How do I find the forces acting on a ladder?

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Homework Help Overview

The discussion revolves around analyzing the forces acting on a ladder placed against a house, involving a person climbing it. The problem includes parameters such as the masses of the ladder and the person, the distances involved, and the angle of inclination. Participants are tasked with finding the normal and friction forces at the base of the ladder.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants explore various equations related to torque and forces, questioning the definitions of symbols used and the assumptions made regarding the center of mass and the components of forces. There is a focus on ensuring the correct application of lever arms in torque calculations.

Discussion Status

Some participants have provided guidance on clarifying symbols and checking assumptions, while others have confirmed the correctness of certain calculations. There are ongoing discussions about the accuracy of the results and the methods used, with no explicit consensus reached on the final values.

Contextual Notes

Participants note potential discrepancies in the interpretation of the problem statement and the calculations, particularly regarding the forces of gravity and their components. There is also mention of differing results compared to a physics textbook, indicating possible confusion or errors in the source material.

Eclair_de_XII
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Homework Statement


"To get up on the roof, a person (mass 70.0 kg) places a 6.00-m aluminum ladder (mass 10.0 kg) against the house on a concrete pad with the base of the ladder 2.00 m from the house. The ladder rests against a plastic rain gutter, which we can assume to be friction-less. The center of mass of the ladder is 2.00 m from the bottom. The person is standing 3.00 m from the bottom. Find the normal reaction and friction forces on the ladder at its base."
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Homework Equations


##\theta=cos^{-1}(\frac{1}{3})=tan^{-1}(2\sqrt{2})##
##m_0=10kg##
##s_0=\frac{2 m}{tan\theta}##
##m_1=70kg##
##s_1=\frac{3 m}{tan\theta}##
##||s||=6m##

The Attempt at a Solution


I'm choosing my lever arm to be the point at which the ladder touches the ground.

##∑|τ|=-g(m_0s_0+m_1s_1)+||s||cos\theta⋅F_r=0##
##∑F_x=-gcos\theta(m_0+m_1)-F_r+f_s=0##

##F_r=f_s-gcos\theta(m_0+m_1)##
##F_r⋅||s||⋅cos\theta=g(m_0s_0+m_1s_1)##
##F_r=\frac{g}{||s||}sec\theta(m_0s_0+m_1s_1)##
##f_s-gcos\theta(m_0+m_1)=\frac{g}{||s||}sec\theta(m_0s_0+m_1s_1)##
##f_s=gcos\theta(m_0+m_1)+\frac{g}{||s||}sec\theta(m_0s_0+m_1s_1)##

Can anyone tell me if I'm going in the right direction? Thanks.
 
Last edited:
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You have the correct approach. But I noticed a few things:

(1) It is always helpful to define the symbols that you are using. For example, I had to try to decipher your equations to decide what angle you are calling ##\theta##. Likewise for the symbols ##s_1##, ##s##, and ##s_0##.

(2) The problem states that "the center of mass of the ladder is 2.00 m from the bottom". I think this probably means that the center of mass is 2.00 m along the ladder starting from the bottom of the ladder. If they meant it the way you interpreted it, I think they would have said that the center of mass is 2.00 m above the ground. Similarly for the position of the person.

(2) You wrote the equation ##∑|τ|=-g(m_0s_0+m_1s_1)+||s||cos\theta⋅F_r=0##. Check to make sure that the expression for the lever arm for ##F_r## is correct.
 
On more thing, it looks like you have assumed that the forces of gravity have a horizontal component. Is this right?
 
TSny said:
Check to make sure that the expression for the lever arm for ##F_r## is correct.

Oh, it's ##||s||sin\theta⋅F_r##, right? ##F_r## acts horizontally, so the lever arm is the vertical component of ##||s||##.

TSny said:
Is this right?

Forgive me. I think I should treat the ladder as a point mass for the summation of forces expression.

##∑F_x=f_s-F_r=0##
##∑F_y=-(m_0+m_1)g+F_N=0##
 
Eclair_de_XII said:
Oh, it's ##||s||sin\theta⋅F_r##, right? ##F_r## acts horizontally, so the lever arm is the vertical component of ##||s||##.

##∑F_x=f_s-F_r=0##
##∑F_y=-(m_0+m_1)g+F_N=0##
That all looks good.
 
##\theta=cos^{-1}(\frac{1}{3})##
##m_0=70 kg##
##s_0=3 m##
##m_1=10kg##
##s_1=32 m##

##∑|τ|=-gcos\theta(m_0s_0+m_1s_1)+F_r(||s||sin\theta)=0##
##F_r=(\frac{g}{||s||})(cot\theta)(m_0s_0+m_1s_1)=(\frac{9.8\frac{m}{s^2}}{6m})(\frac{1}{2\sqrt{2}})((70kg)(3m)+(10kg)(2m))=133 N##
##∑F_x=f_s-F_r=0##
##f_s=F_r=133N##

##∑F_y=F_N-g(m_0+m_1)=0##
##F_N=g(m_0+m_1)=784N##
 
I tried to do a quick check and it looks like your results for Fr and FN are correct.
 
Is that right? I probably need a new physics problem book because it says that ##F_N=784N## but ##f_s=376N##.
 
I just repeated the sum of the moment equation and once again calculated 132.8 N for Fr, which is equal to -fs, since those are the only 2 horizontal forces. So I think that is the correct answer unless you and I are both doing something fundamentally wrong.
 
  • #10
It looks like the book incorrectly used (Fr)(||s||)(cosθ), instead of (Fr)(||s||)(sinθ) when calculating the moment from force Fr.
 

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