3.8367
V
3.8367
V
0.000816
A
6.6639
mW
0
%
3.8367
V
3.8367
V
0.000816
A
6.6639
mW
0
%
The voltage divider is one of the most fundamental and widely used circuits in electronics. Two resistors in series, connected between a supply voltage and ground, produce an output voltage at their junction proportional to the resistance ratio: Vout = Vin × R2 / (R1 + R2). Simple, elegant, and requiring no active components, voltage dividers appear in virtually every electronic circuit as biasing networks, reference voltage generators, signal attenuators, and level shifters.
The voltage divider principle follows directly from Kirchhoff's Voltage Law and Ohm's Law. With the same current flowing through both series resistors (I = Vin / (R1 + R2)), the voltage drop across R2 equals I × R2 = Vin × R2/(R1+R2). The ratio R2/(R1+R2) is the divider ratio — ranging from 0 (when R2 = 0) to 1 (when R1 = 0). Any intermediate voltage between 0 and Vin is achievable by selecting the appropriate ratio.
The unloaded voltage divider is ideal — it produces exactly Vout = Vin × R2/(R1+R2) when no current is drawn from the output node. However, connecting a load resistance RL across R2 changes the effective bottom resistance to R2||RL = (R2 × RL)/(R2 + RL), reducing Vout below the unloaded value. This 'loading effect' is a critical practical consideration: for the divider to maintain accurate output voltage, the load resistance should be much larger than R2 (typically RL ≥ 10 × R2 for less than 10% error).
Choosing divider resistor values involves balancing two competing requirements: lower resistance values minimize loading error but increase quiescent current and power dissipation; higher resistance values reduce power waste but increase susceptibility to loading by the downstream circuit. A practical rule of thumb: set divider current to 10× the maximum load current expected, keeping loading error below 10%. For precision reference dividers, use 0.1% tolerance resistors and keep divider current high relative to load current.
Voltage dividers are used for: ADC input voltage scaling (5 V signal to 3.3 V MCU input); battery voltage monitoring (scaling high voltage to ADC range); transistor base biasing (establishing operating point); DAC output attenuation; audio pot (potentiometer) volume controls; and in Wheatstone bridge sensor circuits where four resistors form two voltage dividers that are compared for differential measurement.
This calculator provides both unloaded and loaded output voltages, along with divider current, power dissipation in R1, and loading error percentage — giving a complete picture of voltage divider performance under practical operating conditions.
Unloaded: Vout = Vin × R2 / (R1+R2). Loaded: R2_eff = R2||RL = (R2×RL)/(R2+RL); Vout_loaded = Vin × R2_eff / (R1 + R2_eff). Divider current I = Vin/(R1+R2). Power in R1: P = I² × R1 (in mW). Loading error % = |Vout_unloaded − Vout_loaded| / Vout_unloaded × 100. Enter RL = 0 for no-load condition.
Loading error < 1%: use RL ≥ 100 × R2. Loading error < 10%: use RL ≥ 10 × R2. Large loading error means R2 is too high relative to RL — reduce both R1 and R2 proportionally while keeping the ratio the same. Higher divider current reduces loading but increases power dissipation — balance for your application's power budget.
Inputs
Results
R1=10k, R2=15k divides 5V to 3.0V unloaded. With 100k load: Vout drops to 2.86V (4.8% error). For 1% error, use RL ≥ 1,500 kΩ or reduce R1/R2 to 1k/1.5k.
Inputs
Results
100kΩ/33kΩ divider scales 12V battery to 2.97V for a 3.3V ADC input. With no external load (ADC input impedance >> 33k), quiescent current is only 90 µA, drawing < 1 mW — acceptable for battery-powered designs.
The Thevenin equivalent of a voltage divider is: V_th = Vin × R2/(R1+R2) (Thevenin voltage) and R_th = R1||R2 = (R1×R2)/(R1+R2) (Thevenin resistance). Any load connected to the divider output 'sees' a voltage source V_th with internal resistance R_th. For stable output voltage, R_load >> R_th.
A potentiometer is a three-terminal variable voltage divider with a sliding wiper contact. Rotating the wiper changes the R1/R2 ratio continuously from 0 to 1. Used as volume controls, position sensors, and manual adjustment controls. A rheostat uses only two terminals (wiper + one end) as a variable resistor rather than a full divider.
1) Calculate required ratio: ratio = Vout/Vin. 2) Select R2 to be 10–100× smaller than expected load resistance. 3) Calculate R1 = R2 × (Vin/Vout − 1). 4) Round to nearest E24 standard values. 5) Verify power dissipation (P = Vin²/(R1+R2)) is within resistor ratings. 6) Check loading error with actual load resistance.
BJT bias: two resistors from supply to ground set the base voltage. V_B = Vcc × R2/(R1+R2). For stable biasing (stiff divider): I_divider ≥ 10 × I_base. V_E = V_B − 0.7 V, I_C ≈ I_E = V_E/R_E. This four-resistor (R1, R2, RC, RE) bias circuit provides stable operating point independent of transistor beta variations.
A voltage divider produces a specific output voltage ratio. An attenuator (typically L-pad, T-pad, or π-pad) is designed for specific input and output impedances while providing a given attenuation ratio — crucial for RF and audio systems where maintaining 50 Ω or 600 Ω impedance matching matters. Simple voltage dividers don't control impedance; attenuators do.
Only for loads much larger than the divider resistance (no significant current draw). For applications requiring stable reference voltage independent of load current changes, use a dedicated voltage reference IC (LM4040, LM336) or an LDO regulator instead. These provide temperature compensation, low output impedance, and load regulation that a passive divider cannot match.
Roboculator Team
The Roboculator Team explains calculations, planning tools, and practical formulas in clear language for real-life situations.
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