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.
Generated at 2020-06-05T21:39:08Z by OpenModelica 1.16.0~dev-442-g2e5bc9f