Our first objective is to find the Norton equivalent at terminals a-b. ZNis found in the same way as ZTh. We set the sources to zero as shownin Fig. (a). As evident from the figure, the (8 − j2) and (10 + j4)impedances are short-circuited, so that
ZN= 5Ω To get IN, we short-circuit terminals a-b as in Fig. (b) and apply mesh analysis. Notice that meshes 2 and 3 form a supermesh because of the current source linking them. For mesh 1,
-j40 + (18 +j2) I1 - (8 – j2) I2 - (10 + j4) I3 =0 …(1)
For the supermesh,
(13- j2)I2 + (10 + j4) I3 – (18 + j2) I1 = 0 …(2)

At node a, due to the current source between meshes 2 and 3,
I3= I2+ 3 …(3)
Adding Eqs. (1) and (2) gives
−j40 + 5I2= 0 ⇒I2= j8
From Eq.(3),
I3= I2+ 3 = 3 + j8
The Norton current is
IN= I3= (3 + j8) A
Figure (c) shows the Norton equivalent circuit along with the impedanceat terminals a-b. By current division
