With conventional electric current defined into the positive terminal, an ideal junction has
The reverse-bias branch tends to before breakdown. In forward bias the electric current rises exponentially; a visibly sharp “turn-on” is a convenient operating description rather than a discontinuity in the equation. A powered LED emits in quadrant I, where , and the device absorbs electrical power . Strong reverse breakdown lies outside the ideal curve below.
Figure 1.
Ideal diode characteristic with reverse saturation and forward LED operation
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