What Is the Angle of Incline for a Sphere Rolling Without Slipping?

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Homework Help Overview

The problem involves a uniform solid sphere rolling down an incline without slipping, with a given linear acceleration of 0.22g. The goal is to determine the angle of the incline with respect to the horizontal.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants discuss the relationship between linear acceleration and the angle of incline, referencing the equation a = gsin(theta). There are attempts to set up equations for both translational and rotational motion, with some questioning the role of friction in the context of rolling without slipping.

Discussion Status

Some participants have provided insights into the necessary equations and the importance of static friction in the scenario. There is ongoing exploration of how to relate translational and rotational motion, with multiple interpretations of the equations being discussed.

Contextual Notes

Participants note that the incline cannot be frictionless due to the rolling condition, and there are references to the need for further clarification on the role of static friction and its maximum value in the equations being set up.

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Homework Statement



A uniform solid sphere rolls down an incline without slipping. If the linear acceleration of the center of mass of the sphere is 0.22g, then what is the angle the incline makes with the horizontal?

Homework Equations



a=gsin(theta)

The Attempt at a Solution



The only thing I can think of is acceleration down an incline=gsin(theta). Since we have a=0.22g, I made gsin(theta)=0.22g and thereby arcsin(0.22) should give me theta...but it doesn't...any help please??
 
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hejo said:
The only thing I can think of is acceleration down an incline=gsin(theta).
That's the acceleration down an incline if the only force acting parallel to the incline is gravity, for example when a box slides down a frictionless incline. Hint: Since the sphere rolls without slipping, the incline cannot be frictionless. (Solve for the acceleration using Newton's 2nd law twice; once for translation, once for rotation.)
 
Okay. I set up my equation for translational motion to be ma=mgsin(theta) - (coefficient of friction)*mgcos(theta). So a=gsin(theta) - gcos(theta)*(coefficient of friction).

Is that right? I don't understand how I can get acceleration from rotational motion.
 
hejo said:
Okay. I set up my equation for translational motion to be ma=mgsin(theta) - (coefficient of friction)*mgcos(theta). So a=gsin(theta) - gcos(theta)*(coefficient of friction).

Is that right?
No, it's not quite right. Since there's no slipping, the relevant friction is static friction. And static friction can be anything up to a maximum of μN. So you can't just set it equal to that maximum value. Just call the friction "F" and continue.
I don't understand how I can get acceleration from rotational motion.
That friction force also exerts a torque on the sphere which produces an angular acceleration. Set up an equation for that. (You can relate the angular acceleration to the translational acceleration.)

Note that you have two unknowns--the friction and the acceleration--but you also have two equations.
 

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