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
| Question | Idea 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 |