Voltage Drop Calculator
Size your conductors with confidence. Check your voltage drop, find the smallest cable that passes, or see how far a run can go — every result cross-checked against current rating.
| Size | Drop V | Drop % | Limit | Rating A |
|---|---|---|---|---|
| 2.5 mm² | 9.63 | 4.19% | ✓ | 20 |
| 4 mm² | 6.01 | 2.61% | ✓ | 26 |
| 6 mm² | 4.04 | 1.76% | ✓ | 33 |
| 10 mm² | 2.41 | 1.05% | ✓ | 45 |
| 16 mm² | 1.53 | 0.67% | ✓ | 60 |
Where Voltage Drop Actually Bites

Where drop shows up first — distance multiplies every milliohm.

Measure at the load, not the board — that's the real number.

Cheap at rough-in, expensive once the walls close.
How the Calculation Works
| 5% | Point of supply to the far point of use — the AS/NZS 3000 maximum. |
| 2% | Consumer mains guideline, leaving budget for the sub-circuits. |
| 3% | Final sub-circuit guideline, best-practice split of the 5%. |
| 7% | Allowed where supply comes from a private transformer within the installation. |
Indicative values for planning. Confirm against the full AS/NZS 3008 tables and manufacturer data before installation.

If a run is over 30 metres, assume voltage drop decides the cable size — not the breaker.
Below that, ampacity almost always governs. Past it, the 5% budget runs out first and every extra metre costs you. Check both, then buy the larger of the two.
Run The Numbers Yourself
Vd = √3 × 36.9 × 100 × (1.38 × 0.86 + 0.079 × 0.510) ÷ 1000 = 7.85 V → 1.96%

“One size up costs a few hundred dollars at rough-in. Getting it wrong costs a re-pull… and in 21 years of Sydney installs, I've never once had a callback about a cable that was too big.”
Voltage Drop, Explained Properly
Everything behind the numbers above — the AS/NZS 3008 formulae, the legal limits, where the conductor data comes from, and the questions we get asked most on site. Open what you need.
AS/NZS 3008.1.1 gives two ways to arrive at the same answer: the impedance method, where you multiply current, length and the conductor's resistance and reactance; and the tabulated mV/A·m method, where the standard has already done that multiplication for you. This calculator uses the impedance method so the power factor and conductor temperature you enter are actually applied, then reports the equivalent mV/A·m figure so you can cross-check it against the printed tables.
Vd% = Vd ÷ Vnominal × 100. Use the nominal voltage of the system you are calculating — 230 V for single-phase, 400 V for three-phase line-to-line. Mixing 400 V drop against 230 V nominal is the single most common error we see in submitted calculations.
The tables in AS/NZS 3008.1.1 list a millivolt drop per amp per metre for each size and installation arrangement. Multiply it by your current and route length, divide by 1000, and you have volts: Vd = mV/A·m × I × L ÷ 1000. It is quick, but the printed figure assumes a fixed power factor and conductor temperature, so it will not match a corrected impedance calculation exactly.
Every conductor has resistance. Push current through it and some of the supply voltage is consumed getting to the load instead of doing work there — that loss is voltage drop. A 230 V outlet at the board can be a 213 V outlet at the end of a long sub-main, and the appliance only ever sees 213 V.
It is not just a compliance number. The lost voltage becomes heat in the cable, so you pay for it on every kilowatt-hour, and the equipment at the far end compensates by drawing more current — which increases the drop again. Motors are the clearest example: torque falls with the square of the voltage, so a 10% drop costs roughly 19% of starting torque and the motor runs hotter to deliver the same shaft power.
| Equipment | What excessive drop looks like |
|---|---|
| Induction motors, pumps, compressors | Hard starting, nuisance overload trips, higher running current, shortened winding life |
| LED lighting & drivers | Visible dimming along a run, flicker, mismatched colour between the first and last fitting |
| EV chargers | Charger derates or faults out; continuous full-load current makes drop worse than any other domestic circuit |
| Resistive heating, ovens, HWS | Slow heat-up — output falls with the square of voltage, so 5% low is about 10% less heat |
| Grid-connect solar inverters | Voltage rise instead of drop — inverter throttles or disconnects on over-voltage during peak export |
| Switchboards & sub-boards | Reduced fault level at the far end, which can push protective device clearing times out of compliance |
The practical consequence is that voltage drop, not current-carrying capacity, is what determines cable size on most long runs. A 6 mm² cable may be perfectly rated for 34 A, but at 60 metres it will fail the 5% limit long before it gets warm.
AS/NZS 3000 (the Wiring Rules) sets the ceiling: 5% from the point of supply to any point of use. That is a total budget for the whole path — consumer mains, sub-mains and final sub-circuit combined — not 5% per section. Where the installation is fed from its own transformer inside the site, the allowance increases to 7% measured from the transformer's LV terminals.
| Allowance | Applies to | At 230 V / 400 V |
|---|---|---|
| 5% | Point of supply to the far point of use — the hard limit | 11.5 V / 20.0 V |
| 2% | Working target for consumer mains, leaving room downstream | 4.6 V / 8.0 V |
| 3% | Working target for a final sub-circuit; also the common spec for lighting | 6.9 V / 12.0 V |
| 7% | Installations supplied from a private transformer within the site | 16.1 V / 28.0 V |
A workable division for a house or small commercial job is 1–2% on the consumer mains, 1% on sub-mains to a sub-board, and 2–3% on the final sub-circuit. Fix the mains allowance first — it is the section you can least afford to re-pull later. Use the cascaded-run mode in the calculator above to add the segments up properly rather than checking each one in isolation.
Two things sit outside the Wiring Rules but still bind you. Distributors publish their own service and connection rules — some require the mains drop to stay within 1% or specify a minimum consumer mains size regardless of calculation. And for grid-connect solar, AS/NZS 4777.1 limits the total drop from the inverter to the point of supply to 1%, because on export the same impedance produces a voltage rise at the inverter terminals.
The R and X figures in this calculator follow AS/NZS 3008.1.1 for annealed copper and aluminium conductors at their normal operating temperature — 75 °C for V-75 PVC and 90 °C for XLPE. Resistance rises with temperature at about 0.393% per °C for copper, so a cable running hot drops more voltage than the same cable running cool. That is why the insulation selection in the advanced panel changes the answer.
| Copper size | R at 75 °C (Ω/km) | X (Ω/km) | Reactance share |
|---|---|---|---|
| 2.5 mm² | 8.87 | 0.121 | Negligible |
| 6 mm² | 3.70 | 0.112 | Negligible |
| 16 mm² | 1.38 | 0.102 | Minor |
| 35 mm² | 0.627 | 0.0967 | Starts to count |
| 95 mm² | 0.232 | 0.0918 | Significant |
| 240 mm² | 0.0985 | 0.0879 | Comparable to R |
Notice the pattern: resistance falls almost in proportion to cross-sectional area, but reactance barely changes. Below about 25 mm² the resistive term dominates and power factor hardly affects the result. Above it, reactance becomes a real share of the impedance — which is why going up two sizes on a large three-phase sub-main returns less improvement than you would expect, and why paralleling two smaller cables is sometimes the better answer.
Aluminium is roughly 1.6 times the resistance of copper for the same area, so an aluminium conductor needs about two sizes up to match a copper one on voltage drop. It is still common on larger consumer mains because the cost and weight savings outweigh the extra size.
A compliant cable has to satisfy four tests, and voltage drop is only one of them. Sizing on drop alone is how undersized mains get installed on short runs and oversized cable gets bought on long ones.
| Ambient air 40 °C / 45 °C / 50 °C (V-75 PVC) | 0.94 / 0.87 / 0.79 |
| 2 / 3 / 4 circuits grouped and enclosed | 0.80 / 0.70 / 0.65 |
| Touching thermal insulation on one side | 0.75 |
| Completely surrounded by thermal insulation | 0.50 |
| Buried direct, thermal resistivity above 1.2 K·m/W | 0.90 or lower |
The current-rating line in the results above applies a single set of assumptions as a sanity check. It tells you when the size that passes voltage drop is clearly under-rated for the load — it does not replace a full Table 4 selection against your actual installation method, grouping and ambient temperature.
Disclaimer: This calculator is designed in accordance with AS/NZS 3008.1.1 — Electrical Installations: Selection of Cables and typical Australian installation conditions. While every effort has been made to ensure accuracy using official formulae and data, Spark Innovation Group accepts no liability for design or compliance decisions based on these calculations.
