Breaking a Wall: What Determines its Threshold for Crumbling?

In summary, the conversation discusses the concept of Newton's third law, where a force on an object results in an equal and opposite force. The example of breaking a wall with a hammer is used to explore this concept, with questions raised about the threshold value at which the wall begins to crumble and why it does not fall completely even when the force applied is just above this threshold. The conversation also touches on the idea that the equal and opposite force is a fundamental property of nature and not dependent on the material.
  • #1
I'm clever
4
0
I was thinking about this today:

When a force acts on an object, the object exerts on equal and opposite force - Newton's third law. Imagine this situation:

I am breaking down a wall with a hammer. I begin hitting the wall gently and this wall doesn't break. I then hit harder and the force exerted on the wall increases. As I'm hitting the wall harder, the wall begins to crumble and break.

What I want to know is:

- Does the wall have a certain threshold value at which point it cannot exert a force opposite and equal to the force I hit with and begins to crumble? The harder I hit, the more I exceed its threshold value and the more it crumbles and breaks.

-Why does the wall not fall down completely if I exert a force just above this theorized threshold value? Is it due to friction forces in the planes of atoms? Is it due to the composition of the wall itself? Or is it due to the way atoms are arranged in the wall?
 
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  • #2
Welcome to PF!

Hi I'm clever! Welcome to PF! :smile:

The horizontal reaction force doesn't really matter …

the wall breaks because of vertical forces …

the hammer makes the wall bend slightly, that produces a vertical force, and if that force is too great, the wall breaks. :wink:
 
  • #3
Interesting thoughts. A wall crumbling has very little to do with the 'equal and opposite force' however. The wall begins to crumble once enough damage has been done that it cannot support its own weight. Damage begins to be done once the force (only considering the 'force' is a simplification... but its okay) you apply is greater than the structural forces in the material (e.g. the forces between clumps of sheet-rock, or dry-wall, or whatever).

The equal and opposite nature of forces is (in most situations) a fundamental property of nature---not the material. There is no strength of hitting the wall at which there would no longer be an equal and opposite force. At a certain strength, however, the wall would give way.
 
  • #4
Yes zhermes, completely Ok.
Let'sjust remenber that the same damage caused to the wall has been "trying t be done" to the hummer. However , since the particles of the hummer are much more strongly related it does not affect them as much as it does on the particles of the wall whome are less strong related. After times of doing walls by the same hummer it will became less usefull. So:
- there is not "seuil" limit to the reaction,the 3 rd law always exists.
-the reaction is equal to the action in value opposant in direction.
 
  • #5
zhermes said:
Interesting thoughts. A wall crumbling has very little to do with the 'equal and opposite force' however.

I don't think a wall can pick or choose whether or not to go along with Newton III. If you hit the wall, the wall hits back. What can happen, though is that the force you actually exert can be less, if it starts to move away from your hammer and not all the momentum is lost (i.e. transferred to the Earth) But even in that case, there will be an equal and opposite force on hammer and wall.

If you try to 'break' a sheet of paper that's floating past you, using a hammer, you just can't get enough force on the paper. It will just accelerate along with the head of the hammer and you won't feel any reaction force. You can't transfer much energy into the air by punching it with a hammer, either, for the same reason.

To break something, it's usually necessary to keep one bit stationary (clamped in some way) and to exert a force on another bit of it. That will maximise the force. If you are a martial arts specialist, you can whizz your sword so fast through the air that you can cut a hair floating in front of you. You impose such a high acceleration on the tiny mass that the force is enough to go clean through it.
 
  • #6
zhermes said:
The equal and opposite nature of forces is (in most situations) a fundamental property of nature---not the material. There is no strength of hitting the wall at which there would no longer be an equal and opposite force. At a certain strength, however, the wall would give way.
same
sophiecentaur said:
I don't think a wall can pick or choose whether or not to go along with Newton II...the force you actually exert can be less...But even in that case, there will be an equal and opposite force on hammer and wall.
 
  • #7
More or less, yes.
 

Related to Breaking a Wall: What Determines its Threshold for Crumbling?

1. What is F=ma?

F=ma is a mathematical formula that represents Newton's second law of motion. It states that the force applied to an object is directly proportional to its mass and acceleration.

2. How is F=ma used in science?

F=ma is a fundamental equation in physics and is used to calculate the motion of objects when given information about their mass and acceleration. It is also used to understand the relationship between force, mass, and acceleration in various physical systems.

3. What are the units of measurement for F=ma?

The unit of force is typically measured in Newtons (N), mass in kilograms (kg), and acceleration in meters per second squared (m/s^2). Therefore, the unit for F=ma is N = kg x m/s^2.

4. Can F=ma be applied to all types of motion?

Yes, F=ma can be applied to both linear and rotational motion, as long as the mass and acceleration are known. It can also be used to understand the motion of objects in various forces, such as gravity or friction.

5. How does F=ma relate to real-life situations?

F=ma is applicable to many real-life situations, such as understanding the motion of a car, a person jumping, or the forces acting on a rocket during launch. It is also used in engineering and design to ensure the safety and stability of structures and machines.

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