Imagine a simple circuit: a battery, a wire, a resistor. A positive charge +q+q leaves the ++ terminal, crosses the resistor losing energy qVqV (dissipated as heat), arrives at the - terminal at lower potential, then enters the battery and must return to the ++ terminal.

The delicate point is precisely this last stretch. Inside the battery the charge is moving against the internal electric field: the electrostatic field alone would push it back, towards the - terminal. Something, inside the battery, must do positive work on it to bring it back to the positive pole.

Principle — A non-electrostatic force is needed

To sustain the current, inside the source the positive charges must climb back up the potential, that is, move against the electrostatic field. Only a non-electrostatic force can perform the necessary positive work.

This “something” is a non-electrostatic force, whose origin varies with the type of source:

  • chemical in a battery;
  • mechanical in a dynamo generator;
  • thermal in a thermocouple;
  • light-driven in a photovoltaic cell.

The effect, whatever its origin, is the same: to push the positive charges towards the ++ terminal, compensating for the internal electrostatic “drop”. It is this force that sustains the potential difference at the terminals and hence the current in the external circuit.

Topics: Circuiti elettrici Concepts: Forza elettromotrice

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