What Is the Minimum Coefficient of Friction Needed for a Sphere Against a Wall?

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Homework Help Overview

The problem involves a uniform sphere supported by a rope against a vertical wall, with the goal of determining the minimum coefficient of friction required between the sphere and the wall. The setup includes specific dimensions and forces acting on the sphere, including tension, friction, and gravitational forces.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the derivation of equations related to the forces acting on the sphere, particularly questioning the initial equation relating torque and friction. There is an exploration of the pivot point used for torque calculations and its implications on the frictional force.

Discussion Status

The discussion is ongoing, with participants examining the correctness of their initial assumptions and calculations. Some have offered insights into the torque analysis, while others are reconsidering their approaches based on feedback and observations.

Contextual Notes

There is a noted discrepancy between the calculated coefficient of friction and a reference value from the textbook, prompting further investigation into the assumptions made during the problem-solving process.

rpthomps
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Homework Statement


A uniform sphere of radius R is supported by a rope attached to a vertical wall,as shown in the figure. The point where the rope is attached to the sphere is located so a continuation of the tope would intersect a horizontal line through the sphere’s centre a distance R/2 beyond the centre, as shown. What is the smallest possible value for the coefficient of friction between wall and sphere.

wtf2q.png


Homework Equations


##T_x=F_N\\\\F_f+T_y+Mg\\\\\Sigma\tau=0=\frac{1}{2}RMg-RF_f\\\\tan30^o=\frac{T_x}{T_y}\\\\F_f=\mu F_N##

The Attempt at a Solution



okr3sz.png


##\frac { 1 }{ 2 } RMg=RF_{ f }\\ \\ \frac { 1 }{ 2 } Mg=\mu F_{ N }\\ \\ \\ \frac { 1 }{ 2 } Mg=\mu T_x\\ \\ ##

equation 1
##F_f+\frac{T_x}{tan30^o}=Mg\\\\\mu F_N+\frac{T_x}{tan30^o}=Mg\\\\\mu T_x+\frac{T_x}{tan30^o}=Mg\\\\##

equation 2Solve equation 1 for Tx and substitute into equation 2.##\mu=\frac{1}{tan30^o}=1.73…##Back of the book says 0.87
 
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How do you get your first equation, ##\frac 12 RMg=RF_f##?
 
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I used the end of the rope where it connects to the sphere to be the pivot position and set all the torques to 0. This equated the Frictional Force with the Center of Mass but now that I see it, that would be that the Frictional force is 1.5 R away not R. I will try and recalculate it based on this, I think I did this before though...checking..
 
yup, that was it.

Thanks again.
 

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