What the calculator does
- Network mode: reduces any series–parallel combination of up to 24 resistors to one equivalent resistance, then works back out to find the current, voltage and power for each resistor. It checks that the power dissipated equals the power supplied.
- Ohm’s law mode: enter any two of voltage, current, resistance and power to find the other two.
The rules
Resistors in series carry the same current, and their resistances add:
Resistors in parallel share the same voltage, and their conductances add:
Ohm’s law and the power relations link everything together:
Worked example: 100 Ω + (220 Ω ∥ 330 Ω) on 12 V
- Parallel pair: 1/(1/220 + 1/330) = 132 Ω.
- Total: 100 + 132 = 232 Ω.
- Supply current: I = 12 / 232 = 51.7 mA. All of it flows through R1.
- Voltages: R1 drops 5.17 V, leaving 6.83 V across the parallel pair.
- Branch currents: R2 carries 31.0 mA and R3 carries 20.7 mA. Together they make up the 51.7 mA.
- Power check: the source supplies 621 mW and the resistors dissipate 621 mW in total.
Common mistakes
- Adding parallel resistances directly. Add the reciprocals, then take the reciprocal of the sum.
- Forgetting the final reciprocal, which leaves an answer in siemens rather than ohms.
- Assuming every resistor has the full supply voltage. That is only true for resistors connected directly across the source.
- Mixing kΩ and Ω, or mA and A. The calculator accepts prefixes and shows results in engineering units.
Practical applications
- Voltage dividers for sensors and setting reference voltages.
- LED current limiting, choosing a series resistor.
- Checking power ratings before building a circuit.
- Electronics coursework, where series–parallel reduction is a core skill.
Assumptions and limitations
The calculator models ideal resistors, ideal wires and a single ideal DC source, either a voltage source or a current source. Only circuits that reduce step by step to series and parallel combinations are supported; bridges, multiple sources, capacitors, inductors and AC analysis are not. Resistance is treated as constant, although real resistors change slightly with temperature. Results are computed in double precision.