Calculating Work Done by an Engine to Keep Wagon Moving

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Homework Help Overview

The problem involves calculating the work done by an engine to maintain the constant speed of a railway wagon that is being loaded with coal. The subject area includes concepts from mechanics, specifically work, energy, and the work-energy theorem.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • The original poster attempts to calculate the work done as 50,000 J and questions whether this is equal to the kinetic energy imparted to the coal. Other participants inquire about the method used to arrive at this value and suggest considering the work-energy theorem.

Discussion Status

The discussion is ongoing, with participants exploring different interpretations of the work done and its relationship to kinetic energy. Some guidance regarding the work-energy theorem has been introduced, but no consensus has been reached.

Contextual Notes

The problem is framed within the constraints of a homework assignment, and participants are navigating the implications of loading coal onto the wagon and its effects on the system's energy dynamics.

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Homework Statement



A railway wagon runs on frictionless rails and is pulled by an engine traveling at
10 ms−1 . The wagon is loaded at constant rate with 1000 kg of coal, dropped vertically
from rest for a time of 2 s. What is the work done by the engine to keep the wagon
moving at constant speed? Is the work done equal to the kinetic energy imparted to
the coal and, if not, explain why not.


Homework Equations





The Attempt at a Solution



So the work done is 50,000J right?

My hench is that this is not exactly equal to the KE imparted to the coal...but I am not sure how to explain this...something to do with downward impulse of coal on wagon?

Thanks
 
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anyone?
 
How did you get 50,000J?
 
KE before = 0.5mv^2

KE after = 1/2(m+1000)v^2..

difference = 50,000J

So please could you help with my second Q?
 
Well, do you know about the work-energy theorem?
 

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