As shown in Fig., 4 Ω resistance has been removed thereby open-circuiting the terminals A and B. We will now find VAB and RAB which will give us Vth and Rth respectively. The potential drop across 5Ω resistor can be found with the help of voltage-divider rule. Its value is
= 15 × 5/(5 + 10) = 5V.

For finding VAB, we will go from point B to point A in the clockwise direction and find the algebraic sum of the voltages met on the way.
∴ VAB = − 6 + 5 = − 1 V.
It means that point A is negative with respect to point E, or point B is at a higher potential than point A by one volt.
In Fig., the two voltage source have been short circuited. The resistance of the network as viewed from points A and B is the same as viewed from points A and C.
∴ RAB = RAC = 5 || 10 = 10/3 Ω
Thevenin’s equivalent source is shown in Fig. in which 4 Ω resistor has been joined back across terminals A and B. Polarity of the voltage source is worth nothing.

∴ I = 1/((10/3) + 4) = 3/22 = 0.136A