About locality in classical physics

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SUMMARY

This discussion centers on the concept of locality in classical physics, specifically in relation to Coulomb's law and Maxwell's Equations. It establishes that while Coulomb's law implies instantaneous action at a distance, Maxwell's Equations adhere to the principle of locality by incorporating the finite propagation speed of electromagnetic fields. The introduction of the vector potential A is highlighted as a crucial development that mediates interactions between charges, ensuring that physical quantities in equations of motion are evaluated at the same position, although solutions may involve integration over all space.

PREREQUISITES
  • Understanding of Coulomb's law and its implications in classical physics
  • Familiarity with Maxwell's Equations and their role in electromagnetism
  • Knowledge of vector potential A and its significance in mediating electromagnetic interactions
  • Basic grasp of equations of motion in physics
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  • Study the derivation and implications of Maxwell's Equations in electromagnetism
  • Explore the concept of vector potentials and their applications in physics
  • Investigate the role of locality in quantum mechanics and its differences from classical physics
  • Examine the implications of signal propagation speed in electromagnetic theory
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Physicists, students of classical mechanics, and anyone interested in the foundational principles of electromagnetism and the concept of locality in physical laws.

karlzr
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In wikipedia it says that "Coulomb's law of electric forces was initially also formulated as instantaneous action at a distance, but was later superseded by Maxwell's Equations of electromagnetism which obey locality."

I don't really understand in which sense Maxwell's equations solve the problem of locality? Is it the invention of vector potential A, which mediates the action of charges at a distance?
I am interpreting locality in this way:
what locality requires is that when we write an equation of motion, all physical quantities present should be evaluated at the same position, such as Maxwell's equations, Schrödinger's equation, Einstein's equations, etc. But locality doesn't say anything about the solution. Take the Maxwell's equation in the presence of external currents as an example, the solution might include integration over all space.
Thanks,
 
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Is it the invention of vector potential A, which mediates the action of charges at a distance?
No, the key point is the final propagation speed of changes in this field. With Coulomb's law, changing a charge distribution directly changes the potential everywhere. With the Maxwell equation (and the electromagnetic vector potential), this does not happen any more.

Take the Maxwell's equation in the presence of external currents as an example, the solution might include integration over all space.
Only in the static case, and then signal distribution speed does not matter.
 

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