How Does Ladder Stability Change with Different Forces and Distances?

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The discussion focuses on the stability of a ladder under various forces and distances, analyzing the forces acting at the bottom and top of the ladder. The participant calculates the forces, concluding that the force at the top is 133 N and the force at the bottom is approximately 795 N. There is confusion regarding the direction of the force, F_w, and whether it has vertical components, particularly in relation to a "frictionless rain gutter." The conversation explores the implications of different angles and surfaces on the forces acting on the ladder, emphasizing the importance of understanding normal forces and their directions. Overall, the exchange highlights the complexities of analyzing ladder stability in physics.
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Homework Statement


image.jpg


Where it says ''from the bottom'' I assumed it's referring to a distance along the ladder. So:
image.jpg


Data:

##w_{ladder} = 98.0\ N##

##w_{person} = 686\ N##

##d_1 = 4\sqrt(2)\ m##

##d_2 = 1\ m##

##d_3 = 2/3\ m##

Homework Equations



##\sum \tau = 0##

##\sum F = 0##

The Attempt at a Solution


[/B]
Diagram:

image.jpg
image.jpg


I chose my pivot point to be the bottom of the ladder. Hence, torques due to normal force ##N## and friction ##f## are zero. ##ccw## is positive and ##cw## is negative.

##0 = w_pd_2 + w_ld_3 - F_wd_1##

##F_wd_1 = w_pd_2 + w_ld_3##

##F_w = \frac{w_pd_2 + w_ld_3}{d_1} = \frac{686\ N \cdot 1.00\ m + 98.0\ N \cdot 2/3\ m}{4\sqrt{2}\ m} = 133\ N##

##F_w = f = 133\ N##

Then:

##N = w_p + w_l = 686\ N + 98.0\ N = 784\ N##

The force at the top of the ladder is just ##133\ N##.
The force at the bottom is ##\small{\sqrt{N^2+ f^2} = \sqrt{ (784\ N)^2+ (133\ N)^2} = 795\ N}##. Doubt: this magnitude, whether it's correct or not, acts along the ladder, right? (as a tension would?).

The textbook's solutions are ##126\ N## and ##751\ N##, respectively. It seems I haven't missed anything, so I don't know where the mistake is.
 
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Which direction does Fw point ?
 
BvU said:
Which direction does Fw point ?

To the right.

And in a cw direction about the pivot point.
 
No vertical component ?
 
BvU said:
No vertical component ?

Components of ##F_w##? Mmm, It didn't occur to me that there could be vertical components there. Has that of a ''frictionless rain gutter'' something to do with it?
 
It seems that I also forgot to take ##F_w## into account when finding the force at the bottom.
 
Jazz said:
Components of ##F_w##? Mmm, It didn't occur to me that there could be vertical components there. Has that of a ''frictionless rain gutter'' something to do with it?
Frictionless says there will only be a normal force. Normal means perpendicular to the surface of contact. What direction will that be? You should assume the ladder projects slightly beyond the point of contact with the gutter.
 
Jazz said:
Components of ##F_w##? Mmm, It didn't occur to me that there could be vertical components there. Has that of a ''frictionless rain gutter'' something to do with it?
Consider a more extreme case where the ladder is at 45 degrees (or even less) wrt the ground. Would it lean ON the gutter, as well as against the gutter ?
 
I think I'm getting the idea. It would be something like this:

gutter.jpg
However I'm not sure what is the correct direction that ##F_w## takes.

I think the sharp corner of the gutter can be viewed as a fulcrum. Should ##F_w## act perpendicular to the edge of the gutter, as bisecting it? If that were the case, my drawing wouldn't be totally accurate. Would it be in that direction, independent of the angle that the ladder makes with the ground?.
 
  • #10
Jazz said:
Should ##F_w## act perpendicular to the edge of the gutter, as bisecting it?
No. It might help to rotate the problem around to a more familiar set-up. Imagine a table on flat level ground, but the legs of the table are sharp wedges, meeting the ground at some odd angle. Which way would the normal force act?
More generally, as I wrote, normal means perpendicular to the contact plane. I'm not sure how contact planes are defined generally, but if either surface is differentiable then it will be the tangent plane which passes through the point of contact. Taking the ladder uprights to be rectangular in section, they have a differentiable surface. Or if you take them to be arbitrarily thin rods then it must be a plane containing that rod and containing the edge line of the gutter - there is only one such. Sounds complicated, but the underlying idea is fairly intuitive.
 
  • #11
Another approach: ladder pushes against gutter. In which direction ? Gutter pushes back, opposite direction (no friction).

If there were a rubber hose between the two, how would it compress ? To a vertical ellipse ? Or to an ellipse with the long axis parallel to the ladder ?
 
  • #12
I would say to an ellipse with the long axis parallel to the ladder, which would mean that the force exerted by the gutter on the ladder is perpendicular to it.

In the other case (leaning against a wall), the wall becomes the differentiable surface and the rubber hose would compress parallel to it. It makes sense.

If the gutter weren't frictionless, friction would act parallel to the ladder's structure, right?
 
  • #13
Jazz said:
I would say to an ellipse with the long axis parallel to the ladder, which would mean that the force exerted by the gutter on the ladder is perpendicular to it.

In the other case (leaning against a wall), the wall becomes the differentiable surface and the rubber hose would compress parallel to it. It makes sense.

If the gutter weren't frictionless, friction would act parallel to the ladder's structure, right?
Yes, I agree with all of that.
 
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