Calculating Work Done by Engine on Railway Wagon

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SUMMARY

The discussion focuses on calculating the work done by an engine on a railway wagon that is loaded with coal at a constant rate. The engine maintains a speed of 10 m/s while 1000 kg of coal is dropped into the wagon over 2 seconds. It is established that the work done by the engine is not equal to the kinetic energy (KE) imparted to the coal due to energy losses during the inelastic collision between the coal and the wagon. The work-energy theorem applies only to rigid bodies of constant mass, and in this scenario, the variable mass of the wagon complicates the conservation of mechanical energy.

PREREQUISITES
  • Understanding of the work-energy theorem
  • Knowledge of inelastic collisions
  • Familiarity with Newton's second law and variable mass systems
  • Basic principles of momentum and kinetic energy
NEXT STEPS
  • Study the implications of variable mass in dynamics
  • Learn about inelastic collision mechanics
  • Explore the work-energy theorem in non-rigid systems
  • Investigate the relationship between work done and momentum changes
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Physics students, mechanical engineers, and anyone interested in dynamics and energy conservation principles in variable mass systems.

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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



Done the first part fine..Just unsure about the second part...I know the work-energy theorem..But am i right in thinking that the WD =/= KE imparted to coal as some KE of coal is lost as heat as it collides with the wagon on its descent?
 
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You can just compare the work done with the gain in KE of the coal and see if they're equal. You're right that mechanical energy is not conserved as the coal is brought up to speed--think of the wagon as inelastically colliding with the coal. (It's not the KE due the coal's falling that matters here; you can just assume that the coal is dropped into the wagon from a low height with small vertical speed.)
 
The work-energy theorem is valid only to a rigid body of constant mass.You have variable mass here. Newton's second law is valid in the form dp/dt =F. The momentum is mv, so
dp/dt= v dm/dt +m dv/dt.
v is constant, so F=v*dm/dt. Multiplying both sides with v, and integrating with respect to time you get the relation between work and the change of the KE in this case.

As Doc Al said, you can not expect energy conservation, as this is kind of inelastic collision.



ehild
 

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