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EMF and internal resistance

Intermediate

Terminal voltage drops under load.

Key relationV = ε − Ir

A real source has EMF ε and internal resistance r, so terminal voltage V = ε − Ir drops under load. EMF is the open-circuit voltage.

Worked example

A 12 V battery with r = 0.1 Ω delivering 30 A: V = 9 V.

Common mistake

Short circuit current is ε/r.

In more detail

A real cell has an electromotive force (EMF) and an internal resistance. Its terminal voltage falls as current is drawn, V = ε − Ir.

Real-world uses

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Frequently asked questions

What is EMF?

The energy per unit charge supplied by the cell, measured in volts, though it is not a force.

Why does voltage drop when current is high?

Because some voltage is used across the internal resistance.

What is the emf of a cell?

The voltage the cell provides when no current is drawn, which is the energy given to each coulomb of charge.

Related topics in Current Electricity & Circuits

Electric power · Heating effect of current · Electrical energy and cost · Cells in series and parallel · Kirchhoff's current law · Kirchhoff's voltage law

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