Home & workshop Electrical

Power, current and voltage calculator

Last reviewed 7 Sept 2026 ·Method: P = V × I for DC and resistive loads; V × I × pf single phase, √3 × V × I × pf three phase on AC. Ohm’s law solves for whichever two quantities are left blank. The 125% row is the NEC continuous-load rule for sizing the protective device, not part of the current itself, and it has no equivalent under BS 7671 or IEC 60364.
Voltage
V
Current
A
Power 2,300 W
P = V × I = 230 × 10 · no power factor, so DC or a resistive load
Kilowatts 2.3 kW
Resistance 23 Ω
Current 10,000 mA
P = VI · AC adds power factor · 3-phase adds √3

Estimates for planning and study. Fixed wiring must be designed and installed to the wiring regulations that apply where you are, by someone competent to do it. The 125% rows follow the NEC continuous-load rule and apply in the United States; BS 7671 and IEC 60364 size the device against the cable instead.

Power is volts times amps. On AC, real power is V × I × pf single phase and √3 × V × I × pf three phase, so a three-phase 400 V supply at 16 A with a 0.9 power factor delivers 9.98 kW real out of 11.09 kVA apparent. Give any two of volts, amps, ohms and watts to get the rest.

How to calculate electrical power

1 Pick the pair of quantities you actually know, or take the Ohm’s law mode and leave the two you do not know empty.
2 For AC, set the power factor: 1 for heaters and lamps, 0.8–0.9 for motors.
3 Choose single or three phase where the mode offers it.
4 Read real power in watts, apparent power in VA for sizing a supply, and — if you are wiring to the NEC — the 125% row for a load that runs continuously.
5 Sanity-check the power figure. A surprisingly large one almost always means a unit slipped: milliamps entered as amps, or kilohms as ohms.

The gap between watts and volt-amps is the single most misunderstood thing in electrical sizing. Watts is the power actually doing work; volt-amps is the product of the voltage and the current the supply has to deliver. For a resistive load they are equal. For a motor, current lags voltage and the two diverge by the power factor, so a 10 kW motor at 0.8 might pull 12.5 kVA. Cables, breakers and generators all have to be sized for the apparent power, because the current is real whether it is doing useful work or not.

Going the other way, from a load rating to a current, is where domestic limits become concrete. A 230 V circuit protected at 16 A tops out near 3.7 kW; a 120 V circuit at 15 A stops at 1.8 kW. That is why showers, hobs and EV chargers need their own circuits rather than a socket, and why a 7.4 kW charger is 32 A on single phase but only 10.7 A per line at 400 V three phase. The 125% row is the NEC’s answer to a load that runs three hours or more, which would otherwise sit at the protective device’s thermal limit with nothing in reserve; BS 7671 and IEC 60364 reach the same safety a different way, by requiring the design current, the device rating and the cable’s derated capacity to fall in that order, with no uplift applied to the current itself. Either way a motor’s inrush of six or seven times its running current for a second or two is a separate matter, handled by the device’s trip curve rather than by its rating.

At 12 and 24 volts the same arithmetic turns thick. A 500 W inverter load is 41.7 A at 12 V against 2.2 A at 230 V, so vehicle and van wiring is far heavier than mains wiring for the same power, and doubling the system voltage to 24 V halves the current and quarters the loss in the cable. It is also why the fuse belongs close to the battery: the fuse protects the cable, and unprotected cable between battery and fuse is the dangerous part.

Ohm’s law itself is one equation, V = I × R, with P = V × I as a separate one, and between them any two of the four quantities determine the other two — the twelve rearrangements of the familiar wheel. The law describes ohmic components, which is a real restriction. A resistor is ohmic: double the voltage and the current doubles. A filament lamp is not, because its resistance rises sharply as it heats, which is why bulbs almost always fail at the moment you switch them on. Diodes, LEDs, motors and anything semiconductor are non-ohmic too, so the law gives a number that is right only at one operating point.

What people use it for

  • Sizing a generator or UPS in kVA
  • Converting a motor nameplate figure into supply current
  • Checking a circuit will carry an appliance
  • Converting between kW and horsepower
  • Sizing a fuse or breaker for a new load
  • Working out the supply voltage a component needs
  • Sizing a supply for three-phase machinery
  • Checking a heater against a household circuit
  • Converting an appliance wattage into current draw
  • Turning a clamp meter reading into watts
  • Sizing a circuit for an EV charger or heat pump
  • Finding the voltage across a resistor at a known dissipation
  • Fusing a 12 V accessory in a van or car
  • Comparing a 12 V and a 24 V system design
  • Checking headroom on a 230 V socket circuit
  • Solving an Ohm’s law problem from any two values
  • Finding a resistor value and the rating it needs
  • Checking total demand against the main supply fuse
  • Comparing the 120 V and 230 V versions of the same appliance
  • Working out the DC current an inverter pulls from a 12 V or 24 V bank
  • Comparing a single-phase and a three-phase supply for the same machine
  • Checking a motor nameplate against a clamp meter reading

Questions

P = V × I. DC stops there, because direct current has no power factor. AC adds one: P = V × I × pf on single phase, and P = √3 × V × I × pf on three phase.

IEC 60038:2009, IEC standard voltages (IEC catalogue entry; the standard is paywalled)NFPA 70, the National Electrical Code (NFPA offers free read-only access after a sign-in)NIST; the SI base units
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