This  question is designed to give you practice in manipulating circuit  equations using j notation, and to demonstrate that techniques that you  have already studied in the d.c. context can be applied equally  successfully to the solution of steady-state a.c. problems.

The  sketch (right) shows the approximate equivalent circuit of a real  transformer (inside the dotted line) with its parameters referred to the  primary side, and with a referred load resistance of 5 ω. Find
(a) the  open-circuit voltage VL , and
(b) the voltage across the 5 ω 'referred' load, by the following three methods.
 Method  1: Direct approach. First find the open circuit voltage by simple  'potential divider' approach (but with complex impedances Z replacing  the simple resistances we used under d.c. conditions). Then find the  equivalent series impedance of the two parallel branches on the right,  and again use the 'potential divider' idea to find VL. The calculations are lengthy, and you will probably find it best to use polar form for the multiplications and divisions.
Method  2: Thévenin. Find the Thévenin equivalent circuit for the transformer  and 100 V supply. Then apply the load and use the potential divider  approach.
Method  3: Nodal Analysis. Call the node at the top of j35 node a and that at  the top of the 5 ω load node b, with the reference (zero) node at the  bottom. Write down the nodal equations in terms of the complex  impedances, and solve for Vb.
Calculate  the % change in the output voltage when the load is applied (this is  known, as the 'regulation'). What would you expect the regulation to be  if the transformer were ideal?