High voltage transmission line with ABCD complex equations

AI Thread Summary
The discussion focuses on solving a homework problem involving a high-voltage transmission line using ABCD parameters. Participants are calculating sending-end voltage (V_S) and current (I_S) based on an open-circuit received voltage of 88.9 kV, with initial calculations yielding V_S as 77325+j3149 kV and I_S as j119.9 A. There is confusion regarding the application of frequency and line length in calculating the primary line coefficients R, L, G, and C, with suggestions to use complex impedance and power equations. Participants explore the relationship between the ABCD parameters and T-circuit elements, attempting to derive values for the transmission line components. The conversation highlights the complexities of transmission line modeling and the need for precise calculations to ensure accurate results.
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Homework Statement



Figure shows a 50 Hz, high-voltage, transmission line. The relationships between the sending and receiving end voltages and currents are given by the complex ABCD equations:

V_S = V_R (A_1+jA_2)+I_R (B_1+jB_2)

I_S = V_R(C_1+jC_2)+I_R(D_1+jD_2)

where 'S' stands for sending-end and 'R' stands for receiving-end

(a) Given the parameter values in TABLE C and an open-circuit received voltage measured as 88.9 kV, calculate the values of V_S and I_S and hence the power P_{SO} absorbed from the supply by the transmission line on open circuit.

(b) If the line is modeled by the T-circuit of FIGURE 3(b), see if you can estimate the primary line coefficients R, L, G and C. The line is 50 km long.

Homework Equations



<br /> \begin{bmatrix}<br /> V_S\\<br /> I_S<br /> \end{bmatrix}<br /> =<br /> \begin{bmatrix}<br /> A_1+jA_2 &amp; B_1+jB_2\\<br /> C_1+jC_2 &amp; D_1+jD_2<br /> \end{bmatrix}<br /> \begin{bmatrix}<br /> V_R\\<br /> I_R<br /> \end{bmatrix}<br />

The Attempt at a Solution



What I'm thinking is I_R=0 as this is an open-circuit and given V_R; V_S and I_S can be calculated.
Now,
V_S=77325+j3149 KV
I_S=j119.9 A
But I don't think that is correct because V_S should not be lower than V_R, also 50Hz frequency is given for a reason, I'm sure it has to be used somewhere.

And as for question (b) I have only got ideas. I can find coefficient of propagation γ and Z_o from R,L,G,C but I don't know how to produce them vice versa (from ABCD), I don't see where I could go from there either.

Or another idea:
\frac{V_R}{V_S}=e^{-αl}
where
α=\sqrt{RG}

Any comments are appreciated.
 

Attachments

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I wouldn't worry about Vr > Vs.

How much current is flowing through the resistor and inductor on the right leg of the circuit?
Do the values of those two components matter?
What is the voltage at the top center node of the circuit?

You can compute the total loss of power through the other two resistors. They're the only components that will generate real heat.
 
A transmission line is usually modeled in my learning material by the figure shown in attachment, I reckon this should be the case in this exercise.

Right, the current in the right leg is zero which means that resistor and inductor are out of consideration, hence, the voltage in the top centre node is V_R.

Now, P = Re[VI^*] = 377565.1 W
Is that correct so far?

R can be calculated via P = \frac{V_S^2}{R}

Where do frequency and line length come in?
 

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bizuputyi said:
Right, the current in the right leg is zero which means that resistor and inductor are out of consideration, hence, the voltage in the top centre node is V_R.
Yes, it is!
bizuputyi said:
Now, P = Re[VI^*] = 377565.1 W
Is that correct so far?
My skills at this are seldom practiced. It looks good to me.
bizuputyi said:
R can be calculated via P = \frac{V_S^2}{R}You've got two resistors to deal with. The one on the base leg will dissipate \frac{(88.9KV)^2}{Rb}. But I think I misled you. That total power value doesn't seem to be useful intermediate value.
I do notice that the current at the center node is Is, so you have Vc=(88.9+0j)KV and Ic=(0+119.9j)A. I'm guessing that, along with the 50Hz, that's enough information to solve for the capacitor and resistor values in the stem of the "T".
Then that same sort of logic should be able to solve for the inductor and resistor on the left side.
bizuputyi said:
Where do frequency and line length come in?
The frequency is needed in the computation of the inductor and capacitor values.
Line length doesn't seem to be part of the problem - although once you've computed all of the parameters to your "T", there may be some engineering method for estimating line length.
 
I've been googling and figured that this is Ferranti effect:

http://en.wikipedia.org/wiki/Ferranti_effect
http://www.electrical4u.com/ferranti-effect-in-power-system/

If the impedance in the stem is \frac{V_R}{I_S} I get j741.45Ω, from which

X_c=\frac{1}{\omega lC} (where l is length in metres)

C=85.86pF that is far too low for such a long line.
Without putting 'length in metres' in that equations capacitance is 4.29\muF.

Resistance can be neglected, so can conductance, from that source.

I don't feel I'm on the right track. I've got the voltages and currents all right I think but I'm lost from there.
 
I've got new ideas, see the pictures attached. The T-circuit can be modeled by ZYZ circuit shown in figure.

We know ABCD, frequency and length of line, the question is how to find R,L,G,C.

I'm so close, just need the last nudge.
 

Attachments

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This may be the blind leading the blind, but this is what I did for the base leg:

The voltage over the base leg is 88900V and the current is 119.9jA. so I calculated the resistance:
R = 88900V/119.9jA = -741.5jOhms.

I went to this site:
http://chemandy.com/calculators/ac-networks/capacitor-and-resistor-in-parallel-calculator.htm
and entered 0.05KHz, 4.293uF, and 99,999,999MOhms, to get -741.5jOhms.

So, I conclude (with less than full confidence) that the resistor in the base leg is open (infinite resistance) and the capacitor is 4.293uF.

The voltage across the left arm is (77325+3149j)V-88900V and the current is 119.9jA.
R = (-11575+3149j)V/119.9jA = (26.26 + 96.54j)Ohms.

I went to this site:
http://chemandy.com/calculators/ac-networks/inductor-and-resistor-in-series-calculator.htm
and entered 0.05KHz, 307.3mH, and 26.26Ohms, to get (26.26+96.54j)Ohms.

So I concluded that the left arm inductor is 307.3mH and the resistor is 26.26ohm. Since this is suppose to be a symmetric T circuit, I would use those same values for the right arm.

Do my numbers work better for you?

--- edit
I just noticed your last post. I hope we don't have to go in that direction.
Also, if you need a complex calculator, there is one here:
http://www.mathsisfun.com/numbers/complex-number-calculator.html
 
Last edited:
Yes, that's great, thank you. Let's go down the other line I just figured and see if the values match. I think I'll need 4 equations with 4 unknowns. I need some time to figure them out.
 
I think I've got it. Referring to my latest attachments the left or right series element Z = \frac{A-1}{C}, shunt element Y = \frac{1}{C}
Real part of Z = R/2, imaginary part of Z = L/2, divide by ω for L value.
1/C=jωCs (shunt capacitor)
Divide all values by line length.
 
  • #10
I get the same L and R values as you did. Thank you very much indeed!
 
  • #11
Very good. Does that give you an estimate of the line length?
 
  • #12
Line length is given in the exercise.
 
  • #13
Why does Z=A-1/C and Y=1/C. How are these left/right and shunt elements obtained?
 
  • #14
Hi Guys,

I am struggling with this question as well. Could you explain, how we get from this ABCD matrix formed from a T - network to the Z=A-1/C and Y=1/C ??
How the above equations are obtained?
line-jpg.71986.jpg


Please help
 

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