Minimum linear velocity attained by sphere

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Homework Help Overview

The problem involves a sphere of mass M and radius R moving on a rough surface with a coefficient of friction μ. The sphere has an initial linear velocity v and angular velocity ω, and the discussion centers on determining the conditions under which the sphere attains a minimum linear velocity while rolling with slipping.

Discussion Character

  • Exploratory, Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • Participants discuss the equations governing the motion of the sphere, including the effects of friction and the relationship between linear and angular velocities. Questions arise regarding the interpretation of "minimum linear velocity" and the presence of a missing minus sign in the equations.

Discussion Status

The discussion is ongoing, with participants exploring different interpretations of the equations and the physical meaning of the terms involved. Some guidance has been offered regarding the direction of acceleration and the implications of the signs in the equations, but no consensus has been reached.

Contextual Notes

Participants are examining the implications of the sphere's initial conditions, specifically the requirement that v must be greater than ωR, and how this affects the equations of motion. There is also a focus on the definitions and assumptions related to friction and acceleration in the context of the problem.

utkarshakash
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Homework Statement


A sphere of mass M and radius R is moving on a rough fixed surface, having co-efficient of friction μ, with a velocity v towards right and angular velocity ω clockwise. It will attain a minimum linear velocity at time (take v>ωR)

The Attempt at a Solution


Since v>ωR the sphere rolls with slipping. So frictional force will act in the backward direction. Using the equation \int \tau dt = \int dL where τ=μmgR.

\mu mgRt= \frac{2}{5} mR^2 (\omega &#039; - \omega) \\<br /> <br /> \mu mg = m \frac{dv}{dt} \\<br /> <br /> \mu gt = (v&#039; - v)<br />

Using the relation v'=ω'R and solving the above two equations I get
t= 2(v-ωR)/3μg. But the correct answer has 7 in the denominator.
 
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utkarshakash said:
\mu mg = m \frac{dv}{dt}
There is a minus sign missing.

I don't see why this point is called "minimum linear velocity" - it is the point where the sphere stops slipping.
 
mfb said:
There is a minus sign missing.

I don't see why this point is called "minimum linear velocity" - it is the point where the sphere stops slipping.

Why there should be a minus sign? Since friction acts backwards, so is the acceleration. Hence both minus cancels out. Are you trying to say that since velocity is decreasing that's why dv/dt should carry a '-' with it?
 
Acceleration is backwards, but as you write your equation both sides are positive, so v increases. You can use a negative v everywhere, but then things get really confusing and the initial v>ωR does not work.
 

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