How is momentum conserved when external forces are present?

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Discussion Overview

The discussion revolves around the conservation of momentum in a scenario where an external force, specifically gravity, is acting on a system during a collision. Participants explore the implications of this external force on momentum conservation, particularly in the context of a mallet striking a stake.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • One participant questions how momentum can be conserved when gravity is acting on the system during the collision.
  • Another participant argues that the time interval of the collision is so small that gravity does not do work on the system, allowing momentum to be conserved at that instant.
  • A different participant acknowledges the presence of gravitational force but suggests that its effect is negligible compared to the collision force due to the short duration of the impact.
  • Some participants discuss the relationship between force, time, and momentum change, emphasizing that momentum can still be conserved if the external force does not perform work during the collision.
  • There is a contention regarding the significance of the gravitational force during the infinitesimal time of collision, with some asserting that it remains influential despite the short duration.

Areas of Agreement / Disagreement

Participants express differing views on the role of gravitational force in momentum conservation during collisions. No consensus is reached regarding the extent to which gravity affects momentum in this context.

Contextual Notes

The discussion highlights the complexity of analyzing momentum conservation in the presence of external forces, with participants relying on different interpretations of the effects of time intervals and forces involved.

azizlwl
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Sorry the title should be : Impulse and Momentum

3000Solved Problems in Physics-Shaum's

9.6:
A camper let's fall a heavy mallet of mass M from the height y upon the top of a tent stake of mass m and drives it into the ground a distance d. Find the resistance of the ground, assuming it to be constant and the stake and mallet stay together on impact.

Solution given:

The speed of the mallet on just striking the stake is v= √(2gy). Momentum is conserved at the instant of collision so that Mv=(M+m)v', where v' is the speed of the stake plus mallet just after impact.


My question is why the momentum is conserved since there is external force acting on the system, that is gravity.
 
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azizlwl said:
The speed of the mallet on just striking the stake is v= √(2gy). Momentum is conserved at the instant of collision so that Mv=(M+m)v', where v' is the speed of the stake plus mallet just after impact.My question is why the momentum is conserved since there is external force acting on the system, that is gravity.

Mind the wording. They write "at the instant..." or "just after". That means that the time interval is extremely small, infinitesimal. The time just before impact and just after impact are extremely close. In such a short instance of time gravity has done no work on the system, thus momentum is conserved.

Take for example "the instant of time" you drop something from rest. You've already dropped it, but it's speed is still zero. At least a measurable interval of time has to pass before gravity can change the momentum.
 
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Thank you.
But I still believe how small the time interval is, the gravity does not stop from exerting force.
 
Okay. It's true there's still a gravitational force, but the change in momentum is equal to the force times the time interval:

\frac{\mathrm{d}p}{\mathrm{d}t} = F
\Delta p = \int F\;\mathrm{d}t = F \Delta t = 0

So, even when there is a force (which I have never denied), momentum is conserved as long as this force doesn't do any work.
 
azizlwl said:
Thank you.
But I still believe how small the time interval is, the gravity does not stop from exerting force.
Sure, but if the duration of the collision is very short, the force of gravity is a tiny fraction of the force of the collision. Consider what happens if you just rest the hammer on the stake (nothing).
 
jahaan said:
Okay. It's true there's still a gravitational force, but the change in momentum is equal to the force times the time interval:

\frac{\mathrm{d}p}{\mathrm{d}t} = F
\Delta p = \int F\;\mathrm{d}t = F \Delta t = 0

So, even when there is a force (which I have never denied), momentum is conserved as long as this force doesn't do any work.

I think FΔt≠0 since Δt≠0
You can assume it is so small that its product is negligible.
But if F is large value then the product should have the effect on momentum.
 

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