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AN2657 Datasheet(PDF) 7 Page - STMicroelectronics |
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AN2657 Datasheet(HTML) 7 Page - STMicroelectronics |
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7 / 18 page ![]() AN2657 Model description and parameter extraction 7/18 L is the physical channel length of the MOS, while L0 influences the output conductance which depends on KE and EPS. DEL and DELVG affect the VDSAT and are extracted from the output characteristics in the saturation region. As mentioned previously, all the equations have been implemented in verilog language. JFET resistance The quasi-saturation region is modeled by a nonlinear JFET resistor. The mathematical empirical equation is defined in Equation 12, where pres depends on the current and on the drop voltage across Rj. Equation 12 Figure 2. Rjfet vs. Vds Useful to delete any convergence problem, Figure 2 shows the resistor law for the variation of Vds (using the right hand function approach) (Equation 13). A similar graph and function can be obtained by varying Vgs [3]. Equation 13 The function g(pres) was created to bind the Rj to the current Id. This is accomplished by introducing a new parameter linked to the dissipated power on Rj (Equation 14), where pres is linked to the dissipated power on Rj through RPWR. Equation 14 h(T) (Equation 15), introduces the temperature dependence of Rj, where TCR1 and TCR2 are temperature coefficients in the linear region. Rj is extracted from the DC output characteristics in the linear region with high bias current. R j fVds Vgs , () gpres () hT () ⋅ ⋅ = R j Vds () RI0 SR FSI Log 10 110 Vds VDI – FSI ---------------------------- + ⎝⎠ ⎜⎟ ⎛⎞ FSF Log 10 110 Vds VDF – FSF ------------------------------ + ⎝⎠ ⎜⎟ ⎛⎞ ⋅ – ⋅ ⋅ + = gpres () 1 PCR1 PCR2 pres ⋅ + () pres ⋅ + = |
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