Skip to content
Answer the following · Q15

Q.Define angular velocity. Show that the centripetal force on a particle undergoing uniform circular motion is −mω2r⃗-m\omega^2\vec{r}.

Maharashtra MsbshseTextbookSubjectiveImportance★★★★★est
58% · 15/26 Questions
🔒 Locked · start free trial →

You're viewing a preview — the full solution, concept, methods & PYQ mapping are locked.

Start your 14-day free trial to unlock the full solution →

Angular velocity ω is a vector quantity equal to the rate at which the radius vector (from the centre of rotation to the particle) sweeps out angle, ω=dθdt\omega = \dfrac{d\theta}{dt}, with its direction along the axis of rotation (given by the right-hand rule) — although for motion confined to one plane, as in this chapter, only its magnitude (angular speed) is generally used. For a particle in UCM at radius r, write the position vector as r⃗=rcos⁡(ωt)i^+rsin⁡(ωt)j^\vec{r}=r\cos(\omega t)\hat{i}+r\sin(\omega t)\hat{j} (starting on the x-axis at t=0). Differentiating once gives velocity v⃗=−rωsin⁡(ωt)i^+rωcos⁡(ωt)j^\vec{v}=-r\omega\sin(\omega t)\hat{i}+r\omega\cos(\omega t)\hat{j}, and differentiating again gives acceleration a⃗=−rω2cos⁡(ωt)i^−rω2sin⁡(ωt)j^=−ω2[rcos⁡(ωt)i^+rsin⁡(ωt)j^]=−ω2r⃗\vec{a}=-r\omega^2\cos(\omega t)\hat{i}-r\omega^2\sin(\omega t)\hat{j}=-\omega^2\left[r\cos(\omega t)\hat{i}+r\sin(\omega t)\hat{j}\right]=-\omega^2\vec{r}. The …

Unlock everything free for 14 days

  • Full step-by-step solutions
  • Concept-first explanations
  • Methods, shortcuts & mistakes
  • PYQ mapping + timed mock tests

Full access for 14 days. No credit card required.