MOSFET (the BJT) as an amplifier: when the transistor is operated in the active region, $V_{GS}$ controls $i_D$ ($V_{BE}$ controls $i_C$) in the manner of a voltage-controlled current source.
Fundamental parameter is characterizing the small-signal linear operation is transconductance $g_m$
For a MOSFET:
$$ g_m = \mu n C{ox} (W/L) V_{ov} \newline = \sqrt{2 \mu n C{ox}(W/L)I_D} \newline = \frac{2I_D}{V_{ov}} $$
For the BJT:
$$ g_m = \frac{I_C}{V_T} $$
Transconductance $(g_m)$: represents the control of the gate-source voltage $V_{GS}$ has on the drain current $I_D$ in a MOSFET, or the base-emitter voltage $V_{BE}$ on the collector current $I_C$ in a BJT
Output resistance $(r_o)$: ****Models effect of channel-length modulation in MOSFETs or Early effect in BJTs
Input resistance $(r_{\pi})$ or $(r_{in})$: ****For BJTs, $r_{\pi}$ is the dynamic resistance at the base-emitter junction, and is derived as $r_{\pi} = \frac{\beta}{g_m}$