This diode model is an improved version of the simple diode model. It includes a series resistance, parallel conductance, and also models reverse breakdown. The model is divided into three parts:
- lower half of reversed bias region including breakdown: -Ids·(exp(-(vd+Bv)/(N·Vt)) + 1 - 2·exp(-Bv/(2·N·Vt)))
- upper half of reverse biased region and forward biased region before conduction: Ids·(exp(vd/(N·Vt)) - 1)
- forward biased region after conduction: iVdMax + (vd - VdMax)·diVdMax
Temperature dependent behaviour is modelled when useHeatPort=true. In that case, the Vt parameter is ignored, and Vt is computed as k·T/q, where
- k is Boltzmann's constant
- T is the heat port temperature.
- q is the electron charge.
- November 2015
by Stefan Vorkoetter
implemented dynamic temperature dependency
- November 2015
by Kristin Majetta
defined parameter Vt based on fixed temperature
- June 2014
by Stefan Vorkoetter, Kristin Majetta, and Christoph Clauss
implemented
- October 2011
Stefan Vorkoetter - new model proposed.
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