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Q.What is centripetal acceleration? Derive an expression for centripetal acceleration of a particle in uniform circular motion along a plane. What will be the direction of the velocity and acceleration at any instant? (1+3+1=5)

Nagaland NbseNagaland Board of School Education (Class XI) 2025Subjective· 5mImportance★★★★★
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Centripetal acceleration is the radially-inward acceleration that continuously changes the direction (not the speed) of a particle in uniform circular motion; it is derived here from the time-derivative of the position vector, and its direction is shown to be always perpendicular to the (tangential) velocity.

  1. What is centripetal acceleration? In uniform circular motion, a particle moves with constant speed vv along a circle of radius rr, but its velocity direction keeps changing. This continuous change of direction requires an acceleration, directed at every instant towards the centre of the circle — this is called centripetal ('centre-seeking') acceleration.
  2. Derivation of the expression for centripetal acceleration: Let the particle move on a circle of radius rr in the xy-plane, with angular speed ω\omega (constant, for uniform circular motion). At time tt, its position vector is: r⃗(t)=rcos⁡(ωt) i^+rsin⁡(ωt) j^\vec r(t) = r\cos(\omega t)\,\hat i + r\sin(\omega t)\,\hat j Velocity: v⃗(t)=dr⃗dt=−rωsin⁡(ωt) i^+rωcos⁡(ωt) j^\vec v(t) = \dfrac{d\vec r}{dt} = -r\omega\sin(\omega t)\,\hat i + r\omega\cos(\omega t)\,\hat j Its magnitude is ∣v⃗∣=rωsin⁡2(ωt)+cos⁡2(ωt)=rω=v|\vec v| = r\omega\sqrt{\sin^2(\omega t)+\cos^2(\omega t)} = r\omega = v (constant, as expected for uniform circular motion), and v=rωv=r\omega. Acceleration: a⃗(t)=dv⃗dt=−rω2cos⁡(ωt) i^−rω2sin⁡(ωt) j^=−ω2 r⃗(t)\vec a(t) = \dfrac{d\vec v}{dt} = -r\omega^2\cos(\omega t)\,\hat i - r\omega^2\sin(\omega t)\,\hat j = -\omega^2\,\vec r(t) So the acceleration vector is directed exactly opposite to the position vector r⃗\vec r (which points from the centre to the particle) — i.e. a⃗\vec a points from the particle towards the centre of the circle. Its magnitude: ∣a⃗∣=ω2r|\vec a| = \omega^2 r. Using v=rω⇒ω=v/rv=r\omega \Rightarrow \omega = v/r: ac=ω2r=(vr)2r=v2ra_c = \omega^2r = \left(\dfrac{v}{r}\right)^2 r = \dfrac{v^2}{r} …

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