Ladder against a frictionless wall

In summary, the given scenario involves a uniform ladder leaning against a vertical wall at a 45 degree angle to the horizontal ground. The wall is 100% slippery while the coefficient of friction at the ground is represented by µ. It can be proven that µ≥0.5 since the ladder is not falling. However, if the wall is sloping away from the ladder at an angle of 2theta, the angles between the ladder and the wall and ground will no longer be equal, creating an isosceles triangle. This can be physically seen by placing the ladder against two different walls, resulting in different distances between the foot of the ladder and the base of the wall.
  • #1
rcouto
4
0
A uniform ladder leans safely against a vertical wall at an angle 45° to the horizontal
ground. The wall is 100% slippery, while at the ground the coefficient of friction is µ .
Prove that since the ladder is not falling, µ [itex]\geq[/itex] 0.5

I've attempted to solve this, and think I have, granted that Friction=[itex]\mu[/itex]mg, but is this true? If so, is it always true? I was taught that Friction=[itex]\mu[/itex]*Normal Force, and normal force=mg, but there are 2 normal forces in this problem, that of the wall on the ladder and that of the ground on the ladder.
 
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  • #2
But what if the wall is not vertical, but sloping away from the ladder at an angle to the ground of 2theta? Arrange the ladder so it makes the same angle with the wall as it makes to the ground


Wouldn't 2theta just equal 90 degrees then? Because 2theta+theta+theta=180 degrees
in which case the wall isn't actually sloping away from the ladder at all...
 
  • #3
rcouto said:
I've attempted to solve this, and think I have, granted that Friction=[itex]\mu[/itex]mg, but is this true?
Yes, for this problem, since you want the smallest value of µ.
If so, is it always true? I was taught that Friction=[itex]\mu[/itex]*Normal Force, and normal force=mg, but there are 2 normal forces in this problem, that of the wall on the ladder and that of the ground on the ladder.
So? Only the ground surface has friction.
 
  • #4
rcouto said:
But what if the wall is not vertical, but sloping away from the ladder at an angle to the ground of 2theta? Arrange the ladder so it makes the same angle with the wall as it makes to the ground

If the wall was not vertical, then there would be a vertical component to the Normal Reaction Force from the wall to take into account.
 
  • #5
PeterO said:
If the wall was not vertical, then there would be a vertical component to the Normal Reaction Force from the wall to take into account.

Yes, but I don't understand how it could be sloping away from the ladder using the given values for the angles. If the wall makes an angle of 2theta with the ground, and the angles the ladder makes with the wall and the ground are equal, wouldn't 2theta=90 degrees?
 
  • #6
rcouto said:
Yes, but I don't understand how it could be sloping away from the ladder using the given values for the angles. If the wall makes an angle of 2theta with the ground, and the angles the ladder makes with the wall and the ground are equal, wouldn't 2theta=90 degrees?

In the first problem, the wall was vertical, the angle between wall and ground = 90
The ladder was placed so that the ladder made two 45 degree angles, one with the wall, one with the ground. The Ground, wall and ladder form an isosceles triangle

The sloping wall situation appears to be changing the situation between wall, ground and ladder, but retaining the isosceles triangle condition. Ther will not be 45 degree angles anymore.

To physically arrange this: suppose you have have a smooth vertical wall at one end of a basketball court, and a smooth angled wall at the other end.
First you place the ladder against the vertical wall, creating an isosceles triangle.
Next you pick up the ladder, carry it to the other end of the court and place the ladder against that wall - again creating an isosceles triangle.
The foot of the ladder will be different distances from the base of the wall in each case!
 

Related to Ladder against a frictionless wall

1. What is a ladder against a frictionless wall?

A ladder against a frictionless wall is a theoretical physics problem that involves a ladder leaning against a wall with no friction between the ladder and the wall. This means the ladder can slide up and down the wall freely without any resistance.

2. What is the significance of this problem?

The ladder against a frictionless wall problem is commonly used in physics to demonstrate the concept of equilibrium and how forces interact with each other. It also helps to understand the role of friction in keeping objects in place.

3. What are the forces acting on the ladder in this scenario?

There are two main forces acting on the ladder in this scenario: the weight of the ladder pulling it downwards and the normal force from the wall pushing it upwards. Since there is no friction, there is no force preventing the ladder from sliding up and down the wall.

4. How does the angle of the ladder affect the forces acting on it?

The angle of the ladder affects the forces acting on it by changing the magnitude of the weight and normal force. As the angle increases, the weight of the ladder pulling it downwards also increases. However, the normal force from the wall remains the same regardless of the angle.

5. Can a ladder against a frictionless wall exist in real life?

No, a ladder against a frictionless wall cannot exist in real life as it goes against the laws of physics. In reality, there will always be some amount of friction between the ladder and the wall, which will prevent it from sliding up and down freely. This problem is used as a theoretical exercise to better understand the concepts of equilibrium and forces.

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