Transformer Exercise (Part 3)

Two transformers are placed in series. The transformers obey the following equations:

E 1 = Z S 1 I 1 + Z M 1 I 2 E 2 = Z M 1 I 1 + Z S 1 I 2 E 3 = Z S 2 I 3 + Z M 2 I 4 E 4 = Z M 2 I 3 + Z S 2 I 4 E_1 = Z_{S1} I_1 + Z_{M1} I_2 \\ E_2 = Z_{M1} I_1 + Z_{S1} I_2 \\ E_3 = Z_{S2} I_3 + Z_{M2} I_4 \\ E_4 = Z_{M2} I_3 + Z_{S2} I_4

In the equations, E 1 E_1 , E 2 E_2 , E 3 E_3 , and E 4 E_4 are the terminal voltages and I 1 I_1 , I 2 I_2 , I 3 I_3 , and I 4 I_4 are the terminal currents (note the polarity conventions in the diagram). Z S 1 Z_{S1} and Z M 1 Z_{M1} are the self and mutual impedances for the first transformer, and Z S 2 Z_{S2} and Z M 2 Z_{M2} are the self and mutual impedances for the second transformer.

An AC voltage source with internal voltage E S 1 E_{S1} and internal impedance Z 1 Z_1 supplies the transformers on one side, and an AC voltage source with internal voltage E S 2 E_{S2} and internal impedance Z 2 Z_2 supplies the transformers on the other side.

A certain amount of active power enters the left terminals of the first transformer. Since the transformers have no resistance, the same amount of active power exits the right terminals of the second transformer.

How much active power is transferred through the transformers?

Details and Assumptions:
1) E S 1 = 10 + j 3 E_{S1} = 10 + j 3
2) E S 2 = 10 + j 0 E_{S2} = 10 + j 0
3) Z 1 = 3 + j 3 Z_1 = 3 + j 3
4) Z 2 = 2 + j 1 Z_2 = 2 + j 1
5) Z S 1 = 0 + j 4 Z_{S1} = 0 + j 4
6) Z M 1 = 0 + j 2 Z_{M1} = 0 + j 2
7) Z S 2 = 0 + j 6 Z_{S2} = 0 + j 6
8) Z M 2 = 0 + j 2 Z_{M2} = 0 + j 2
9) Consider all quantities to be complex numbers. The quantity j j is the imaginary unit
10) This article explains what active power is


The answer is 0.3391.

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2 solutions

Very nice problem.

The basic 8 8 equations are: E 1 = ( 0 + j 4 ) I 1 + ( 0 + j 2 ) I 2 E_{1}=(0+j4)I_{1}+(0+j2)I_{2} E 2 = ( 0 + j 2 ) I 1 + ( 0 + j 4 ) I 2 E_{2}= (0+j2)I_{1}+(0+j4)I_{2} E 3 = ( 0 + j 6 ) I 3 + ( 0 + j 2 ) I 4 E_{3}= (0+j6)I_{3}+(0+j2)I_{4} E 4 = ( 0 + j 2 ) I 3 + ( 0 + j 6 ) I 4 E_{4}=(0+j2)I_{3}+(0+j6)I_{4} E S 1 I 1 Z 1 = E 1 E_{S1}-I_{1}Z_{1}=E_{1} I 2 = I 3 I_{2}=-I_{3} E 2 = E 3 E_{2}=E_{3} E S 2 I 4 Z 2 = E 4 E_{S2}-I_{4}Z_{2}=E_{4}
Solving this 8 simple equations gives I 1 = 5083 5654 j 5795 5654 I_{1}=\frac{5083}{5654}-j\frac{5795}{5654} I 2 = 617 5654 j 33 514 I_{2}=\frac{-617}{5654}-j\frac{33}{514} I 3 = 617 5654 + j 33 514 I_{3}=\frac{617}{5654}+j\frac{33}{514} I 4 = 999 2827 j 3805 2827 I_{4}=\frac{999}{2827}-j\frac{3805}{2827} E 1 = 11953 2827 + j 9549 2827 E_{1}=\frac{11953}{2827}+j\frac{9549}{2827} E 2 = 6521 2827 + j 3849 2827 E_{2}=\frac{6521}{2827}+j\frac{3849}{2827} E 3 = 6521 2827 + j 3849 2827 E_{3}=\frac{6521}{2827}+j\frac{3849}{2827} E 4 = 22467 2827 + j 601 257 E_{4}=\frac{22467}{2827}+j\frac{601}{257}
Now the read the 7 t h 7^{th} and 8 t h 8^{th} line of the problem carefully.
To calculate active power , we only calculate the real part of P a c t i v e = E 1 I 1 ˉ P_{active}=E_{1}\bar{I_{1}}
Where the bar line over the I 1 ˉ \bar{I_{1}} tells the complex conjugate of I 1 I_{1}
Suppose we take take a complex number N = x + j y N=x+jy
Then it's complex conjugate is N ˉ = x j y \bar{N}=x-jy
Now come to the problem P a c t i v e = ( 11953 2827 + j 9549 2827 ) ( 5083 5654 + j 5795 5654 ) P_{active}=(\frac{11953}{2827}+j\frac{9549}{2827})(\frac{5083}{5654}+j\frac{5795}{5654}) P a c t i v e 0.3391324 + j 7.3702608 P_{active} \approx 0.3391324+j7.3702608
Our job is to take real part only P a c t i v e 0.3391324 \Large \boxed{\textcolor{#3D99F6}{P_{active} \approx 0.3391324}}


