Series vs Parallel Circuits: Current, Voltage and Resistance
Connecting parts in a single line is a series connection; connecting them side by side with their ends joined is a parallel connection. In series, the same current flows through every part and the voltage is divided among them. In parallel, the same voltage appears across every part and the current is divided among them. That is why resistances add in series, while in parallel the equivalent resistance is the reciprocal of the sum of reciprocals, smaller even than the smallest resistor. Capacitors are the exception: their formulas are reversed, adding in parallel and combining as reciprocals in series.
| Aspect | Series connection | Parallel connection |
|---|---|---|
| Shared quantity | Current (the same current flows through every part) | Voltage (the same voltage appears across every part) |
| Divided quantity | Voltage, divided in proportion to resistance (voltage divider): 2 kΩ and 1 kΩ on 12 V give 8 V and 4 V | Current, divided in inverse proportion to resistance (current divider): 3 A into 10 Ω and 20 Ω splits into 2 A and 1 A |
| Equivalent resistance | R = R1 + R2 + …: 100 Ω, 200 Ω and 300 Ω give 600 Ω | 1/R = 1/R1 + 1/R2 + …: 100 Ω, 200 Ω and 300 Ω give about 54.5 Ω; for two resistors, product over sum |
| Equivalent capacitance | 1/C = 1/C1 + 1/C2 + …, so it gets smaller: 10 µF and 22 µF give about 6.88 µF | C = C1 + C2 + …, so it adds: 10 µF and 22 µF give 32 µF |
| Equivalent inductance (no magnetic coupling) | L = L1 + L2 + … (same form as resistors) | 1/L = 1/L1 + 1/L2 + … (same form as resistors) |
| Part that dissipates more power | The larger resistance, because the current is the same (P = I²R) | The smaller resistance, because the voltage is the same (P = V²/R); two equal resistors share the power equally, but the ratings still need margin (derating) |
| When one part opens | Current stops in the whole circuit | Current keeps flowing through the other parts |
| Connecting batteries | Voltages add (two 1.5 V cells give 3 V); the capacity (mAh) stays that of one cell | The voltage stays that of one cell; capacities add, so it lasts longer |
| Examples in electronics | Voltage dividers, current-limiting resistors for LEDs, thermal resistances stacked from junction to case to heat sink | Paralleling power MOSFETs to lower on-resistance, many vias and power straps in parallel to reduce IR drop, decoupling capacitors, household outlets |
Figures are typical orders of magnitude and vary by process generation and product.