A voltage divider is one of the simplest and most widely used circuits in electronics. It uses two resistors in series to convert an input voltage into a lower output voltage. This calculator lets you enter the input voltage and resistor values (R1 and R2) and immediately see the resulting output voltage at the junction between the two resistors.
Use this tool when you want to design simple level shifters, bias points for analog circuits, or quick reference voltages. By experimenting with different resistor ratios, you can quickly understand how each parameter affects the output.
Directly above or beside this explanation, you should see the calculator interface with three inputs:
The calculator assumes an ideal, unloaded voltage divider, which is a very common and useful approximation for many signal-level applications. The sections below explain how the divider works, show the key formulas, and outline the assumptions and limitations you should keep in mind.
A basic voltage divider consists of two resistors, R1 and R2, connected in series across an input voltage source, Vin. The output voltage, Vout, is taken from the node between R1 and R2, relative to the lower reference node (usually ground).
Because the resistors are in series, the same current flows through both of them. The total resistance seen by the source is R1 + R2. According to Ohm’s law, the current I through the series combination is:
I = V_in / (R1 + R2)
The output voltage is just the voltage drop across R2. Since the current through R2 is I, the drop across R2 is:
V_out = I × R2
Substituting the expression for I into this equation gives the classic voltage divider formula.
The standard ideal voltage divider relationship is:
In plain text form:
V_out = (R2 / (R1 + R2)) × V_in
This shows that the output voltage depends only on the ratio of R2 to the total resistance, multiplied by the input voltage. If R2 is small compared with R1, the output will be a small fraction of Vin. If R2 is large compared with R1, the output will be close to Vin.
The same expression also gives you the series current:
I = V_in / (R1 + R2)
Once you know Vout and I, you can work out power dissipation in each resistor using:
P_R1 = I² × R1P_R2 = I² × R2These relationships are useful when you want to ensure that your chosen resistor values will not overheat in operation.
After entering Vin, R1, and R2 into the calculator and running the computation, you will typically see at least one primary result:
Conceptually, you can think of the divider in either of two ways when you interpret this number:
If you increase R1 while holding R2 and Vin constant, the denominator (R1 + R2) increases, so the ratio R2 / (R1 + R2) decreases. The calculator will show a lower Vout. Conversely, increasing R2 while keeping R1 constant will increase Vout, bringing it closer to Vin.
When you interpret the result, it is essential to remember that the formula assumes the output is feeding a very high-impedance input (that is, almost no current is drawn from Vout). The Assumptions and Limitations section below expands on this point.
This example mirrors a common microcontroller scenario: scaling a 5 V signal down to approximately 3 V for an input that cannot tolerate the full 5 V level.
Using the formula:
V_out = (R2 / (R1 + R2)) × V_in = (3000 / (2000 + 3000)) × 5 V
The sum R1 + R2 is 5000 Ω, so:
V_out = (3000 / 5000) × 5 V = 0.6 × 5 V = 3 V
The calculator should show an output close to 3 V. This is suitable for many devices that expect a nominal 3.3 V logic level, provided their absolute maximum rating is at or above 3 V and other design constraints are satisfied.
If you keep Vin = 5 V and R2 = 3 kΩ but change R1 to 1 kΩ (1000 Ω), then:
V_out = (3000 / (1000 + 3000)) × 5 V = (3000 / 4000) × 5 V = 0.75 × 5 V = 3.75 V
By comparing these two cases, you can see how the R2 / (R1 + R2) ratio controls the output voltage. Small changes in the ratio lead to proportional changes in Vout.
The table below summarizes some typical voltage divider configurations to illustrate how different resistor ratios affect the output voltage. All examples assume an ideal, unloaded divider.
| Vin (V) | R1 (Ω) | R2 (Ω) | Vout (V) | Primary Use Case |
|---|---|---|---|---|
| 5 | 2,000 | 3,000 | 3.0 | Level shifting 5 V logic down near 3 V |
| 5 | 10,000 | 10,000 | 2.5 | Mid-supply reference for op-amp circuits |
| 12 | 47,000 | 10,000 | 2.11 | Scaling a 12 V signal into an ADC input range |
| 3.3 | 1,000 | 2,000 | 2.2 | Biasing a transistor base or MOSFET gate |
| 24 | 100,000 | 10,000 | 2.18 | Monitoring an industrial 24 V rail with a microcontroller |
These examples highlight two important design levers:
Voltage dividers are used across many areas of electronics. Common applications include:
In all of these cases, the divider is usually feeding a high-impedance input (for instance, the input pin of an ADC or op-amp), so that the loading on the divider is minimal and the ideal formulas remain accurate.
The calculator is based on an ideal model of a voltage divider. When you interpret the results and apply them to real circuits, it is important to understand the assumptions behind the math:
One of the most important practical limitations is loading. If you connect a low-impedance load (such as a motor or another resistor of similar magnitude to R2) to Vout, then R2 and the load form a parallel combination. The effective resistance seen in the divider formula becomes smaller than R2 alone, which reduces Vout compared with the ideal prediction.
Because of this, voltage dividers are generally not recommended for powering devices that draw substantial current, such as motors, LEDs without series resistors, or entire boards. They are best reserved for signal-level tasks, where currents are tiny and the loading of Vout is negligible.
For robust designs, always check:
When choosing resistor values for a real-world voltage divider:
The calculator gives you the ideal Vout. Combine that result with these checks to produce a design that is both accurate and reliable.
In most cases, no. A voltage divider is poor at supplying power to loads that draw significant current because the output voltage will drop as the load current increases. Use a regulator or dedicated power supply instead, and reserve voltage dividers for low-current signal applications.
Resistor tolerances cause the actual values of R1 and R2 to deviate from their nominal values. This changes the ratio R2 / (R1 + R2) and therefore shifts Vout. For precision applications, use tighter tolerance parts (for example, 1% metal film resistors) and, if necessary, account for worst-case combinations in your design calculations.
Unless the interface specifically supports suffixes, enter all resistor values in ohms as plain numbers. For example, 2 kΩ becomes 2000, 47 kΩ becomes 47000, and 1 MΩ becomes 1000000. The electrical behavior depends only on the numeric ratio, not the units, as long as both R1 and R2 are expressed in the same unit.
Playable attenuation study
Hold Vout inside a moving band for ~80 seconds. Nudge R1 and R2 while drift and jitter push the divider around. Feel how Vout = Vin · R2 / (R1 + R2) responds to tiny tweaks.
Controls
A/D or ←/→ tune R1. W/S or ↑/↓ tune R2. Touch buttons mirror these moves. Keep the teal band hugging the cyan rails to build streak heat.
Higher R2 or lower R1 lifts Vout, but total resistance changes current and power—mind the tradeoff.