Loads halve your bottom leg
Any load on Vout sits in parallel with R2. A 10 kΩ R2 feeding a 10 kΩ load behaves like 5 kΩ, pulling Vout down by ~2×.
Ideal (no load):
$$ V_{out} = V_{in} \cdot \frac{R_2}{R_1 + R_2} $$
Rearrangements:
Divider current (no load): \( I_{div} = \dfrac{V_{in}}{R_1 + R_2} \). Power: \( P_1 = I_{div}^2 R_1 \), \( P_2 = I_{div}^2 R_2 \).
Rule of thumb: make divider current ≳10× the input bias current of what you’re driving, or buffer the node.
A voltage divider is one of the most fundamental building blocks in electronics. It is created by connecting two resistors in series across a voltage supply and taking the output from the junction between them. The ratio of the two resistances determines how the input voltage (Vin) is divided into a smaller output voltage (Vout). The simplicity of this circuit makes it an essential tool for engineers, hobbyists, and students learning about circuits.
The key idea is proportionality: the output voltage depends on the fraction of total resistance contributed by the lower resistor (R2). Mathematically, this is expressed as \( V_{out} = V_{in} \times \dfrac{R2}{R1 + R2} \). This formula highlights why the voltage divider is so flexible—by choosing appropriate values for R1 and R2, you can generate almost any intermediate voltage between zero and the input supply.
In practice, voltage dividers are used in many applications:
While useful, voltage dividers have limitations. They are not suitable for supplying significant power to a load because the output voltage drops if the connected device draws current. That is why dividers are best for measurement and signal purposes rather than powering circuits. To overcome this, designers often buffer the output with an operational amplifier or use a dedicated voltage regulator.
Understanding voltage dividers not only helps with practical circuit design but also builds intuition about how resistance, current, and voltage interact. They serve as a stepping stone toward mastering more complex networks, Thevenin equivalents, and real-world power management. Whether you are working on robotics, audio electronics, or embedded systems, the voltage divider is a concept you will use repeatedly.
Any load on Vout sits in parallel with R2. A 10 kΩ R2 feeding a 10 kΩ load behaves like 5 kΩ, pulling Vout down by ~2×.
Scale R1 and R2 up or down by the same factor and Vout/Vin stays identical; only current and resistor power change.
Make divider current at least ~10× the input bias current of what you’re driving (ADC pin, op-amp). If not, buffering beats guessing.
1% resistors rarely give 1% Vout; worst-case error is set by the ratio. A +1% R1 with -1% R2 skews Vout by ~2%.
Feeding a noisy, high-impedance divider into an LDO’s sense pin can cause oscillations. Many regulators require a minimum load or a low-impedance feedback network.