Concept:
For a field-effect transistor (FET) under certain operating conditions, the resistance of the drain-source channel is a function of the gate-source voltage alone and the JFET will behave as an almost pure ohmic resistor
For a MOSFET in the saturation region:
VGS > Vth and
VDS > VGS – Vth
The current equation for a MOSFET in the saturation region is given by:
\({{I}_{D}}=\mu C_{ox} \frac{W}{2L}\left\{\left( {{V}_{GS}}-{{V}_{th}} \right)^2\right\}\)
Taking the derivative of the above w.r.t. VDS, we get:
\(\frac{\partial I_D}{\partial V_{DS}}=\mu C_{ox}\left( {\frac{W}{L}} \right)\left( {{V_{GS}} - {V_{TH}}} \right)\)
Voltage-controlled Resistor (rDS) is defined as:
\({r_{DS}} = \frac{{{V_{DS}}}}{{{I_{DS}}}} = \frac{1}{{{\mu _n}{C_{ox}}\left( {\frac{W}{L}} \right)\left( {{V_{GS}} - {V_{TH}}} \right)}}\)
Calculation:
Given:
VGS = 2.0 V,
VTH = -0.5 V,
\(\frac{W}{L} = 100\)
Cox = 10-8 f/cm2
μn = 800 cm2/V-s,
VDS = 5 V
Putting on the respective values in Equation (1), we get:
\({r_{DS}} = \frac{1}{{800 \times {{10}^{ - 8}} \times 100 \times \left( {2 - \left( { - 0.5} \right)} \right)}}\)
\({r_{DS}} = 500\;{\rm{\Omega }}\)