Calculating Tension and Reactive Force in a Leaning Ladder System

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Homework Help Overview

The discussion revolves around a physics problem involving a ladder leaning against a wall, where participants are tasked with calculating the tension in a rope and the reactive force at the base of the ladder. The scenario includes specific measurements and conditions, such as the ladder's length, mass, and the presence of a person climbing it.

Discussion Character

  • Exploratory, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • Participants explore the forces acting on the ladder, including the tension in the rope, the weight of the ladder, and the normal forces. Questions arise regarding the correct angles to use in calculations and the identification of all forces involved.

Discussion Status

Some participants have offered guidance on identifying missing forces and correcting angles in the equations. There is an ongoing exploration of different interpretations of the problem setup and the forces at play, with no explicit consensus reached on the correct approach yet.

Contextual Notes

Participants mention specific constraints such as the frictionless nature of the wall and floor, as well as the need to maintain static equilibrium. There is also a reference to the coefficient of static friction in a related problem, which adds complexity to the discussion.

Geoff
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Hello.
I got the following question.
a 12 m ladder, whose mass is 20 kg is leaning agains a wall with its base being 6 m from the wall and the angle between the floor and the ladder is 60 degrees. The wall and the floor are frictionless. So we tie a rope 0.5 m from the base of the ladder to the wall to keep the ladder from sliding. A 72 kg person climbs 3 quarters up the ladder and stps. We need to find the tension in the rope and the reactive force in the floor.
For the force on the floor it is easy, u just get the mass and multiply it by 9.i8 to get the total force up in order for thsi to be static equalibirum.
Now i was trying to find the tension in the rope, so i did this:
i set the place where the ladder is tied to the rope to be the pivot and did this:
0=-(9-0.5)sin 30 * 72 *9.8 -5.5 sin30 * 20 * 9.8 + sin 30*11.5 Fx
So i solved for Fx adn i get:
600. The correct answer is 380. The reason i used 30 is because that is the angle between the force applied and the arm as opposed to use 60 which is the angle between the floor and the ladder.
any ideas where i made the mistake?
Thx
 
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First what if Fx? If it is the tension in the rope then it won't appear in the equation as it is applied at the pivot point.
If Fx is the reaction of the wall, then the angle is not 30, it would be 60.

Second, there are 5 forces on the ladder and you missed 1/2 in the equation. (Vertical up reaction from floor, weight of ladder at center, weight of person, tension of rope and horizontal reaction from the wall)

As you said, the normal reaction from floor = (72+20)*9.8. To calculate th e tension in rope, take the point at rope as pivot,
0=-(9-0.5)sin 30 * 72 *9.8 -5.5 sin30 * 20 * 9.8 + sin 60*11.5 Fx - 0.5 * sin30 * 92*9.8
 
thx a lot, i think i get it now
i applied what i learned to yet another ladder question:D
Here it is:
a ladde length 5 m and whose weight is 400 N is leaning agains frictionless wall. coefficient of static friction between the ladder and the ground is 0.46. I need to determine the greatest distance the ladder can be placed without slipping.
The prolbme here is that i don;t know the correct answer, but i do have a solution, and it got me:
Angle between the ladder and the floor being 47.4 degrees, therefor the distance is 3.39 m from the wall.
Could someone check it out and tell me if my solution gave me the correct answer or not? If not then how do u solve this?
I did this
0=Weight * half distance cos theta -Total distance * sin theta*Frictional force.
from this i got
tan theta=1000/5*Frictional force.
And i know
that Ff= 0.46 *400. tehrefor i got the angle and so on.
So any ideas if this is right?
 
I assume you are considering the pivot where the ladder touches the wall. You have forgotten one more force, the normal reaction of wall. A component of that will be reflected in the equation.
Also, both frictional force and weight of ladder tend to "rotate" in the same direction; and normal reaction in the opposite.

Include these and try again.
 

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