2026-04-29
Every linear circuit, no matter how tangled, can be reduced to a single voltage source in series with a single resistor (Thevenin) or a single current source in parallel with a single resistor (Norton). This isn't just a textbook trick — it's the most powerful analysis tool you'll use when designing real circuits.
Why it matters: When you connect a sensor to an amplifier, or an amplifier to a speaker, you need to know how the source circuit will behave under load. Thevenin's theorem lets you collapse everything upstream into two numbers: Vth (open-circuit voltage) and Rth (output impedance). That's all the load ever "sees."
Finding the Thevenin equivalent:
Norton is just the dual: IN = Vth / Rth, and the Norton resistance equals Rth. You can convert freely between the two forms.
Real-world example: You have a resistive voltage divider — 10kΩ on top, 20kΩ on bottom — fed by 12V. You want to know what happens when you connect a 10kΩ load across the bottom resistor. Instead of re-solving the whole network, find the Thevenin equivalent at the output:
Now your circuit is just 8V in series with 6.67kΩ driving a 10kΩ load. The loaded output voltage is 8V × 10k / (6.67k + 10k) = 4.8V — a significant drop from the unloaded 8V. This immediately tells you the divider is too weak (Rth too high) for that load. You'd either need lower-value resistors or a buffer amplifier.
Rule of thumb: To keep loading effects under 10%, make Rload at least 10× Rth. In the example above, you'd want a load of at least 67kΩ to preserve the divider voltage.
Where you'll use this constantly:
