Optimal Ladder Position for Painting: Friction and Wall Conditions Explained

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Homework Help Overview

The discussion revolves around a physics problem involving a ladder leaning against a wall, focusing on the conditions under which the ladder begins to slip as a painter climbs it. The subject area includes concepts of friction, moments, and forces in static equilibrium.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the setup of force diagrams and moments acting on the ladder, questioning the correctness of their expressions for moments and forces. They explore the relationship between the distance climbed by the painter and the conditions of the ladder's slipping.

Discussion Status

There are multiple interpretations of the moments involved, with participants attempting to clarify their calculations and assumptions. Some have proposed expressions for the distance x in terms of the ladder length d and the coefficient of friction, while others are questioning the accuracy of their formulations.

Contextual Notes

Participants are working under the constraints of a homework problem, which may limit the information available and the methods they can use. The problem involves both rough and smooth surfaces, leading to different conditions for the ladder's stability.

Myrddin
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Ladder Problem (urgent)

A light of negligible mass and length d is supported on a rough floor and leans against a smooth vertical wall makeing an angle (theta) with the floor. The coefficient of friction between the ladder and floor is M.

If a painter climbs the ladder up distance x, what value of x is when the ladder begins to slip? And how far can he climb is the floor is smooth and the wall is rough?

Attempt at solution:

Have a force diagram with mass of painter Mg downwards, with anti clockwise moment xMgcos(theta) taking base of the ladder as a pivot.

clockwise moment from the top off ladder reaction from the wall R2.
= R2cos(theta)d (i think)

R2 = Mmg (i think)

So both moments ---> Mmgcos(theta)d = mgcos(theta)x

so from this x = dM which doesn't seem right..
 
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Myrddin said:
A light ladder of negligible mass and length d is supported on a rough floor and leans against a smooth vertical wall making an angle θ (theta) with the floor. The coefficient of friction between the ladder and floor is M. (I'd rather use μ .)

If a painter climbs a distance x up the ladder, at what value of x does the ladder begin to slip? And how far can he climb is the floor is smooth and the wall is rough?

Attempt at solution:

Have a force diagram with mass of painter Mg downwards, with anti clockwise moment x·m·g·cos(θ) taking base of the ladder as a pivot.

clockwise moment from the top off ladder reaction from the wall R2.
= R2·cos(θ)·d (i think)
This should be R2·sin(θ)·d .
R2 = μ·m·g (i think)

So both moments ---> μ·m·g·cos(theta)d = m·g·cos(theta)x

so from this x = d·μ which doesn't seem right.
R2 looks OK.

Just fix the anti-clockwise moment.
 


Anti clock wise moment should equal, dR2sin(theta)? so ---> dMmgsin(theta)
this gives anticlock wise = clockwise

So dMmgsin(theta) = xmgcos(theta)
so x = dMmgsin(theta) / mgcos(theta) = dMtan (theta)?
 


x = d·μ·tan(θ) looks good to me.

x is proportional to d and μ. x increases as θ increases.
 

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