Feyman and layman explanation of energy conservation

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SUMMARY

In the discussion, Richard Feynman elucidates the principle of energy conservation in the context of levers and balancing weights. He emphasizes that when a lever is balanced, the potential energy (PE) of the raised mass equals the decrease in PE of the lowered mass, assuming no energy is added to the system. The conclusion drawn is that while the lever oscillates, the kinetic energy (KE) remains zero at the balance point, as the system is stationary. This understanding clarifies the relationship between potential energy and kinetic energy in a balanced lever system.

PREREQUISITES
  • Understanding of basic physics concepts such as potential energy and kinetic energy.
  • Familiarity with the law of levers and mechanical equilibrium.
  • Knowledge of energy conservation principles in closed systems.
  • Basic grasp of oscillatory motion and its implications in physics.
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  • Study the principles of mechanical equilibrium in detail.
  • Explore the mathematical formulation of energy conservation in oscillatory systems.
  • Learn about the dynamics of levers and their applications in engineering.
  • Investigate the relationship between potential energy and kinetic energy in various physical systems.
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This discussion is beneficial for physics students, educators, and anyone interested in understanding the fundamental principles of energy conservation and mechanical systems.

AntiElephant
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Skip to 29:50. Here Feynman is explaining how some laws are not independent of energy conservation. In this case he goes on to explain how instead of using the law of levers were can use energy conservation to see what weight an object needs to on one side be to balance (or be in a state where is tilts back and forth without problems)

However I'm unsure how he comes to explain it. He seems to conclude that the potential energy at balance should be the same as the potential energy when it's titled. Why is this exactly? I thought it should be the total energy we need to worry about? Actually in an analogy previously it seems quite clear that only the total energy should be conserved. I probably wouldn't have worried about it except for the fact it also plops out the right answer, W = 8lb, so I must be understanding something wrong.

When it's tilted there is maximum potential energy, when it returns to balancing point some of the potential energy is now rotational kinetic energy. Right? How can the potential energy always stay zero?
 
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His point is that when a lever is balanced it can very easily (i.e. by only adding enough energy to overcome friction) be rotated a small distance about the fulcrum. So as no energy has been added, the increase in potential energy of the mass that is raised at one end of the lever must equal the decrease of the PE in the mass that is lowered. It is assumed that the system is stationary before and after the rotation so that KE is zero.
 
MrAnchovy said:
His point is that when a lever is balanced it can very easily (i.e. by only adding enough energy to overcome friction) be rotated a small distance about the fulcrum. So as no energy has been added, the increase in potential energy of the mass that is raised at one end of the lever must equal the decrease of the PE in the mass that is lowered. It is assumed that the system is stationary before and after the rotation so that KE is zero.

Okay. So when it oscillates to the horizontal position would we have to conclude that KE at this point is practically 0? Because if the PE is always 0 at all stages then it could not have gained any KE.
 
AntiElephant said:
Okay. So when it oscillates to the horizontal position would we have to conclude that KE at this point is practically 0? Because if the PE is always 0 at all stages then it could not have gained any KE.
No, it does not oscillate to the horizontal position, it remains in the displaced position because there is no change in PE. Perhaps you are thinking about a balance rather than a simple lever where there is a counterweight that gains PE when the balance arm is displaced.
 

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