The distributor circuit is shown in Fig.(a). Currents in various sections are as shown. First, consider the load at point B acting alone as in Fig.(b). The input current at point A divides in the inverse ratio of the impedances of the two paths A B and ACB.
Let the currents be I1′ and I2′
Now, consider the load at point C to act alone as shown in Fig. (c). Let the currents now be I1″ and I2″.
As per Superposition theorem, the current I1 in section A B is the vector sum of I1′ and I1″
Potential of B = 400 – drop over A B
= 400 − (19.5 − j16.5)(1 + j2) = 347.5 − j22.5 = 348 ∠ −3.7°V
Potential of C = 400 − (14.5 − j19.5)(1 + j3) = 327 − j24 = 328 ∠−4.2°V