Approaching the Torque and Ladder Problem

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Homework Help Overview

The discussion revolves around a torque problem involving a ladder, focusing on the forces acting on it and the conditions for equilibrium. Participants are exploring the implications of the ladder's mass not being given and the behavior of the pivot point as the ladder slides.

Discussion Character

  • Exploratory, Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • Participants discuss the appropriate pivot point for analyzing torques and question whether the pivot point can move if the ladder slides. There is an exploration of the forces acting on the ladder, including friction and normal forces, and the conditions required for the ladder to remain stationary.

Discussion Status

Some participants have provided guidance on analyzing the forces and torques involved, suggesting that the forces at play must be balanced for the ladder to not slip. There is ongoing clarification regarding the components of forces and the correct application of torque principles.

Contextual Notes

Participants are navigating assumptions about the ladder's mass and the definitions of forces involved, such as the normal force and friction. There is also a discussion about the axes used for analyzing the problem, which may affect the interpretation of forces.

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Homework Statement


wcEDaVN.png


Homework Equations


F = μ FN

τ = r F

The Attempt at a Solution


how do I approach this problem? Mass isn't given. And If i set the top of the ladder to be the pivot point, the pivot point will move vertically downwards if the ladder slides - is that even allowed?
 
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If the ladder does not slip, the pivot point is also in rest. Collect all the forces and all the torques. What is the condition that the ladder does not start to move?
 
ehild said:
If the ladder does not slip, the pivot point is also in rest. Collect all the forces and all the torques. What is the condition that the ladder does not start to move?
dEtntjD.png


does this look correct?
 
goonking said:
dEtntjD.png


does this look correct?
No.
First, what is "Fgy"? The horizontal component of the gravitational force?!
Secondly, what force stops the ladder from slipping (until it does)?
 
haruspex said:
No.
First, what is "Fgy"? The horizontal component of the gravitational force?!
Secondly, what force stops the ladder from slipping (until it does)?
Force of the wall should equal force of friction.
 
Is the x-axis horizontal, and the y-axis vertical? I think, you mean Fg the force of gravity. It acts at the centre of mass of the ladder, not at the ends. What is its direction? What are the x and y components?

The normal force at the wall is not the same as the normal force from the ground.

And you completely ignored the force of friction at the ground.
 
ehild said:
Is the x-axis horizontal, and the y-axis vertical? I think, you mean Fg the force of gravity. It acts at the centre of mass of the ladder, not at the ends. What is its direction? What are the x and y components?

The normal force at the wall is not the same as the normal force from the ground.

And you completely ignored the force of friction at the ground.
mg = FN at the bottom of the ladder.

so Force of wall = force of friction since ladder doesn't move.

Fwall = Ffriction = μ FN = μ mg

torques : Torque of wall pushing ladder should equal torque of ladder at the center of mass.
let's pick the bottom of the ladder as the pivot point since the ladder doesn't move.
Fwall⋅ d ⋅sin 55.2 = mg ⋅ d/2 ⋅ cos 55.2

plugging in μ mg for Fwall

μ mg ⋅ d ⋅sin 55.2 = mg ⋅ d/2 ⋅ cos 55.2

canceling out mg and d from both sides, μ should come out to be 0.347
 
It looks correct.
 

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