Ladder leaned against a wall; forces

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The discussion revolves around analyzing the forces acting on a 5m ladder leaning against a frictionless wall. Participants work through creating a force diagram, identifying forces such as gravity, friction, and normal forces, while ensuring the system is in static equilibrium. Key equations discussed include torque calculations, with emphasis on determining the line of action and direction of torques for each force. The final equations derived show that the frictional force equals the normal force from the wall, leading to the conclusion that FNwall can be expressed as (mg 2.5cosθ)/(5sinθ). The conversation highlights the importance of understanding torque direction and equilibrium conditions in solving the problem.
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Homework Statement


There is a 5m ladder leaned against a wall, making an angle of θ with the ground. The ground is rough (getting at friction), and the wall is frictionless. Here's an ASCII attempt:

|\
|..\
|...\5
|...\
|...θ\

We want to make a force diagram for the ladder, then find the value of the forces acting on it.

Dealing purely with variables aside from the 5m length.

Homework Equations


Sum of F = ma
Torque = F x l

The Attempt at a Solution


I'm fine with the force diagram, I think. You've got gravity downwards, the force of friction to the left, some normal force upwards, and some normal force by the wall directly to the right.

As for what they are...

Force of gravity = mg
FNfloor = mg?
Ff = ?
FNwall = ?
Ff = FNwall

I think FNfloor = mg, and Ff = FNwall, because this is an instance of static equilibrium, so sum of F = 0. Is that correct? And how do I account for torque?
 
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For the torque, pick any convenient point and calculate the moments about it.
 
Ok, I'll pick the bottom of the ladder, where it meets the ground.

For force of g: T = mg x 2.5cos θ
For force of FNwall: T = ? x 5cos θ
For the other two forces, T = 0

I'm not sure where that brings me, though.
 
kffd said:
Ok, I'll pick the bottom of the ladder, where it meets the ground.

For force of g: T = mg x 2.5cos θ
For force of FNwall: T = ? x 5cos θ
Not quite. Try that second one again. And pick a consistent direction for positive torque. And you already have a name for the unknown (the '?').
For the other two forces, T = 0

I'm not sure where that brings me, though.
Is there any rotational acceleration?
 
haruspex said:
Not quite. Try that second one again. And pick a consistent direction for positive torque. And you already have a name for the unknown (the '?').

Is there any rotational acceleration?

Another go for FNwall: 5sin θ x Ff

Here's a diagram to help explain what I'm not getting:

||\
||..\
||...\-->
||...\
v|...θ\

Vertical arrow is what I now think torque for FNwall should be, 5sin θ x Ff. Horizontal is torque for g. Is that correct? If so, is one positive and the other negative? I just don't get that, but that's what I'm led to think given your advice.

EDIT: No rotational acceleration.
 
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kffd said:
Another go for FNwall: 5sin θ x Ff

Here's a diagram to help explain what I'm not getting:

||\
||..\
||...\-->
||...\
v|...θ\

Vertical arrow is what I now think torque for FNwall should be, 5sin θ x Ff. Horizontal is torque for g. Is that correct?
No, a torque is neither horizontal nor vertical. In the present case it is clockwise or counterclockwise.
The force FNWall is clearly horizontal, but what is the distance from its line of action to the base of the ladder? Is it 5 cos θ, 5 sin θ, 2.5 cos θ or 2.5 sin θ? Does its torque act clockwise?
 
haruspex said:
No, a torque is neither horizontal nor vertical. In the present case it is clockwise or counterclockwise.
The force FNWall is clearly horizontal, but what is the distance from its line of action to the base of the ladder? Is it 5 cos θ, 5 sin θ, 2.5 cos θ or 2.5 sin θ? Does its torque act clockwise?

Ok, good news is I knew that about torque, at least. That's what I didn't understand, how a "torque" could work if it were simply a line. (We have only discussed it as clockwise/counterclockwise.)

|\-LOA->
|..\...|
|...\...|
|...\.|
|...θ\

I think that is the line of action, and the vertical is what I'm trying to find, so I'm going to say 5sinθ is the answer. (Whoops, that's actually what I meant last time, but I'm still not positive whether it's correct.) I don't think it's 2.5 anything because the force is not applied to the ladder's center of gravity.

I think that moment (I think it's a moment) acts clockwise. If I made the LOA a tangent line to a circle, it would "point" in the clockwise direction, which is my rationale. It would follow that the moment caused by Fg is counterclockwise.
 
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It looks good, so what is the net torque then?

ehild
 
Well, net torque must be 0 if it's in equilibrium. So,
mg 2.5cosθ - 5sinθ Ff = 0

I used a minus just to indicate that one direction is negative. (I arbitrarily picked clockwise.)

Going off of that:
mg 2.5cosθ = 5sinθ Ff
Ff = (mg 2.5cosθ)/(5sinθ)
Ff = FNwall, so
FNwall = (mg 2.5cosθ)/(5sinθ)

Did I bring it home?
 
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  • #10
kffd said:
Well, net torque must be 0 if it's in equilibrium. So,
mg 2.5cosθ - 5sinθ Ff = 0

I used a minus just to indicate that one direction is negative. (I arbitrarily picked clockwise.)

Going off of that:
mg 2.5cosθ = 5sinθ Ff
Ff = (mg 2.5cosθ)/(5sinθ)
Ff = FNwall, so
FNwall = (mg 2.5cosθ)/(5sinθ)

Did I bring it home?

Ok so far, but you can simplify it.

ehild
 
  • #11
= 0.5 mg cotθ

I think that's all. Thanks a lot, ehild and haruspex; I've been out of school sick recently, going through this problem with me really did help me catch up. Once I'm a bit more learned when it comes to physics, I'll do my diligence to help out some other people on here, too. :)
 
  • #12
Nice plans! Go ahead.:smile:

ehild
 
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