Series circuits
What a series circuit is
- Components in series are connected one after another in a single loop.
- There is only one path for the charge to follow.
- If one component breaks or is removed, the whole circuit stops — the path is broken.
The three rules
Current is the same everywhere.
- There is only one path, and charge is conserved, so every coulomb that passes through one component must pass through all the others.
- An ammeter placed anywhere in the loop reads the same value.
Voltages add up to the supply voltage.
- Each coulomb receives energy in the battery and delivers it to the components in turn, so the energy given out must equal the energy taken in.
- This is conservation of energy applied to each coulomb.
Resistances add.
- Adding another resistor in series adds another obstruction to the single path, so the total resistance always increases.
How the voltage divides
- The voltages divide in proportion to the resistances.
- The largest resistance gets the largest share of the supply voltage, because the same current flows through all of them and .
- Two equal resistors in series split the supply voltage exactly in half.
Consequences worth knowing
- Adding a component in series increases , so from the current falls everywhere in the circuit.
- Existing bulbs get dimmer when another is added in series, because both the current through them and the voltage across them fall.
- Series is used where components must share a supply voltage, or where a switch must control everything at once — but rarely for lighting, because one failure kills the whole circuit.
Worked ExampleA two-resistor series circuit
A V battery is connected in series with a Ω and a Ω resistor. Find the total resistance, the current, and the voltage across each resistor.
Step 1 — Total resistance
Step 2 — Current (the same everywhere)
Step 3 — Voltage across each resistor
Step 4 — Check
Worked ExampleAdding a resistor to a series circuit
A V battery drives a current through a single Ω resistor. A second Ω resistor is then added in series. Find the current before and after, and the change in the power dissipated by the Ω resistor.
Step 1 — Before
Step 2 — After: new total resistance
Step 3 — New power in the Ω resistor
Step 4 — The change