Solving Mass Flow Problem Homework

AI Thread Summary
The discussion revolves around a physics homework problem involving a sand-spraying locomotive and a freight car. The key focus is on calculating the speed of the freight car over time as it receives sand at a constant rate while maintaining a constant distance from the locomotive. Participants explore the relationship between mass transfer, momentum, and the equations governing the system, particularly emphasizing the change in momentum and the impact of the sand's velocity relative to the freight car. The conversation includes inquiries about the correct application of momentum equations and how to express the mass of the freight car plus sand as a function of time. Overall, the discussion seeks clarification on the momentum delivery rate and its implications for the freight car's speed.
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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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