R₂L = R₂∥RL; Uout = Uin·R₂L/(R₁+R₂L)
The load is parallel to the lower resistor, reducing its effective value and the output voltage.
The load is parallel to the lower resistor, reducing its effective value and the output voltage.
Select a target and calculate.
The load is parallel to the lower resistor, reducing its effective value and the output voltage.
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.
Pure resistors and steady DC; source resistance, changing input current and component tolerances are excluded.
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.
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.
R₂L = R₂∥RL; Uout = Uin·R₂L/(R₁+R₂L)
R₂L = R₂ · RL / (R₂ + RL)Uout = Uin · R₂L / (R₁ + R₂L)| Symbol / input | Meaning |
|---|---|
| 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. |
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.
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.
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.
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 for ADC inputs, meters, sensors, bias networks and any circuit whose input resistance is not much greater than R₂.
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.
Useful for ADC inputs, meters, sensors, bias networks and any circuit whose input resistance is not much greater than R₂.
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.
The model assumes linear resistors at steady state. Source resistance, dynamic input current, capacitors, protection diodes, self-heating and resistor tolerance are excluded.