2

Where:

  • vvv = linear speed along circular path

  • rrr = radius of the circle

  • ω\omegaω = angular speed (rad/s)

Key Points:

  • SI unit = m/s²

  • Direction = toward center

  • Magnitude depends on speed and radius


🔵 2️⃣ Centripetal Force (FcF_cFc)

✅ Definition:

Centripetal force is the net force that keeps a body moving in a circular path, directed toward the center.

  • Without this force, the body would move in a straight line (Newton’s first law).

  • It is not a new kind of force — it can be tension, gravity, friction, or normal force.


🔹 Formula:

Fc=mac=mv2r=mrω2F_c = m a_c = \frac{m v^2}{r} = m r \omega^2Fc=mac=rmv2=mrω2

Where:

  • mmm = mass of particle

  • vvv = linear speed

  • rrr = radius of circle

  • ω\omegaω = angular speed

Key Points:

  • SI unit = Newton (N)

  • Points toward the center

  • Acts perpendicular to motion, so no work is done by centripetal force


🔹 Examples

Situation Centripetal Force Source
Stone tied to string whirled Tension in string
Car on circular track Friction between tires and road
Planets around Sun Gravitational force
Ball on a curved table (loop) Normal force from surface

🔹 Important Tips

  1. Centripetal acceleration depends on speed squared → faster = more acceleration.

  2. Smaller radius → more acceleration and force needed.

  3. Centripetal force is always toward the center.

  4. Work done by centripetal force = 0 (perpendicular to motion).


🔹 Quick Summary Table

Concept Symbol Formula Direction Unit
Centripetal acceleration aca_cac v2/rv^2/rv2/r or rω2r\omega^2rω2 Toward center m/s²
Centripetal force FcF_cFc mv2/rm v^2/rmv2/r or mrω2m r \omega^2mrω2 Toward center N
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