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DC Electricity Beginner 9 min read Nov 2026

Voltage Divider

A voltage divider uses two resistors to produce a fraction of the input voltage. Learn the formula, the loading effect and where dividers are used in sensors and references.

Definition

A voltage divider is a circuit of two or more resistors in series across a voltage source, where the voltage across one resistor is a fixed fraction of the source voltage. For two resistors, V_out = V_in × R₂ / (R₁ + R₂), where V_out is taken across R₂.

Learning objectives

  • Apply the two-resistor voltage divider formula.
  • Calculate the divider current and the power dissipated in each resistor.
  • Explain how a connected load changes the output voltage.
  • Choose sensible resistor values for a given load and accuracy.
Voltage Divider diagram A two-resistor voltage divider R₁ R₂ V out tap
Voltage Divider — schematic illustration
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Progressive explanation

Start with the plain-language idea, then move into the engineering detail. Each level stands on its own, so you can stop at the depth you need.

Beginner The core idea
A voltage divider turns a larger voltage into a smaller one using two resistors in series. The same current flows through both, so the voltage across each resistor is proportional to its resistance. If R₂ is half of the total resistance, the output across R₂ is half the input voltage.

Dividers are common in sensor circuits, reference settings and signal scaling. But a divider is not a power supply: if you connect a load across the output, it draws current and changes the division. This loading effect is one of the most important practical limitations of a simple divider.
Intermediate How it behaves in a circuit
For an unloaded divider, the current is I = V_in/(R₁ + R₂), and the output across R₂ is V_out = I × R₂ = V_in × R₂/(R₁ + R₂). The output can be taken across either resistor; swapping R₁ and R₂ inverts the ratio. The divider current should be large compared with any load current if the output is to remain close to the calculated value.

When a load R_L is connected across R₂, the effective lower resistance becomes R₂ || R_L, and V_out = V_in × (R₂ || R_L)/(R₁ + R₂ || R_L). This is always lower than the unloaded value. For a given load, a divider with smaller resistances is stiffer but draws more current and dissipates more power.
Advanced Limits, assumptions, engineering detail
A divider is a simple voltage-scaling network whose accuracy depends on resistor tolerance, temperature coefficient, self-heating and load impedance. For precise references, the Thevenin equivalent of the divider is useful: its open-circuit voltage is V_out and its source resistance is R₁ || R₂. This output resistance limits the bandwidth of a measurement because it forms a low-pass filter with cable and input capacitance.

Dividers are often used with a buffer amplifier to isolate the load, or replaced by a regulator when the load current varies. In high-voltage measurement, the divider must be designed with appropriate creepage, clearance and resistor voltage ratings, and the voltmeter’s input resistance is part of the divider. Capacitive dividers are used for AC and pulse measurements, where the ratio depends on capacitances instead of resistances.

Formulas and variables

Unloaded voltage divider
V_out = V_in × R₂ / (R₁ + R₂)
V_out Output voltage across R₂ · V V_in Input voltage · V R₁ Upper resistor · Ω R₂ Lower resistor · Ω
12 V with R₁ = 10 kΩ and R₂ = 4.7 kΩ gives V_out ≈ 3.84 V.
Divider current
I = V_in / (R₁ + R₂)
I Current through the divider · A V_in Input voltage · V R₁, R₂ Divider resistors · Ω
12 V across 14.7 kΩ gives I ≈ 0.816 mA.
Loaded divider
V_out = V_in × (R₂ || R_L) / (R₁ + R₂ || R_L)
V_out Output voltage with load · V R_L Load resistance · Ω R₂ || R_L R₂ in parallel with R_L · Ω
A 9 V divider with 1 kΩ and 2 kΩ loaded by 10 kΩ gives about 5.63 V instead of 6.0 V.

Units of measurement

QuantitySymbolUnit
Voltage V volt (V)
Resistance R ohm (Ω)
Current I ampere (A)
Power P watt (W)

Worked examples

Worked example

Output of an unloaded divider

Problem. A 12 V supply feeds R₁ = 10 kΩ in series with R₂ = 4.7 kΩ, with the output across R₂. Find V_out.

Solution. V_out = 12 × 4.7/(10 + 4.7) = 12 × 4.7/14.7 = 56.4/14.7 ≈ 3.84 V.

V_out ≈ 3.84 V.
Worked example

Effect of connecting a load

Problem. A 9.0 V supply feeds R₁ = 1.0 kΩ and R₂ = 2.0 kΩ. Find V_out unloaded and then with a 10 kΩ load across R₂.

Solution. Unloaded: V_out = 9.0 × 2.0/3.0 = 6.0 V. Loaded: R₂ || R_L = (2.0 × 10)/(2.0 + 10) = 20/12 ≈ 1.667 kΩ. V_out = 9.0 × 1.667/(1.0 + 1.667) = 9.0 × 1.667/2.667 ≈ 5.63 V.

V_out = 6.0 V unloaded; ≈ 5.63 V with the 10 kΩ load.

Practical applications

  • Sensor signal scaling
  • Reference and bias voltages
  • Battery voltage monitoring
  • Adjustable feedback networks

Automotive applications

Voltage dividers appear in sensor circuits and module inputs: a thermistor or potentiometer forms one arm of a divider, and the module measures the resulting voltage. A damaged ground or an unexpected parallel path changes the divider ratio and produces a plausible but wrong sensor reading. Technicians compare the measured voltage with the expected divider value and check the reference and ground supplies before condemning the sensor.

Industrial applications

Industrial measurement uses dividers to scale high voltages into the input range of meters, PLC analogue inputs and data-acquisition systems. Signal conditioning often adds buffering and filtering, because a bare divider has a relatively high output impedance and is susceptible to noise and cable capacitance. For safety-related high-voltage measurement, the divider’s insulation and resistor ratings are part of the design.

Measurement procedure

  1. A voltmeter’s input resistance appears in parallel with the lower resistor and lowers the measured output.
  2. Use a high-impedance meter, or account for its resistance when the divider resistors are comparable in value.
  3. Measure the input voltage and the output voltage together, since the input may sag when loaded.
  4. Check both resistors and the ground connection; an open upper resistor gives zero output, while an open lower resistor gives the full input.

Common mistakes

  • Ignoring the load and using the unloaded formula for a loaded output.
  • Swapping R₁ and R₂ when the output is expected across the other resistor.
  • Trying to power a load from a divider instead of using a regulator or buffer.
  • Choosing resistor values so high that the meter or load resistance dominates the result.

Safety considerations

  • A divider does not provide isolation from the input; the whole network may be at a hazardous potential.
  • Check the voltage rating of the resistors, especially in high-voltage dividers.
  • Allow for power dissipation in each resistor; an undersized resistor can overheat even in a low-current divider.

Frequently asked questions

Why does the output voltage drop when I connect a load?
The load is in parallel with the lower resistor, which reduces the effective lower resistance and therefore the output voltage.
Can I use a voltage divider as a power supply?
Only for very light, fixed loads. The output changes with load current, so a regulator or buffer is normally required.
How do I choose the resistor values?
Choose them so the divider current is large enough compared with the load or meter current, while keeping power dissipation and loading within acceptable limits.
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