As explained in , we will replace the 6Ω resistance by a short-circuit as shown in Fig.. Now, we have to find the current passing through the short-circuited terminals A and B. For this purpose we will use the mesh analysis by assuming mesh currents I1 and I2.
From mesh (i), we get
3 − 4 I1 − 4 (I1 − I2) + 5 = 0 or 2 I1 − I2 = 2 ...(i)
From mesh (ii), we get
− 2 I2 − 4 − 5 − 4 (I2 − I1) = 0 or 4I1 − 6I2 = 9 ...(ii)
From (i) and (ii) above, we get I2 = − 5/4
The negative sign shows that the actual direction of flow of I2 is opposite to that shown in Fig. . Hence, Ish = IN = I2 = − 5/4 A i.e. current flows from point B to A.
After the terminals A and B are open-circuited and the three batteries are replaced by short circuits (since their internal resistances are zero), the internal resistance of the circuit, as viewed from these terminals’ is
Ri = RN = 2 + 4 || 4 = 4 Ω
The Norton’s equivalent circuit consists of a constant current source of 5/4 A in parallel with a resistance of 4 Ω as shown in Fig. . When 6 Ω resistance is connected across the equivalent circuit, current through it can be found by the current-divider rule (Art).
Current through 6 Ω resistor = 5/4 x 4/10 = 0.5 from B to A.