Can Calculus of Variations Prove the Path of Least Resistance for Current Flow?

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SUMMARY

The discussion centers on using the calculus of variations to demonstrate that electric current follows the path of least resistance. Key equations mentioned include the current equation I = dq/dt = nqvA and the resistance formula R = rho*l/A, where v represents drift velocity. The participants clarify that while current does not exclusively take the path of least resistance, it tends to maximize flow along this path when multiple routes are available. The current density is defined by J = σE, linking current density to electric field and conductivity.

PREREQUISITES
  • Understanding of calculus of variations
  • Familiarity with electrical engineering concepts, particularly current and resistance
  • Knowledge of the equations governing current flow, specifically I = dq/dt and J = σE
  • Basic principles of electric fields and conductivity
NEXT STEPS
  • Research the application of calculus of variations in physics
  • Explore advanced topics in electrical conductivity and its implications on current flow
  • Study the derivation and implications of the equation J = σE in various materials
  • Investigate alternative methods to model current flow in complex circuits
USEFUL FOR

Electrical engineers, physicists, and students studying electromagnetism or calculus of variations who are interested in the behavior of electric current in conductive materials.

sodaboy7
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Current follows the path of least resistance or shortest path. I just want to prove this or rather reproduce it using calculus of variations. I just want to show it in a fancy way. I want help to form the FUNCTIONAL for it.
Useful equations:
I=dq/dt=nqvA
R=rho*l/A
Where v is drift velocity

Any suggestion (may be using different equations and parameters)?
 
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The current does not actually take the path of least resistance. It takes all available paths. In general:

J = \sigma E

Where J is current density, E is electric field, and σ is the electrical conductivity.
 
It prefers path of least resistance. Or it maximum current follows the path of least resistance upon division at a point.
 

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