Busch 2006, Abschnitt 4.1.4 Reale Spannungsquelle

Loaded DC source terminal voltage

Load current produces a voltage drop across internal resistance that reduces the source voltage available at the terminals.

MINTSI
01

Inputs

Voltage actually available at the source terminals under the stated load.

Internal unloaded voltage of the source, e.g. nominal battery voltage or cell EMF.

DC current delivered by the source to the connected load at the operating point.

Equivalent source resistance including electrodes, electrolyte or winding and internal connections.

02

Result

Select a target and calculate.

Calculation

Uterm = Uq − Ia·Ri

Load current produces a voltage drop across internal resistance that reduces the source voltage available at the terminals.

Understand the inputs
  • Terminal voltage UtermVoltage actually available at the source terminals under the stated load.
  • Open-circuit source voltage UqInternal unloaded voltage of the source, e.g. nominal battery voltage or cell EMF.
  • Load current IaDC current delivered by the source to the connected load at the operating point.
  • Internal resistance RiEquivalent source resistance including electrodes, electrolyte or winding and internal connections.
Example

Uq=12 V, Ia=5 A and Ri=0.2 Ω give a 1 V drop, Uterm=11 V and internal power loss Ia²·Ri=5 W.

Assumptions and limits

Linear source with constant Ri under steady DC load; state of charge, temperature dependence of Ri and dynamic terminal behaviour are excluded.

Technical article

Understand Loaded DC source terminal voltage

This calculator models a real DC source as an ideal source voltage in series with an internal resistance, showing how far terminal voltage drops below open-circuit voltage under load.

What does this quantity describe?

From the real-source equivalent circuit, Uterm=Uq−Ia·Ri. The term Ia·Ri is the internal voltage drop; it grows proportionally with drawn current and reduces the voltage available to the load.

Formula and variables

Uterm = Uq − Ia·Ri

  • Uterm = Uq − Ia·Ri
  • Pv = Ia²·Ri
  • Ri = (Uq−Uterm)/Ia
Symbol / inputMeaning
Terminal voltage UtermVoltage actually available at the source terminals under the stated load.
Open-circuit source voltage UqInternal unloaded voltage of the source, e.g. nominal battery voltage or cell EMF.
Load current IaDC current delivered by the source to the connected load at the operating point.
Internal resistance RiEquivalent source resistance including electrodes, electrolyte or winding and internal connections.

Choose the inputs correctly

Uq is the unloaded source voltage, such as a battery's rest voltage or a supply's open-circuit voltage. Ia is the actually drawn DC current. Ri is the source's internal equivalent resistance at this operating point.

How to use the calculator

Measure Uq unloaded where possible, then record Ia and the corresponding terminal voltage under load; Ri can be back-calculated as (Uq−Uterm)/Ia or taken from a datasheet.

Worked example

Uq=12 V, Ia=5 A and Ri=0.2 Ω give a 1 V drop, so Uterm=11 V, and internal power loss Ia²·Ri=5 W.

Understand the result and units

A large gap between Uterm and Uq indicates high internal resistance or heavy load. At short circuit (Uterm=0) the model gives the theoretical short-circuit current Uq/Ri.

Uq and Uterm are voltages, Ia a current and Ri a resistance. All values are converted internally to coherent SI units.

Useful next calculation

For the opposite view at a load, see loaded voltage divider; the analogous balance at a motor is DC motor back EMF.

Typical applications

Estimating voltage sag of batteries, rechargeable cells, solar cells or simple power supplies under load, and a basis for sizing buffer capacitors or cable cross-sections.

Assumptions, limits and common mistakes

Linear source model with constant Ri under steady DC load. State-of-charge dependence, temperature effects on Ri, AC components and dynamic settling behaviour are excluded.

Common mistake: Do not accidentally enter the loaded terminal voltage as Uq. Do not confuse Ri with the load resistance; both sit in the same circuit but are distinct quantities.

Frequently asked questions

What is “Loaded DC source terminal voltage” used for?

Estimating voltage sag of batteries, rechargeable cells, solar cells or simple power supplies under load, and a basis for sizing buffer capacitors or cable cross-sections.

Where do the input values come from?

Uq is the unloaded source voltage, such as a battery's rest voltage or a supply's open-circuit voltage. Ia is the actually drawn DC current. Ri is the source's internal equivalent resistance at this operating point.

What does the result not cover?

Linear source model with constant Ri under steady DC load. State-of-charge dependence, temperature effects on Ri, AC components and dynamic settling behaviour are excluded.

Sources, method and review

  • Rudolf Busch, Elektrotechnik und Elektronik für Maschinenbauer und Verfahrenstechniker, 4th ed. 2006, Abschnitt 4.1.4, Reale Spannungsquelle (local chapter PDF)

Our method, source hierarchy and automated checks are documented on the methodology page. Read the methodology

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NormCalc-Redaktion
Last updated
2026-09-16