For the JFET drain characteristics of Fig. 4-2(a), take v_{DS} as the dependent variable [so that v_{DS} = f (v_{GS}, i_D)] and derive the voltage-source small-signal model.
For small variations about a Q point, the chain rule gives
v_{d s} = \Delta v_{D S} \approx d v_{D S} = {\frac{\partial v_{D S}}{\partial v_{G S}}}\bigg|_{Q} v_{g s} + {\frac{\partial v_{D S}}{\partial i_{D}}}\bigg|_{Q}\bigg. i_d (1)
Now we may define
\left.{\frac{\partial v_{D S}}{\partial v_{G S}}}\right|_{Q} = \mu \qquad {\mathrm{and}} \qquad \left.{\frac{\partial v_{D S}}{\partial i_{D}}}\right|_{Q} = r_{ds}
If the JFET operates in the pinchoff region, then gate current is negligible and (1) is satisfied by the equivalent circuit of Fig. 7-1(b).