Busch 2006, Abschnitt 4.2.2.2

Loaded Voltage Divider Calculator

The load is parallel to the lower resistor, reducing its effective value and the output voltage.

MINTSI
01

Inputs

Voltage at the tap after the connected load draws current from the lower divider branch.

Actual supply voltage applied across the complete divider.

Resistance from supply to tap; it carries the combined load and lower-branch current.

Divider resistor from tap to reference, connected in parallel with the load.

Input resistance of the connected load between tap and reference.

02

Result

Select a target and calculate.

Output voltage of the loaded divider versus load resistance

The load sits in parallel with R₂ and pulls the output voltage down. Only when RL is much larger than R₂ (rule of thumb: at least ten times) does Uout approach the unloaded value (dashed). At RL = R₂ the drop is already substantial.

0.11101000246unloadedRL = R₂inputLoaded output voltage Uout [V]Load resistance RL (logarithmic) [kΩ]
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Calculation

R2L = R2∥RLUout = Uin·R2L/(R1+R2L)

The load is parallel to the lower resistor, reducing its effective value and the output voltage.

Understand the inputs
  • Loaded output voltage Uout — Voltage at the tap after the connected load draws current from the lower divider branch.
  • Input voltage Uin — Actual supply voltage applied across the complete divider.
  • Upper resistor R1 — Resistance from supply to tap; it carries the combined load and lower-branch current.
  • Lower resistor R2 — Divider resistor from tap to reference, connected in parallel with the load.
  • Load resistance RL — Input resistance of the connected load between tap and reference.
Example

12 V, R1=1.2 kΩ, R2=1.0 kΩ and RL=2.2 kΩ give R2L=687.5 Ω and Uout≈4.37 V.

Assumptions and limits

Pure resistors and steady DC; source resistance, changing input current and component tolerances are excluded.

Technical article

Understand Loaded Voltage Divider Calculator

This calculator shows the voltage a resistor divider actually delivers under load. It bridges the gap between the unloaded basic calculator and a tap connected to a sensor, ADC or device input that draws current.

What does this quantity describe?

Load resistance RL is electrically parallel to R2. First calculate R2L = R2·RL/(R2+RL), then use that equivalent resistance in the divider equation. The smaller RL is relative to R2, the further Uout falls.

Formula and variables

R2L = R2∥RLUout = Uin·R2L/(R1+R2L)

  • R2L = R2 · RL / (R2 + RL)
  • Uout = Uin · R2L / (R1 + R2L)
Symbol / inputMeaning
Loaded output voltage UoutVoltage at the tap after the connected load draws current from the lower divider branch.
Input voltage UinActual supply voltage applied across the complete divider.
Upper resistor R1Resistance from supply to tap; it carries the combined load and lower-branch current.
Lower resistor R2Divider resistor from tap to reference, connected in parallel with the load.
Load resistance RLInput resistance of the connected load between tap and reference.

Choose the inputs correctly

Measure Uin across the divider's outer terminals. R1 runs from supply to tap and R2 from tap to reference. RL is the effective input resistance connected across that same tap, obtained from a data sheet or measurement.

How to use the calculator

Enter the actual supply voltage, installed resistor values and the lowest expected RL. Calculate Uout and compare it with the connected circuit's permitted input thresholds.

Worked example

With Uin=12 V, R1=1.2 kΩ, R2=1.0 kΩ and RL=2.2 kΩ, R2L=687.5 Ω and Uout falls to about 4.37 V; unloaded it would be 5.45 V.

Understand the result and units

The difference from the unloaded value is loading error. If it is excessive, lower R1 and R2, increase RL, or buffer the tap with a voltage follower.

Resistances may be entered in Ω, kΩ or MΩ and are converted consistently. Uin and Uout use the same voltage dimension.

Useful next calculation

Compare with the unloaded voltage divider. Then use the Ohm's law calculator for branch current checks.

Typical applications

Useful for ADC inputs, meters, sensors, bias networks and any circuit whose input resistance is not much greater than R2.

Assumptions, limits and common mistakes

The model assumes linear resistors at steady state. Source resistance, dynamic input current, capacitors, protection diodes, self-heating and resistor tolerance are excluded.

Common mistake: Do not add RL in series: it is parallel to R2. For microcontroller inputs, a static data-sheet resistance may also be insufficient when a sampling capacitor draws brief current pulses.

Frequently asked questions

What is “Loaded voltage divider” used for?

Useful for ADC inputs, meters, sensors, bias networks and any circuit whose input resistance is not much greater than R2.

Where do the input values come from?

Measure Uin across the divider's outer terminals. R1 runs from supply to tap and R2 from tap to reference. RL is the effective input resistance connected across that same tap, obtained from a data sheet or measurement.

What does the result not cover?

The model assumes linear resistors at steady state. Source resistance, dynamic input current, capacitors, protection diodes, self-heating and resistor tolerance are excluded.

Sources, method and review

  • Rudolf Busch, Elektrotechnik und Elektronik für Maschinenbauer und Verfahrenstechniker, 4th ed. 2006, Abschnitt 4.2.2.2 und Aufgabe 4-12 (local chapter PDF)

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

Responsible
NormCalc-Redaktion
Last updated
2026-09-16