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Obtain current Io in Fig. below using Norton’s theorem.

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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

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