Solving Mass Flow Problem Homework

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SUMMARY

The discussion focuses on solving a mass flow problem involving a sand-spraying locomotive and a freight car. The key equations derived include the change in momentum expressed as ##P(t) = \Delta m u## and the rate of change of momentum given by ##\frac{dP}{dt} = M \frac{dv}{dt} - \frac{dm}{dt} u##. The problem requires finding the speed of the freight car over time, considering the mass transfer rate ##\frac{dm}{dt}## and the constant relative velocity ##u## of the sand. Participants seek clarification on the correctness of their approach and further steps to solve the problem.

PREREQUISITES
  • Understanding of mass flow dynamics
  • Familiarity with momentum conservation principles
  • Knowledge of differential calculus
  • Basic physics concepts related to force and motion
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  • Explore the concept of mass flow rate in fluid dynamics
  • Study the application of the conservation of momentum in variable mass systems
  • Learn how to derive equations of motion for systems with changing mass
  • Investigate the relationship between force, mass, and acceleration in non-constant systems
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Students studying physics, particularly those focusing on mechanics and fluid dynamics, as well as educators looking for examples of mass flow problems in real-world applications.

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Homework Statement


A sand-spraying locomotive sprays sand horizontally into a freight car. The locomotive and the freight car are not attached. The engineer in the locomotive maintains his speed so that the distance to the freight car is constant. The sand is transferred at a rate ##\displaystyle \frac{dm}{dt}##, with a velocity ##\vec{u}## relative to the locomotive. The freight car starts from rest with an initial mass ##M_0##. Find the speed of the freight car for all time t.

Homework Equations


Change in momentum

The Attempt at a Solution


Since this is a flow of mass problem, we will use the concept of mass transfer and momentum, rather than F = ma.

First, we isolate the system such that we initially have a stationary freight car and some sand traveling towards the car.

Taking this system as it is, we can find the change of momentum.

##P(t) = \Delta m u##, where ##u## is the relative velocity of the sand with respect to the freight car, and ##\Delta m## is the mass of the little portion of sand we are analyzing.

##P(t + \Delta t) = M \Delta v + \Delta m \Delta v##

##P(t + \Delta t) - P(t) = M \Delta v + \Delta m \Delta v -\Delta m u ##

##\displaystyle \frac{\Delta P}{\Delta t} = M \frac{\Delta v}{\Delta t} + \frac{\Delta m \Delta v}{\Delta t}- \frac{\Delta m}{\Delta t} u##

##\displaystyle \frac{dP}{dt} = M \frac{dv}{dt} - \frac{dm}{dt} u##

Is this correct so far? If so, how do I proceed? Is ##\displaystyle \frac{dP}{dt} = 0##?
 
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Bump. Some help would be nice...
 
I might approach the problem in a slightly different way. Let ##r = \frac{dm}{dt}## be the rate at which sand is delivered to the freight car. The relative velocity between the arriving sand and the freight car is fixed at ##u## thanks to the matching speed of the locomotive.

What can you say about the mass of the freight car + sand as a function of time? Can you write an expression for it in terms of ##M_o , r, \text{ and } t##?

What is the rate of delivery of momentum to the freight car (that's ##\frac{dp}{dt}##)? Can you write an expression for it in terms of ##r, u, \text{ and }t##?

What's another name for ##\frac{dp}{dt}##?
 

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