Relationship between Electric Field and Potentential

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SUMMARY

The relationship between electric field (E) and electric potential (V) is defined by the equations E=keQ/r² and V=keQ/r. The electric field represents force per unit charge, while electric potential indicates energy per unit charge. The inverse square relationship in the electric field (1/r²) arises from the derivative of the potential (1/r), as E is the negative gradient of V, expressed mathematically as E = -∇V. This connection clarifies how the electric field diminishes with distance squared, while potential decreases linearly with distance.

PREREQUISITES
  • Understanding of electric fields and potentials
  • Familiarity with calculus, specifically derivatives
  • Knowledge of vector calculus and gradients
  • Basic principles of electrostatics
NEXT STEPS
  • Study the mathematical derivation of electric fields from potentials
  • Explore vector calculus applications in physics
  • Learn about electrostatic forces and their implications
  • Investigate the concept of gradient fields in electromagnetism
USEFUL FOR

Physics students, electrical engineers, and anyone interested in understanding the fundamental principles of electromagnetism and the mathematical relationships between electric fields and potentials.

spencerthought
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E=keQ/r2 and V=keQ/r , I'm curious as to what what causes the relationship to r vs r2. I know the electric field is a measure of force per unit charge and the electric potential is a measure of energy per unit charge, just struggling to mentally connect where the inverse square relation to distance loses the square.
 
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One is the derivative of the other. The derivative of 1/r gets you 1/r^2 (save some factor).
 
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spencerthought said:
E=keQ/r2 and V=keQ/r , I'm curious as to what what causes the relationship to r vs r2. I know the electric field is a measure of force per unit charge and the electric potential is a measure of energy per unit charge, just struggling to mentally connect where the inverse square relation to distance loses the square.


The most general form of the relationship between E and V is

[tex]E = -\nabla V[/tex]

This means that E is the vector gradient of the potential field V.

Zz.
 
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