Darlington Pair: The Classic High-Gain Compound Transistor and Its Hidden Costs

2026-08-20

The Darlington pair is two BJTs wired so the emitter of the first drives the base of the second, both collectors tied together. The result is a compound transistor with a current gain roughly equal to the product of the individual betas: βtotal ≈ β1 × β2. Two ordinary transistors with β=100 each give you a compound device with β≈10,000. That's why Darlingtons dominated relay drivers, audio output stages, and solenoid switches for decades before power MOSFETs took over.

The circuit: Q1's collector connects to Q2's collector (the output). Q1's emitter feeds Q2's base directly. Q1's base is the input. Base current entering Q1 gets multiplied by β1 at Q1's emitter, which then becomes Q2's base current, multiplied again by β2. Tiny drive currents control large loads — a 100 µA input can switch 1 A of collector current.

Real-world example: The venerable TIP120 (NPN Darlington, TO-220 package) can switch 5 A at 60 V with a spec'd hFE of 1000. A microcontroller GPIO pushing 5 mA through a base resistor can drive a 12 V automotive relay coil pulling 200 mA with margin to spare — no gate driver, no charge pump, no fuss. This is why every 1980s-era motor controller and every hobbyist "arduino relay board" uses one.

The hidden costs — and there are three big ones:

Rule of thumb: Budget 1 V × Iload of dissipation for any Darlington output stage. At 1 A that's 1 W — manageable with a small heatsink. At 5 A it's 5 W and you need serious thermal design. If your load exceeds ~500 mA and efficiency matters, skip the Darlington and use a logic-level MOSFET instead.

Key Takeaway: Darlington pairs multiply current gain but pay for it with doubled VBE, ~1 V saturation drop, and sluggish turn-off — great for legacy relay drivers, wrong for modern high-efficiency switching.

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