Voltage drop:
why a long, thin cable loses volts on the way
Estimate how many volts a cable run wastes, express that as a percentage of supply and choose a thicker conductor or higher voltage when it is too much.
Calcylator Editorial Team
Updated · 5 min read
A cable is a resistor in series with your load
Copper is a good conductor, not a perfect one. Every metre of cable has a small resistance, and when current flows through that resistance a little voltage is lost along the way. The lost voltage appears as heat in the cable and as a lower supply at the far end.
For a 230 V mains socket a loss of 2 or 3 volts goes unnoticed. For a 12 V pump, a camera or a string of LED lights, the same loss is a large fraction of the supply and can show as dim lamps, slow motors or equipment that resets itself. That is why the topic comes up most often in solar, caravan, CCTV and low-voltage lighting installations.
Three things control the size of the drop: how much current the load draws, how long the cable is and how thick it is. The material enters through its resistivity, a constant that is lowest for silver and copper and noticeably higher for aluminium.
It is useful to separate the two jobs a cable has. As a safety component, it must not overheat, which depends on current and installation. As a performance component, it must deliver enough voltage at the load, which depends on length. A short heavy-duty feed and a long thin extension can both be perfectly safe yet behave entirely differently at the far end.
The formula for a two-wire circuit
Current has to go out to the load and come back, so a circuit of one-way length L uses 2 × L of conductor.
- I:
- Load current in amperes
- ρ:
- Resistivity of the conductor; copper ≈ 1.72 × 10⁻⁸ Ω·m at 20 °C
- L:
- One-way cable length in metres
- A:
- Conductor cross-section in m² (2.5 mm² = 2.5 × 10⁻⁶ m²)
Current
10 A
Length (one way)
20 m
Cable
2.5 mm² copper
Resistance per metre
1.72 × 10⁻⁸ ÷ 2.5 × 10⁻⁶ = 0.00688 Ω
Loop resistance
2 × 20 × 0.00688 = 0.275 Ω
Drop
10 × 0.275
Voltage drop
about 2.75 V
Same as 2 × 10 × 1.72 × 10⁻⁸ × 20 ÷ 2.5 × 10⁻⁶ = 2.752 V.
The figure by itself has no meaning until you compare it with the supply. On 230 V, 2.75 V is 1.2 per cent. On a 12 V system it is 22.9 per cent, which leaves the load with only about 9.2 V.
Turning volts into a percentage and a limit
- ΔV:
- Voltage drop in volts
- Supply voltage:
- Nominal voltage at the source
Wiring codes and equipment makers set limits on the allowed drop, commonly a few per cent of the nominal voltage, often tighter for lighting than for other loads. The numbers differ between countries and installation types, so take the limit from the wiring code or the product's data sheet that applies to your job.
| Supply | Drop in the 10 A, 20 m example | As percentage |
|---|---|---|
| 12 V DC | 2.75 V | 22.9% |
| 24 V DC | 2.75 V | 11.5% |
| 48 V DC | 2.75 V | 5.7% |
| 230 V AC | 2.75 V | 1.2% |
A load that draws a fixed power takes less current at a higher voltage, so a real 24 V system carrying the same power would draw half the current, and the drop would fall to about 1.4 V, or 5.7 per cent. Raising the voltage is one of the most effective cures for a long low-voltage run.
Ways to reduce the drop
- Use a larger cross-section. Doubling the area halves the drop. For the 12 V example, holding the loss to 3 per cent, or 0.36 V, needs 2 × 10 × 1.72 × 10⁻⁸ × 20 ÷ 0.36, about 19.1 mm², which in practice means a 25 mm² cable.
- Shorten the run by moving the supply, battery or inverter closer to the load.
- Raise the system voltage. A 24 V or 48 V design needs less current for the same power.
- Share the load across parallel cables, but only if the installation rules allow paralleling and the cables are matched.
