§525 — Voltage drop: the 3%/5% limit and when it becomes decisive
§525 — Voltage drop: the 3%/5% limit and when it becomes decisive
The guide on cable cross-section & current-carrying capacity
covers how Iz = Itabel × f1 × f2 × f3 determines whether a cable can
thermally handle the current. That is not the only requirement a cable
must meet: §525 of NEN 1010 also sets a recommended limit on voltage
drop between the supply point and the load — a cable whose
cross-section comfortably satisfies the Iz requirement can still produce
too much voltage drop over a long cable run.
The recommended limit values
| Application | Maximum voltage drop |
|---|---|
| Lighting | 3% of nominal voltage |
| Other applications (socket outlets, motors, heat pumps) | 5% of nominal voltage |
On a 230 V installation this works out to roughly 6.9 V for lighting circuits and 11.5 V for other circuits, measured between the installation's supply point and the furthest load on that circuit.
Why this is a separate check
Voltage drop is not a thermal phenomenon like the Iz calculation, but a
consequence of the resistive (and, at larger cross-sections, also
inductive) impedance of the conductor itself: the longer the cable, the
greater the voltage drop at equal current and cross-section. A cable
that comfortably satisfies Iz ≥ Ib based on the correction factors from
§523 can still, over a cable length of say 40-50 meters (an outbuilding,
a shed, a long outdoor run to an EV charger), produce a voltage drop of
more than 5% — the two checks are independent of each other and must
both be performed separately.
A practical rule of thumb
A commonly used practical formula for copper conductors on single-phase circuits:
Uval (%) = (2 × L × Ib × cos φ) / (56 × A × Un) × 100
where L is the single (one-way) cable length in meters, Ib the load
current in A, A the cross-section in mm², Un the nominal voltage, and
56 the conductivity of copper in m/(Ω·mm²). When in doubt about the
exact constant for the material and frequency used: the tables in the
NEN 1010 annex are authoritative, this formula is a practical rule of
thumb for a first estimate.
Practical relevance
For long cable runs — a garden shed, a detached garage, an EV charger supply to the driveway — voltage drop is often the determining factor for the cross-section to choose, not the current-carrying capacity. A cable that would suffice at 2.5 mm² based on Iz sometimes needs to be upsized to 4 mm² or 6 mm², purely to stay within the voltage-drop limit.
Common mistakes
- Performing only the Iz calculation and skipping voltage drop — especially on long runs to outbuildings this results in a cable that is thermally adequate but delivers a noticeably lower voltage at the load (dimming lights, slower motor start-up).
- Applying the 3% limit to a mixed circuit with both lighting and socket outlets — the stricter 3% limit applies as soon as lighting is present on the circuit, not the more lenient 5% limit.
- Calculating voltage drop over the straight-line distance instead of the actual (sometimes detouring) cable route — a cable that has to go around a structural obstacle is longer than the straight-line distance to the load.
- Calculating voltage drop for the whole circuit from the transformer/meter instead of from the installation's supply point — §525 applies to the installation itself, not to the supplying network.
Related
Further reading
- IEC 60364-4-41Conventional touch voltage limit UL — 50V and 25V
- §414SELV, PELV & FELV — the extra-low-voltage measure
- §442Temporary overvoltage from an earth fault in the high-voltage network (§442) — why the substation voltage rise reaches the low-voltage installation
- §514§514 — Identification: labelling, warnings and documentation for the installation
- §714Outdoor lighting installations (§714) — garden lighting, site lighting and the requirements beyond a normal indoor installation
- §715 / IEC 60364-7-715§715 — Extra-low-voltage lighting installations