Can A Painter Safely Stand on a Ladder?

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Homework Help Overview

The discussion revolves around a physics problem involving a painter standing on a ladder. The ladder has a specified mass and length, is positioned at a certain angle, and is subject to static friction. The goal is to determine the maximum mass of the painter that allows the ladder to remain stable as she climbs a specified distance up the ladder.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the forces acting on the ladder, including normal forces, static friction, and weights. There is an exploration of torque calculations and equilibrium conditions. Some participants express confusion about whether all forces and torques have been accounted for, leading to questions about the setup and assumptions made in the problem.

Discussion Status

Participants are actively engaging with the problem, sharing their calculations and reasoning. Some have provided guidance on identifying missing forces and torques, while others are clarifying their understanding of equilibrium conditions. There is a recognition of potential algebraic errors in calculations, and some participants are exploring different interpretations of the problem setup.

Contextual Notes

There is an emphasis on ensuring all forces are considered, particularly in relation to the pivot point chosen for torque calculations. Participants are also navigating the complexities of the problem's algebraic aspects, which may be contributing to confusion in their results.

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A painter wishes to know whether or not she can safely stand on a ladder. The ladder has a mass M1 = 12 kg which is uniformly distributed throughout its length L = 7.4 m. The ladder is propped up at an angle theta = 53o. The coefficient of static friction between the ground and the ladder is mus = 0.42, and the wall against which the ladder is resting is frictionless. Calculate the maximum mass of the painter for which the ladder will remain stable when she climbs a distance d = 6.6 m up the ladder. (The painter's mass might be so low that only Lilliputian painters can safely ascend the ladder.)

I think that I've gotten the problem but my answer is wrong. Just curious if anyone could take the time to look over my formulas and work.

M_L = 12 kg
L= 7.4m
Theta = 53 degrees
Static Friction (mus) = .42

d = 6.6m

I drew my force diagrams and such, I have a the Normal force of the wall against the top of the ladder, The normal force of the ground against the bottom of the ladder (straight up), Static friction pointing towards the wall. The weight of the ladder at the center of mass of the ladder. And the weight of the Painter/Man.
For this to be in equilibrium, Net Torque and Net force must equal Zero.

I suppose this problem is more tough on the algebraic side?
Here's some of my work.
Positive torque - counterclockwise
Negative torque - Clockwise
Goal - To find the mass of the maximum mass of the man.

Torques:
(L/2)*M_L*g Cos(theta)
d*M_man*g*Cos(theta)

X force N_w= mus*Normal Force
Y force (M_man + M_ladder)g = Normal Force

-L*mus*(M_man + M_L)g*sin(Theta)

So the formula i made to find the mass of the man was this.

(L/2)*M_L*g Cos(theta) + d*M_man*g*Cos(theta) - L*mus*(M_man + M_L)g*sin(Theta) = 0

After plugging in numbers i got
M_man(38.92 - 291.9019) = - 261.8617529

I got 1.035 kg. This is incorrect.. What am i doing wrong?
 
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Well, perhaps you should list all of the forces that you need to account for. There are five (you're only accounting for four of them).
 
I drew my force diagrams and such, I have a the Normal force of the wall against the top of the ladder, The normal force of the ground against the bottom of the ladder (straight up), Static friction pointing towards the wall. The weight of the ladder at the center of mass of the ladder. And the weight of the Painter/Man.

Normal force of wall against ladder
Normal foce of ground against ladder
Static Friction between ladder and ground
Weight of Man
Weight of Ladder.

Friction and Normal for of wall against ladder cancel out because net force is = 0 and they are the only x forces.

Haven't I accounted for them all?
 
But the torque for friction, and the torque for the normal force on the wall might not cancel.
 
Don't they have to to make Tnet= 0?

How would you find them with the information given?
 
Last edited:
Maybe this matters, I have my pivot point at the bottom of the ladder.
 
PhysicsPhun said:
Maybe this matters, I have my pivot point at the bottom of the ladder.

Right, so the torque due to friction with the floor will be zero, but the torque due to the normal force of the wall will not.

You should be able to figure out the mangitude of the (maximum) normal force that the wall can exert since [tex]F_{net x}=0[/tex].
 
Didn't I do that?

-L*mus*(M_man + M_L)g*sin(Theta)

That's torque.. nm.

The normal force would just be the .. mus(Mass of man + Mass of Ladder)*g...?
 
Last edited:
Ugh.. I gues the text just makes things hard to read...

Let's see:

[tex]\tau_{ladder}=\frac{L}{2} M_{ladder} g \cos \theta \approx 3.7 \times 12 \times 9.81 \times 0.601 \approx 261[/tex]
[tex]\tau_{man}=d M_{man} g\cos \theta \approx 6.6 M_{man}\times 9.81 \times 0.601 \approx 39 M_{man}[/tex]
[tex]\tau_{wall}\geq -\mu_s g (M_{ladder}+M_{man})L \sin\theta[/tex]
[tex]\approx -.42 \times 9.81 \times (M_{man}+12) 7.4 \times 0.798 \approx - 24.3 M_{man} - 292[/tex]
now
[tex]\tau_{ladder}+\tau_{man}\leq -\tau_{wall}[/tex]
so
[tex]261 + 39 M_{man} \leq 24.3 M_{man} + 292[/tex]
[tex]31 \geq 15 M_{man}[/tex]
[tex]2.0 \geq M_{man}[/tex]

Not sure if that's the right answer, but:

Your result doesn't match the second to last equation, but the equation would, except for some grouping problems, indicate that you lost one of the terms in the algebra.
 
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Well that's actually the right answer, thanks. But where did 24.3M_man come from?
I was just getting 292M_man, as opposed to 292 +24.3M_man.. Grr I think it was just math, i didn't distribute to the M_man.

Thanks a lot for ALL your help : )
 

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