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MOS equations

The well known equations for the MOS transistors are (for the n-type and p-type transistors)[1]:

below saturation

$\displaystyle I_{DSn,p} = \beta_{n,p}\left[(V_{GS}-V_{T_{n,p}})V_{DS}-\frac{V_{DS}^2}{2}\right]$ (4.2)

above saturation

$\displaystyle I_{DS_{n,p}}=\frac{\beta_{n,p}}{2}\left[V_{DSsat_{n,p}}\right]^2$ (4.3)

where $ \beta_{n,p} = \frac{\mu_{n,p}C_{ox}W}{L}$, with $ \mu_{n,p}$ modified by the carrier velocity saturation effect:

$\displaystyle \mu_n = \frac{\mu_{n0}}{1+\frac{V_{DS}}{L {\mathcal E}_{c}}} \quad \mu_p = \frac{\mu_{p0}}{1-\frac{V_{DS}}{L {\mathcal E}_{c} }}$    

The saturation voltage (drain-source), not including the carrier velocity saturation effect, is given by the well known formula:

$\displaystyle V_{DS_{n,p}} = V_{GS_{n,p}}-V_{T_{n,p}}$    

while considering the effect above-mentioned:

$\displaystyle V_{DS_{n,p}} = \pm V_c \left[\sqrt{1\pm \frac{2(V_{GS_{n,p}}-V_{T_{n,p}})}{V_c}} - 1\right]$ (4.4)

where the plus signs are for n-MOSFETs and the minus signs are for the p-MOSFETs, and $ V_c = \vert{\mathcal E}_{c} L\vert$


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