Chapter 6: Problem 29
While the disc skids, its translational and angular acceleration are related as (A) \(a=R \alpha\) (B) \(a=\frac{1}{4} R \alpha\) (C) \(a=\frac{1}{2} R \alpha\) (D) \(a=2 R \alpha\)
/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none}
Learning Materials
Features
Discover
Chapter 6: Problem 29
While the disc skids, its translational and angular acceleration are related as (A) \(a=R \alpha\) (B) \(a=\frac{1}{4} R \alpha\) (C) \(a=\frac{1}{2} R \alpha\) (D) \(a=2 R \alpha\)
All the tools & learning materials you need for study success - in one app.
Get started for free
For a particle in uniform circular motion, the acceleration \(\vec{a}\) at a point \(P(R, \theta)\) on the circle of radius \(R\) is (here \(\theta\) is measured from the \(x\)-axis) [2010](A) \(-\frac{v^{2}}{R} \cos \theta \hat{i}+\frac{v^{2}}{R} \sin \theta \hat{j}\) (B) \(-\frac{v^{2}}{R} \sin \theta \hat{i}+\frac{v^{2}}{R} \cos \theta \hat{j}\) (C) \(-\frac{v^{2}}{R} \cos \theta \hat{i}-\frac{v^{2}}{R} \sin \theta \hat{j}\) (D) \(\frac{v^{2}}{R} \hat{i}+\frac{v^{2}}{R} \hat{j}\)
Four point masses, each of value \(m\), are placed at the corners of a square \(\mathrm{ABCD}\) of side \(\ell\). The moment of inertia of this system about an axis passing through \(A\) and parallel to BD is [2006] (A) \(3 m \ell^{2}\) (C) \(2 m \ell^{2}\)
Which of the following statement is false for a particle moving in a circle with a constant angular speed? [2004] (A) The velocity vector is tangent to the circle. (B) The acceleration vector is tangent to the circle. (C) The acceleration vector points towards the centre of the circle. (D) The velocity and acceleration vectors are perpendicular to each other.
While the disc skids, its translational and angular acceleration are related as (A) \(a=R \alpha\) (B) \(a=\frac{1}{4} R \alpha\) (C) \(a=\frac{1}{2} R \alpha\) (D) \(a=2 R \alpha\)
A wheel is rotating at 900 rpm about its axis. When power is cut off it comes to rest in 1 minute. The angular retardation is \(\frac{\pi}{n} \mathrm{rad} / \mathrm{s}^{2}\), then the value of \(n\) is.
What do you think about this solution?
We value your feedback to improve our textbook solutions.