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Bias Circuit

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The output-characteristic equation in the linear region corresponds to VDS ranging from the<br />

condition of Fig. 3.1(b) to that of Fig. 3.1(c). As VDS increases from zero, the channel begins to<br />

close off at the drain end (i.e., the channel becomes progressively more wedge shaped). The<br />

result is an increase in the resistance of the channel as a function of VDS, and therefore a<br />

sublinear current – voltage relation develops.<br />

When VGS > Vtno, the electron charge in the channel can be related to the gate voltage by Qchan<br />

= Cox(VGS – Vtno) (per unit area of MOSFET looking down at the gate), where Cox is the parallelplate<br />

capacitance (per unit area) formed by the MOS structure. This provides a simple linear<br />

relation between the gate voltage and the charge in the channel.<br />

The conductivity in the channel is σchan = µnQchan/tchan, where µn is the mobility of the electrons<br />

in the channel and tchan is the thickness of the channel into the semiconductor. Thus, in the<br />

case of a uniform channel (i.e., for VDS 0), the channel conductance is<br />

Equation 3.2<br />

where<br />

Equation 3.3<br />

and where KPn = µnCox is the SPICE transconductance parameter (the n subscript is the<br />

equation symbolic notation for the NMOS; the parameter in the device model is just KP), W is<br />

the physical gate width, and L, again, is the channel length. Parameter KPn is related to the<br />

electron mobility in the channel and the oxide thickness. Therefore, it is very specific to a<br />

given MOSFET device.<br />

As VDS increases, but is less than Veffn [transition from Fig. 3.1(b) to 3.1(c)], the wedge-shaped<br />

effect on the channel is reflected functionally in the channel conductance relation as<br />

Equation 3.4<br />

This leads to an output characteristic equation for the linear region, which is<br />

Equation 3.5<br />

The derivation leading to (3.4) and (3.5) is given in Unit 3.4. The linear-region relation, (3.5),<br />

is applicable for VDS up to VDS = Veffn, which is the boundary of the linear and active regions.<br />

The active-region equation is then obtained by substituting into (3.5), VDS = Veffn, giving<br />

Equation 3.6

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