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Current Electricity — Part 2: Cells and combinations of resistors

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Lesson

Inside the cell, and many paths

Part 2 — a cell is not a perfect source: some of its push is used up inside it. And real circuits join resistors one after another or side by side.

In this lesson you will

  • Distinguish the e.m.f. of a cell from its terminal voltage
  • Use E = I(R + r) and V = E − Ir
  • Derive and use the equivalent resistance of resistors in series and in parallel
  • Find currents and potential differences in a simple series–parallel network
Table of everyday questions and the idea each one uses
QuestionIdea used
Why does a torch dim as its cells age?Internal resistance rises
Why do fairy lights go dark together?Series connection
Why do room lamps work independently?Parallel connection
How much current does the battery give?Equivalent resistance