Momentum problem with varying mass

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Homework Help Overview

The discussion revolves around a momentum problem involving a system with varying mass, specifically a cart and a bucket that fills with water over time. The original poster attempts to analyze the forces and momentum changes as water is added to the system.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants explore the relationship between force and momentum in a system with varying mass, questioning the conservation of momentum in different directions. The original poster seeks hints for progressing from their initial equations.

Discussion Status

Some participants have provided insights into the nature of internal forces and the implications for momentum conservation. There is an acknowledgment of the complexity introduced by vertical forces, indicating a productive exploration of the problem.

Contextual Notes

Participants note that the net force is zero in the horizontal direction but question the conservation of momentum in the vertical direction due to external forces acting on the system.

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Homework Statement


I have posted the attachement.


Homework Equations


[tex]\vec{F}=\frac{d\vec{p}}{dt}[/tex]

The Attempt at a Solution



let the time taken for the bucket to fill up be T. then
[tex]\frac{dp}{dt}= m(t)\, \frac{dv}{dt}+v(t)\, \frac{dm}{dt}[/tex]

where m and v are functions of time.

[tex]\frac{dm}{dt}=\frac{\rho V}{T}[/tex] since after time T, [tex]\rho V[/tex] of mass
of water will fill up in the bucket. so

[tex]m(t)=\left(\frac{\rho V}{T}\right)t+m[/tex]

and the momentum at time t would be

[tex]\vec{p}(t)=m(t)\, v(t)[/tex]

but after this I don't have much clue. any hints ?
 

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Consider the problem as inelastic collision of the cart with water drop(s). A water drop of mass Δm, falling vertically into the bucket has zero horizontal momentum, and gains Δm*v(t+Δt) momentum in the collision process. At the same time the momentum of the cart with the bucket and the water inside (mass m(t) ) changes to m(t)*v(t+Δt). The net change of the momentum of the cart-water-water drop system is zero, as there is no external force.

Δp=(Δm+m(t))v(t+Δt) -m(t)v(t)=0 --->Δm*v(t+Δt)+m(t)*[v(t+Δt) - v(t)]=0

Turning to derivatives, we arrive that the time derivative of the momentum is zero.

[tex] \frac{dp}{dt}= m(t)\, \frac{dv}{dt}+v(t)\, \frac{dm}{dt}=0[/tex].


Substitute the time dependent mass, and solve for v.

ehild
 
ah, ehild thanks. I was confused about the force. I forgot to consider the whole system. I now realize that internal forces between the water drops and the bucket don't matter. By the way, the net force is zero only in horizontal direction. I vertical direction, I think, it won't be conserved since the ground will exert some force on the system.
 
Yes, you are right, the vertical component of the momentum is not conserved.

ehild
 

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