- Use good terminations; loose or oxidised joints add resistance that the formula does not capture.
Copper is not the only choice. Aluminium is lighter and cheaper but has about 1.6 times the resistivity, so the same 20 m, 10 A run in 2.5 mm² aluminium would drop roughly 4.5 V instead of 2.75 V. It is typically used in larger sizes on mains feeders where the extra area is easy to accommodate.
Do the arithmetic in a consistent order every time. Fix the supply voltage first, then the load current from the power rating, then the run length, and only then choose a cross-section. Decisions made in that order seldom need undoing, whereas picking a cable size first and testing it afterwards leads to repeated rework.
A second case: a workshop socket
Consider a socket circuit feeding a power tool in a shed at the end of the garden. The tool draws 16 A at 230 V, the cable runs 30 m from the house and the installer used 4 mm² copper.
Current
16 A
One-way length
30 m
Cable
4 mm² copper
Resistance per metre
1.72 × 10⁻⁸ ÷ 4 × 10⁻⁶ = 0.0043 Ω
Loop resistance
2 × 30 × 0.0043 = 0.258 Ω
Drop
16 × 0.258 = 4.13 V
Drop as share of 230 V
about 1.8%
The tool receives about 225.9 V.
That figure looks modest, and for a resistive load it is fine. Motors are more demanding because starting current can be several times the running current, and the momentary drop at start-up is correspondingly higher. A tool that stalls when switched on but runs well afterwards may be telling you about the cable and not the tool.
When you size cable for a motor, work out the drop at the starting current as well as the running current, using the starting figure from the motor's data plate or manual, and compare it with the limit the manufacturer gives for start-up.
Temperature, AC and three-phase circuits
Resistance rises with temperature. Copper increases by about 0.39 per cent for every degree Celsius, so a cable running at 70 °C has roughly 20 per cent more resistance than at 20 °C, and the 2.75 V drop becomes about 3.3 V. Cables bundled in conduit or buried in thermal insulation run warmer than the open-air figure.
For AC circuits the same formula is a good first approximation with small conductors and resistive loads. Larger cables add reactance, and inductive loads such as motors have a power factor below 1, so installers use the tables in the standards for accuracy. In balanced three-phase circuits the line-to-line drop is √3 × I × ρ × L ÷ A, because the currents are phased and do not simply double the length.
Circuit
Three-phase, 400 V
Current
16 A
Length
30 m of 4 mm² copper
Working
√3 × 16 × 1.72 × 10⁻⁸ × 30 ÷ 4 × 10⁻⁶
Line voltage drop
about 3.6 V (0.9%)
Check against the wiring code limit that applies to your installation.
Common questions
What is the formula for voltage drop in a cable?
For a two-wire circuit it is ΔV = 2 × I × ρ × L ÷ A, where I is the current in amperes, ρ the resistivity, L the one-way length and A the cross-section. Copper's resistivity is about 1.72 × 10⁻⁸ Ω·m.
How much voltage drop is acceptable?
It depends on the standard and the load. Many wiring codes and equipment data sheets set a limit of a few per cent of the nominal voltage, tighter for sensitive or lighting circuits. Check the applicable code or product manual rather than relying on one fixed figure.
Why is voltage drop worse at 12 V than at 230 V?
The same cable and current lose the same number of volts, but 2.75 V is 22.9% of 12 V and only 1.2% of 230 V. Low-voltage systems also need higher current for the same power, which increases the drop.
Does a thicker cable reduce voltage drop?
Yes. Drop is inversely proportional to the conductor area, so doubling the cross-section halves the loss. Moving the 20 m, 10 A example from 2.5 mm² to 5 mm² cuts the drop from about 2.75 V to about 1.38 V.
Does temperature affect voltage drop?
Yes. Copper resistance rises about 0.39 per cent per °C, so a warm cable has more drop. At 70 °C the resistance is roughly 20% higher than at 20 °C, which is why standards use correction factors.
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