Question 9.14: The load impedance connected to the secondary winding of the...

The load impedance connected to the secondary winding of the ideal transformer in Fig. 9.45 consists of a 237.5 m Ω resistor in series with a 125 μH inductor. If the sinusoidal voltage source \left( v_{g}\right) is generating the voltage 2500\cos 400t V, find the steady-state expressions for:(a) i_{1} ; (b) v_{1} ; (c) i_{2} ; and (d) v_{2};

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a) We begin by constructing the phasor domain equivalent circuit. The voltage source becomes 2500\angle 0^{\circ} V; the 5 mH inductor converts to an impedance of j2 Ω and the 125 μH inductor converts to an impedance of j0.05 Ω . The phasor domain equivalent circuit is shown in Fig. 9.46.
It follows directly from Fig. 9.46 that

2500\angle 0^{\circ}= (0.25 + j 2)\pmb{I}_{1} +\pmb{V}_{1},

and

\pmb {V}_{1}= 10\pmb {V}_{2} = 10\left[\left(0.2375 + j0.05\right)\pmb{I}_{2}\right].

Because

\pmb{I}_{2}=10\pmb{I}_{1}

we have

\pmb {V}_{1}= 10(0.2375 + j0.05)10\pmb{I}_{1}

= \left(23.75 + j5\right)\pmb{I}_{1}.

Therefore

2500\angle 0^{\circ}= (24 + j 7)\pmb{I}_{1},

or

\pmb {I}_{1}= 100\angle-16.26^{\circ} A.

Thus the steady-state expression for i_{1} is

i_{1}=100 \cos \left(400t – 16.26^{\circ}\right) A.

b)\pmb {V}_{1}= 2500\angle 0° – \left(100 \angle -16.26°\right )\left(0.25 + j 2\right)

= 2500 – 80 – j185

= 2420 – j185 = 2427.06 \angle -4.37° V.

Hence

v_{1}= 2427.06 \cos \left(400t – 4.37^{\circ}\right) V.

c) \pmb{I}_{2}= 10\pmb {I}_{1} =1000\angle-16.26^{\circ} A .

Therefore

i_{2} = 1000 \cos \left(400t – 16.26^{\circ}\right) A.

d)\pmb {V}_{2}= 0.1\pmb {V}_{1} = 242.71 \angle -4.37^{\circ} V,

giving

v_{2} = 242.71 \cos \left(400t – 4.37^{\circ}\right) V.

9.46

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