Common emitter amplifier with voltage divider bias with bypassed emitter resistance with ac equivalent circuit is as shown in fig 4.7(b).
The hybrid π equivalent circuit is as shown below
For voltage gain $A_vs$:
$A_vs = \frac{V_o}{Vs}$
$V_o$ is voltage developed across ($r_o ||R_C ||R_L $) due to current $g_m V_π.$
$V_o= -g_m V_π(r_o ||R_C ||R_L )$
$V_π$ = Voltage across $R'_i$ where $R'_i$ = $R_B ||r_π$
$V_π= \frac{(R_B ||r_π)}{(R_S+R_B ||r_π )} x V_S$ …… ($R_B = R_1 ||R_2$)
$V_S= \frac{(R_S+R_B ||r_π)}{(R_B ||r_π )} x V_π$
Substituting value of $V_o$ and $V_S$ into $A_vs$ formula,
$A_vs = \frac{(-g_m V_π (r_o ||R_C ||R_L )}{([ R_S+R_B |├|r_π ] V_π )} x (R_B ||r_π)
$A_vs = -g_m (r_o ||R_C || R_L ) x \frac{(R_B ||r_π)}{([ R_S+R_B |├|r_π ] V_π )}$
For input resistance $R'_i$:
$R'_i= R_B ||r_π= R_1 ||R_2 ||r_π$
For output resistance $R'_o$:
The output resistance is obtained by setting $V_S$ to 0. As $V_S$ = 0, $V_π$ = 0. Hence $g_m V_π$= 0 and the hybrid circuit modified as shown in fig 4.9 below.
![enter image description here][3]
$R'_o = r_o ||R_C || R_L$
For current gain ($A_IS $):
$A_IS = \frac{I_o}{I_i}$
Refer fig above,
![enter image description here][4]
Consider current division at node A. The current $g_(m ) V_π$ is divided between $r_(o ) ||R_(C )and R_L.$
By using current division rule,
$I_o = \frac{(-g_m V_π (r_o ) ||R_C ))}{(r_o |├|R_C )+ R_L )}$
$I_b$ is obtained by current division rule at node B.
$I_b = \frac{R_B}{(R_B+ r_π )} x I_i$
$V_π = \frac{(R_B r_π)}{(R_B+ r_π )} x I_i = (R_B || r_π) I_i$
Substitute value of $V_π$ for getting $I_o$,
$I_o = (-g_(m ) [(R_B || r_π) I_i ] \frac{(r_(o ) ||R_(C )) )}{( (r_(o ) |├|R_(C ) )+ R_L )}$
Hence current gain is $A_IS = \frac{I_o}{I_i} = (-g_m r_o ||R_C) \frac{(R_B || r_π))}{(R_L+ (r_(o ) |├|R_(C ) ) )}$