Model Equations
Equivalent Circuit

Ids Equations
For the symmetric model (idsmod=1)
MA Model
phi1=P1m*((Vgs-Vpkm) + P2*(Veffp1)2+P3*(Veffp1)3+P2*(Veffp2)2+P3(Veffp2)3
ph1=P1m * Veffp1 + P2*(Veffp1)2 + P3*(Veffp1)3
ph2=P1m * Veffp2 + P2*(Veffp2)2 + P3*(Veffp2)3
Ids1=IPK0*(1+tanh(ph1) + tanh(ph2))
Igs and Igd Equations
Temperature Equations
Charge Equations
Cgs = CGSP
Cgd = CGDP
Qgs = CGSP * Vgsc
Qgd = CGDP * Vgdc
Cgs = CGSP+CGS0 x ( 1 + tanh(Phi1))( 1 + tanh(Phi2))
Cgd = CGDP + CGD0 x ((1 - P111 + tanh(Phi3)) (1 + tanh(Phi4)) + 2 x P111)
Qgs = CGSP x Vgsc
Qgd = CGDP x Vgdc
Lc1 = 1n(cosh(Phi1))
Lc10 = ln(cosh(P10 + P11 X Vds))
Qgs = CGSP x Vgsc + CGS0 x ((Phi1 + Lc1 - Qgs0) x (1 + tanh(Phi2)) / P11 + 2 x P111 x Vgsc
Qgs0 = P10 + P111 x Vds + Lc10
Lc4 = 1n(cosh(Phi4))
Lc40 = 1n(cosh(P40 -P111 x Vds))
Qgd = CGDP x Vgdc + CGD0 x ((Phi4 + Lc4 - Qgd0) x (1 - P111 + tanh(Phi3)) / P41 + 2 x P111 x Vgdc
Qgd0 = P40 - P111 x Vds + Lc40
Excess Phase
In an actual device, the measured phase shift is often larger than the shift predicted by the lumped model. The excess-phase parameter td accounts for this extra phase shift at high frequencies. An all-pass, second-order Bessel function filter creates this extra phase shift. The frequency response of this filter is:

The Bessel filter is implemented with the excess phase network, as shown in the figure below.

Self Heating Model
The power used for the self-heating model is given by:
Noise Model
Broadband Noise:

Parameters NoiseP, NoiseR, and NoiseC model the drain and gate noise sources, and their correlation.



Igs, Igd Shot Noise and Flicker Noise


Ids Flicker Noise



Thermal Noise
Thermal noise of resistances Rgd, Rd, Rg, and Rs


Related Topics
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