@Steven Chase Sir thanks for posting, I have learned something new :)

Karan Chatrath
Jul 12, 2020

Great problem as always. Thanks for posting. The circuit equations as per Kirchoff's voltage law are:

E S 1 + I 1 Z 1 + E 1 = 0 -E_{S1} + I_1Z_1 + E_1 = 0 E 2 + E 3 = 0 -E_2 + E_3 = 0 E 4 I 4 Z 2 + E S 2 = 0 -E_4 -I_4Z_2 + E_{S2}=0

According to Kirchoff's current law for the second loop:

I 2 + I 3 = 0 I_2 + I_3 = 0

Rearranging these four equations in a matrix form:

[ Z 1 + Z S 1 Z M 1 0 0 Z M 1 Z S 1 Z S 2 Z M 2 0 0 Z M 2 Z S 2 + Z 2 0 1 1 0 ] [ I 1 I 2 I 3 I 4 ] = [ E S 1 0 E S 2 0 ] \left[\begin{matrix}Z_1+Z_{S1}&Z_{M1}&0&0\\-Z_{M1}&-Z_{S1}&Z_{S2}&Z_{M2}\\0&0&Z_{M2}&Z_{S2}+Z_2\\0&1&1&0\end{matrix}\right]\left[\begin{matrix}I_1\\I_2\\I_3\\I_4\end{matrix}\right] = \left[\begin{matrix}E_{S1}\\0\\E_{S2}\\0\end{matrix}\right] [ I 1 I 2 I 3 I 4 ] = [ Z 1 + Z S 1 Z M 1 0 0 Z M 1 Z S 1 Z S 2 Z M 2 0 0 Z M 2 Z S 2 + Z 2 0 1 1 0 ] 1 [ E S 1 0 E S 2 0 ] \implies \left[\begin{matrix}I_1\\I_2\\I_3\\I_4\end{matrix}\right] = \left[\begin{matrix}Z_1+Z_{S1}&Z_{M1}&0&0\\-Z_{M1}&-Z_{S1}&Z_{S2}&Z_{M2}\\0&0&Z_{M2}&Z_{S2}+Z_2\\0&1&1&0\end{matrix}\right]^{-1}\left[\begin{matrix}E_{S1}\\0\\E_{S2}\\0\end{matrix}\right]

The active power is the real part of the product of the current through the terminal and the terminal voltage:

P a = r e a l ( E 1 I 1 ) P_{a} = \mathrm{real}\left(E_1I_1^*\right)

Here, I 1 I_1^* is the complex conjugate of current. The required answer evaluates to: P a 0.3391 \boxed{P_a \approx 0.3391}

Thanks for the solution. Did you check the other side too?

Steven Chase - 11 months ago

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Yes, that is how I confirmed that my answer is correct. I was initially computing the power without taking complex conjugates. This check was a helpful hint in the problem statement.

Karan Chatrath - 11 months ago

The absolute value of the real parts of the power at each end are equal.

Karan Chatrath - 11 months ago

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@Karan Chatrath Sir I have also uploaded my solution .
And I am waiting for your RLC problem in which I will post solution through Laplace
Thanks in advance.

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@A Former Brilliant Member It is up now

Karan Chatrath - 11 months ago

@Steven Chase You have added Note, especially to clear my doubt. Smart

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Yes, it's a one-dimensional problem, and it starts at y = 0 y = 0

Steven Chase - 11 months ago

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