Find the angle theta at which the ladder leaves the wall

  • Thread starter Thread starter HiPPiE
  • Start date Start date
  • Tags Tags
    Angle Theta Wall
Click For Summary

Homework Help Overview

The discussion revolves around a physics problem involving a uniform ladder of length L leaning against a smooth wall and a smooth floor. The problem explores the conditions under which the ladder leaves the wall, including the equations of motion and the angle theta at which this occurs.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation, Assumption checking

Approaches and Questions Raised

  • Participants discuss the equations of motion and the relationships between forces acting on the ladder. There are mentions of free body diagrams and the motion of the center of mass. Some participants express confusion about the ladder's motion and the implications of energy conservation.

Discussion Status

The conversation is ongoing, with various participants offering insights and questioning each other's reasoning. Some guidance has been provided regarding the use of free body diagrams and the importance of understanding the motion of the center of mass. However, there is no explicit consensus on the approach to solving the problem.

Contextual Notes

Participants note that the problem may not be a typical homework assignment, as it was encountered in a test context. There is also a suggestion that the ladder's motion involves momentum accumulation, which may influence the analysis.

HiPPiE
Messages
20
Reaction score
0
A uniform ladder of length L leans against a smooth (no friction) wall. The floor is also smooth (no friction) and the ladder makes an angle of Theta-0 with the floor when the ladder is installed at rest.

a) Before the ladder leaves the wall, express the equations of motion of the ladder in terms of a single generalized coordinate.

b) Find a constant of the motion.

c) Find the angel theta at which the ladder leaves the wall.

EDIT:
By the way, the idea is that the ladder accumulates some momentum in the horizontal, the way its motion is, and because of that it detaches from the wall rather than sliding all the way down against it.
 
Last edited:
Physics news on Phys.org
HiPPiE said:
A uniform ladder of length L leans against a smooth (no friction) wall. The floor is also smooth (no friction) and the ladder makes an angle of Theta-0 with the floor when the ladder is installed at rest.

a) Before the ladder leaves the wall, express the equations of motion of the ladder in terms of a single generalized coordinate.

b) Find a constant of the motion.

c) Find the angel theta at which the ladder leaves the wall.

EDIT:
By the way, the idea is that the ladder accumulates some momentum in the horizontal, the way its motion is, and because of that it detaches from the wall rather than sliding all the way down against it.

Nobody is going to solve your problems for you, try telling us what you are stuck with.

Regards,

Nenad
 
You guys are bitter. It's not my homework or anything, I just thought it was a good problem because it was hard and I don't know how to do it. It was on a test my dad was proctoring.
 
HiPPiE said:
You guys are bitter. It's not my homework or anything, I just thought it was a good problem because it was hard and I don't know how to do it. It was on a test my dad was proctoring.

We are not here to solve arbitrary problems, if you want to know how to approach th problem, draw the free body diagram, label all of your axis, create your force equations and work form there. Try doing this first, if you get stuck, come and ask.

Regards,

Nenad
 
OK... this is what I have so far:

Free body diagram: What are the relationships between the normal forces and the gravity?

Motion of center of mass: this works... but we now need to find the acceleration along this path and such... hmmm
 

Attachments

  • free-body.JPG
    free-body.JPG
    5.8 KB · Views: 654
  • position.JPG
    position.JPG
    14.9 KB · Views: 538
Well, this is a classic problem.
As I recall, the sly way to do this is to use energy.
 
Your pictures don't make sense. How can the center of mass move in the fashion demonstrated?
 
I sort of derived why the equation of motion is x^2 + y^2 = 1/4 L^2.
That's the equation of a circle, if you didn't know. Again though, this is only if the ladder stays against the wall, which, in theory, it wouldn't.

As for understanding the motion, though, you can see it pretty easily:
Take a piece of paper, draw the wall and floor. Then draw many of the same-length ladder in different positions against the wall. Completely upright, completely laying down, and many positions in between. Then draw a dot at the middle of each ladder and connect the dots :)
 
First off, your center of mass particle draws out a complete quarter circle, which isn't possible considering its motion is not along the entire ladder (from wlal to floor). Second, you have drawn the CM moving to the right and then concave downward, but the force pulling the ladder is directed downwards. It should be starting down and then concave right as the ladder bottom is pulled out.
 

Similar threads

  • · Replies 20 ·
Replies
20
Views
2K
Replies
6
Views
3K
Replies
8
Views
1K
  • · Replies 11 ·
Replies
11
Views
6K
  • · Replies 5 ·
Replies
5
Views
3K
Replies
9
Views
2K
  • · Replies 12 ·
Replies
12
Views
2K
  • · Replies 9 ·
Replies
9
Views
3K
  • · Replies 3 ·
Replies
3
Views
5K
  • · Replies 27 ·
Replies
27
Views
5K