Sensors & Signal Conditioning

a photodiode

/ FOH-toh-DY-ohd /

A photodiode is a diode that has been turned into a light meter. An ordinary diode is sealed in black plastic precisely so light cannot reach its junction; a photodiode is given a clear window for the opposite reason. When light lands on its PN junction, the photons knock electrons loose and a small current flows. More light, more current — a remarkably honest, linear translation from brightness into a number.

The key fact is that a photodiode produces a current, not a voltage, and that current is proportional to the light hitting it over an enormous range — many decades of brightness. The current is small: a typical part gives perhaps 0.5 amps per watt of incoming light, and real signals are often nanoamps to microamps. Because current is awkward to read directly, a photodiode is almost always paired with a transimpedance amplifier — an op-amp that converts current into a proportional voltage. Run the diode in reverse-bias (photoconductive mode) for speed, or at zero bias (photovoltaic mode) for the lowest noise and offset. A phototransistor is a cousin that adds built-in gain: more sensitive but slower and less linear.

Why this matters: photodiodes are the eyes of countless systems — pulse oximeters, laser power meters, optical fiber receivers, barcode scanners, camera light sensors, and the receiving half of every TV remote. The honest caveats: the raw current is tiny, so the transimpedance stage's noise, bias current, and stray capacitance dominate performance and demand care; the diode also responds to its own dark current and to infrared you cannot see, so filters and good shielding matter. Get the current-to-voltage conversion right and a photodiode is one of the most linear sensors you will ever use.

A photodiode lit by a small lamp produces 2 microamps of current. Feed it into a transimpedance amplifier with a 1 MΩ feedback resistor and the output becomes 2 uA times 1 MΩ = 2 V. Double the light to 4 uA and the output cleanly doubles to 4 V — current in, proportional voltage out.

Light makes current; a transimpedance amplifier turns it into a voltage.

A photodiode is a current source, not a voltage source — trying to read its voltage across a resistor is nonlinear and noisy. Convert its current to voltage with a transimpedance amplifier to get the clean, linear response it is famous for.

Also called
photodetector光檢測器光偵測二極體