FISEKON GmbH · Fischer Elektrokonstruktion

Calculators

Calculate voltage drop

This calculator works the other way round from the cross-section calculation. The cross-section is fixed and the question is what still arrives at the end of the cable. You need exactly this calculation for an existing installation or a later extension.

Input

Result

Voltage drop
—%
Voltage drop, absolute
—V
Voltage at the load
—V
Does the cross-section carry the current?
—

A guide, not a design to standard. We give no warranty for the correctness of the results. The applicable standards and case-by-case verification govern.

Result as PDF

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You receive inputs, result and formula as a PDF by email, to file or pass on.

The grey values are an example. Simply enter your own.

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Calculating is the easy part.

A formula gives you a number. Designing a plant also demands installation method, grouping, discrimination, the standards in force and a look at the installed base. That is what we take on.

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Method and questions

Voltage drop

Voltage drop across a cable of known cross-section.

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Worked example

The default case the calculator starts with, worked through once. Change the values above and it recalculates immediately.

Inputs

System
Three-phase (3~)
Operating current
32 A
One-way cable length
45 m
Conductor cross-section
6 mm²
Nominal voltage
400 V
Power factor cos φ
0.9
Conductor material
Copper (κ = 56 m/Ω·mm²)

Result

Voltage drop
1.67 %
Voltage drop, absolute
6.68 V
Voltage at the load
393 V
Does the cross-section carry the current?
In free air, yes. Installation method, grouping and ambient temperature remain to be checked to IEC 60364-5-52. The cable cross-section calculator does that.
Formula and standards

Formula

  • Three-phase Δu = (√3 · L · I · cos φ) / (κ · A)
  • Single-phase Δu = (2 · L · I · cos φ) / (κ · A)
  • DC Δu = (2 · L · I) / (κ · A)
  • Δu% = Δu / U · 100

Assumptions and standards

  • κ = 56 m/(Ω·mm²) for copper, 35 m/(Ω·mm²) for aluminium at 20 °C.
  • Resistive component only, without inductive reactance.
  • With heated conductors the resistance rises. At 70 °C the actual voltage drop is around 20 % above the value calculated here.
  • The formula is a linear approximation for voltage drops well below the nominal voltage. Once the calculated drop reaches the nominal voltage the design is unusable anyway, the voltage at the load is then left blank.
Why does the measured value differ from the calculated one?

The formula assumes a conductor temperature of 20 °C. In operation the conductor is warmer and its resistance rises, by about a fifth at 70 °C. On top of that comes inductive reactance, which becomes noticeable at large cross-sections.

Does this apply to long motor cables on a drive?

Only to a limited extent. Inverter-fed cables add switching edges, leakage currents and screening effects. The calculation is usable for a rough sizing but not sufficient for the final decision.

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