Solving Static Equilibrum Homework: Can a Man Reach the Top?

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Homework Help Overview

The problem involves a ladder leaning against a frictionless wall, with a man climbing it. The scenario explores static equilibrium, focusing on the conditions under which the ladder may slip as the man ascends. The key aspects include the ladder's angle, the man's position, and the static friction between the ground and the ladder.

Discussion Character

  • Exploratory, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the analysis of forces acting on the ladder, including normal forces and friction. Questions arise regarding the necessity of demonstrating calculations for the second part of the problem, particularly whether to present findings through equations or statements.

Discussion Status

Some participants affirm the correctness of the initial analysis and seek clarification on how to approach the second part of the question. There is an ongoing exploration of the conditions required for the ladder to remain stable as the man climbs.

Contextual Notes

The problem assumes a frictionless wall and specifies a coefficient of static friction for the ground, which may influence the analysis of the ladder's stability. The discussion reflects on the implications of these assumptions for the solution.

abramsay
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I need an assessment on the homework before I submit it.

Homework Statement



A Ladder of length L and negligible mass leans again a vertical wall, making an angle θ with the horizontal. A work man of mass M climbs the ladder a distance x from the bottom along the length of the ladder. Assuming the wall is completely frictionless, but the ground possesses a coefficient of static friction µ,
(a ) how far up the ladder can the man climb before it slips along the ground?
(b) Is it possible for the man to climb to the top of the ladder without slippage occurring?


Homework Equations





The Attempt at a Solution



Let N1, N2 and Fs be the normal reaction from the wall, the ground and the frictional force respectively.
ƩFx=Fs+(-N1)= 0 ⇒Fs=N1
ƩFy=N2+(-Mg)= 0 ⇒N2=Mg
Taking moment about B,
Ʃԏ=N1(Lsinθ)+(-MgLcosθ)x/L=0
N1Lsinθ=xMgcosθ
N1= xMgcosθ/Lsinθ
⇒Fs=xMgcosθ/Lsinθ= µ_s N2
µ_s=Fs/N2= xMgcosθ/MgLsinθ=xcosθ/Lsinθ
Let y be the fraction of the ladder the man climbs before slipping occurs
Fs=N1 and N2=Mg
N1Lsinθ-MgyLcosθ=0
N1= MgyLcosθ/Lsinθ
But Fs= µ_s N2
xcosθMg/Lsinθ=MgyLcosθ/Lsinθ
y=x/L
 
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Your analysis is correct so far. Is there a question you wish to ask?
 
kuruman said:
Your analysis is correct so far. Is there a question you wish to ask?

Ok.

The second part:
(b) Is it possible for the man to climb to the top of the ladder without slippage occurring?
Do you think I have to show that with my workings or say it in a statement.
 
abramsay said:
Ok.

The second part:
(b) Is it possible for the man to climb to the top of the ladder without slippage occurring?
Do you think I have to show that with my workings or say it in a statement.
Both. Use your equations to find what the minimum coefficient of static friction ought to be so that the ladder does not slip no matter how far up the ladder the man climbs.
 

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