Dynamics - rope attached to an object

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SUMMARY

The discussion focuses on a physics problem from Halliday, Resnick, and Krane's "Physics, Fifth Edition," specifically Chapter 5, Problem 11, which involves calculating the minimum downward pull on a rope necessary to lift a heavy object using a wooden dowel. The solution requires understanding the relationship between tension (T), weight (W), and the coefficient of sliding friction (\mu) between the rope and the dowel. The derived formula for the minimum force is F_{\text{down}} = We^{\pi\mu}, emphasizing the importance of analyzing forces acting on a small segment of the rope and integrating a differential equation to solve for the normal force.

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  • Understanding of Newton's laws of motion
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  • Knowledge of differential equations
  • Ability to analyze free-body diagrams
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  • Study the derivation of the formula for tension in ropes under friction
  • Learn about free-body diagram techniques in physics
  • Explore differential equations and their applications in physics
  • Investigate the effects of varying coefficients of friction on tension
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Homework Statement



(Halliday, Resnick, Krane - Physics, Fifth Edition. Chapter 5, Problem 11.)

A massless rope is tossed over a wooden dowel of radius [itex]r[/itex] in order to lift a heavy object of weight [itex]W[/itex] off of the floor. The coefficient of sliding friction between the rope and the dowel is [itex]\mu[/itex]. Show that the minimum downward pull on the rope necessary to lift the object is

[tex]F_{\text{down}} = We^{\pi\mu}[/tex].

2UAw5.png


Homework Equations



[tex]\Sigma \vec{F} = m \vec{a}[/tex]

[tex]f = \mu N[/tex]

The Attempt at a Solution



Note that in order to lift the object, the magnitude of the tension [itex]T[/itex] in the rope must be more than or equal to the weight of the object. (That is, [itex]T \geq W[/itex].) So the rope is pulled on one end by a force of magnitude [itex]T[/itex] and on the other by a force of magnitude [itex]F_{\text{down}}[/itex]. The dowel exerts a normal force [itex]\vec{N}[/itex] on the rope, and the magnitude of the friction between the rope and the dowel is given by [itex]f = \mu N[/itex].

The problem is that I have no idea how to deal with this normal force. If I draw a diagram where [itex]\vec{f}[/itex] opposes the motion of the rope, I end up with [itex]\vec{f}[/itex] and [itex]\vec{T}[/itex] pointing in the opposite direction as [itex]\vec{F}_{\text{down}}[/itex], but [itex]\vec{N}[/itex] is perpendicular to all of those forces. The rope is obviously not moving in the direction of [itex]\vec{N}[/itex], so it seems that some unknown force is balancing the normal force out.
 
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Hint: Analyze forces acting on a small segment of the rope. You'll need to set up a (simple) differential equation and integrate to find your answer.
 

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