In the network shown below, remove terminal C and obtain the Norton equivalent seen at terminals a and b.
Vb−Va12+0.1+Vb−515=0
By solving, we get Vb=4V
VTh=−2V
RTh=12×1512+15=6.667Ω
and IN=VThRTh=−0.3A
In the circuit shown in the figure, the angular frequancy ω (in rad/s), at which the Norton equivalent impendance as seen from terminals b-b' is purely resistive, is