Local Conservation of Charge: Feynman's Thought Experiment Explained

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SUMMARY

Feynman's thought experiment on the conservation of charge illustrates the principle of local conservation, where two observers perceive the disappearance and reappearance of charge differently due to their relative motion. The stationary observer witnesses the charge's appearance and disappearance simultaneously, while the moving observer does not. Feynman emphasizes that if charge changes from Q1 to Q2 over a time interval from T1 to T2, an equivalent amount of charge (Q2-Q1) must pass through a surrounding surface during that interval, reinforcing the concept that conserved quantities must transition smoothly and continuously between nearby points.

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  • Understanding of basic physics concepts, particularly electromagnetism.
  • Familiarity with the principles of relativity and reference frames.
  • Knowledge of conservation laws in physics.
  • Basic mathematical skills to comprehend charge equations and intervals.
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  • Explore the implications of local conservation laws in electromagnetism.
  • Study the principles of special relativity and their effects on observers.
  • Investigate mathematical formulations of charge conservation in different reference frames.
  • Learn about Feynman's lectures and their contributions to modern physics.
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Physics students, educators, and anyone interested in the foundational concepts of electromagnetism and relativity will benefit from this discussion.

AlchemistK
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I was watching the messenger lectures by Feynman and in the third lecture he talks about conservation. In the beginning he talks about the conservation of charge, and at one point demonstrates a thought experiment in which two observers, one stationary and the other moving, see a charge disappear at one point in front of them and another similar charge reappear behind them. The person stationary with respect to the charges see the charge appear at the same time it disappears, but the second person disagrees because of his movement.
Then Feynman states that charge is conserved locally.
What does he mean by that?

(He also states that if something is conserved, it must also be conserved locally.)
 
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It means something like this: if the amount of charge at some point in space changes value from Q1 to Q2 in a time interval from T1 to T2, then there exists a surface surrounding the point such that an amount of charge equal to Q2-Q1 passes through the surface in the same time interval. It's just a way of saying that for a conserved quantity such as charge to change value at a point, it must do so by moving in a smooth and continuous way to some nearby point(s).
 

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