How do we know how long the force is acting on an object?

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Homework Help Overview

The discussion revolves around the dynamics of a collision between two carts of different masses, specifically focusing on the concept of impulse and the duration of force exertion during the impact. The original poster raises a question about how to determine the time duration of the force acting on the objects during the collision.

Discussion Character

  • Exploratory, Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • Participants explore the relationship between impulse and force duration, questioning how to ascertain the time a force acts during a collision. They discuss the implications of different collision types, such as perfectly plastic impacts, and the nature of forces involved during and after the collision.

Discussion Status

The discussion is ongoing, with participants providing insights into the nature of impact forces and the challenges in measuring force duration. Some suggest that while net forces may be zero post-collision, local forces still exist, prompting further exploration of the mechanics involved.

Contextual Notes

Participants note the lack of a theoretical framework for determining the duration of impact forces and mention the need for experimental measurement, highlighting the complexity of real-world collisions.

eprparadox
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Hey all, so I'm self studying and I came across this question:

A ## 2 kg ## cart, traveling on a horizontal air track with a speed of ## 3 m/s##, collides with a stationary ##4 kg## cart. The carts stick together. The impulse exerted by one cart on the other has a magnitude of:

A. ## 0 ##
B. ## 4 N \cdot s ##
C. ##6 N \cdot s ##
D. ## 9 N \cdot s ##
E.## 12 N \cdot s##

So I know the answer is B and that's fine. We find the final speed of the combined system as

v_f = \frac{ 2kg \cdot 3m/s}{2 kg + 4 kg} = 1 m/s

The impulse is equal to the change in momentum of the stationary cart and so that is just equal to [$] 4kg \cdot 1 m/s = 4 kg \cdot m/s [/$]. That's all good.

My question is more of how we know how long a force is exerted. For example, if the objects didn't stick together, then the force exerted would be over the time that the two objects were touching each other.

In this case, is there a way to know this? Is is just as soon as the acceleration stops and we're moving at the combined final speed which is found by conservation of momentum?
 
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There is no theoretical basis for determining the time duration of an impact force. Smaller magnitude acting for a slightly longer time has the same effect as greater magnitude acting for a shorter time.

It is possible to experimentally measure the time history of a particular impact force event, but that requires special equipment and is unique to that particular impact.
 
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eprparadox said:
In this case, is there a way to know this? Is is just as soon as the acceleration stops and we're moving at the combined final speed which is found by conservation of momentum?
I think so. When they are moving together after the collision, there is no acceleration (assuming friction is absent). So Newtons laws would tell you force on each mass should be zero.
 
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I would agree with Terry that in the event of a perfectly plastic impact, such that the bodies travel on together, there is zero net force between them. But that does not mean that there is no force between them. Let me explain.

Consider a bullet shot and embedded in a ballistic pendulum. The bodies travel on together after impact. However, the material of the pendulum block is locally deformed where the bullet penetrates and lodges in the block. This local deformation causes a contact force to exist between the bullet at the block, even though the net force between them is zero.
 
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One can hypothesise a model for the impact process. E.g., likely to be an elastic deformation initially, in the sense that the force is proportional to the compression, but reaching a peak force and plateauing.

If the bodies stick together then the elastic phase will be short but not necessarily absent. The force may be proportional to compression during increasing compression and yet vanish as soon as it starts to decompress. Consider e.g. two blocks connected by a fragile spring. A body impacting one experiences increasing resistance as it pushes the first block along, then the spring breaks, so there is no rebound at the end. The impacted body may behave like that internally.
 
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