Optimal Ladder Position for Painting: Friction and Wall Conditions Explained

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The discussion centers on determining the distance a painter can climb a ladder before it slips, considering the ladder's angle with the floor and the friction between the ladder and the floor. The forces acting on the ladder include the painter's weight and the reaction forces at the wall and floor. The moments are balanced to find the critical point of slipping, leading to the conclusion that the distance x is proportional to the ladder's length d and the coefficient of friction μ. As the angle θ increases, the distance x also increases, indicating that a steeper angle allows for greater climbing distance before slipping occurs. The final formula derived is x = d·μ·tan(θ).
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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 coefficent 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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