By H.L.M. Lee – Updated March 24, 2022
In a series circuit, components are arranged one after another, forming a single closed path for current. The battery powers the loop, forcing the same current to flow through each resistor. Think of the battery as a water pump, current as water, and resistors as houses in a row: the water must pass through each house sequentially before returning to the pump.
Ohm’s law links voltage, current, and resistance:
\(V = IR\)
where V is the voltage across a resistor, I is the current through it, and R is the resistance. In series, because the current is identical for every element, the voltage drop across each resistor depends solely on its resistance.
A parallel circuit connects components like the rungs of a ladder. Each device sits on its own branch of the supply, so the same voltage appears across every resistor, but each can draw a different amount of current based on its resistance. Ohm’s law for current is expressed as I = V/R.
For a series arrangement of resistors R1, R2, R3, …, the equivalent resistance is the simple sum:
\(R_s = R_1 + R_2 + R_3 + …\)
Adding a resistor to a series circuit always raises the overall resistance.
In contrast, resistors in parallel act as a single resistor whose equivalent resistance is found using:
\(\frac{1}{R_p} = \frac{1}{R_1} + \frac{1}{R_2} + \frac{1}{R_3} + …\)
Adding a resistor in parallel always reduces the total resistance, a fact that underpins many practical advantages and disadvantages of this topology.
Fortunately, protective devices such as fuses are placed in series with the wiring. In the event of a short circuit, the fuse blows, breaking the circuit and preventing damage.