Power Transfer Over Cable

An AC voltage source feeds a load resistor through a cable as shown. The cable is modeled as a pi circuit consisting of a series resistive/inductive segment, with two shunt capacitances.

If the load resistor R L R_L consumes 40 40 watts of active power, what is the RMS magnitude of the source voltage?

Bonus: What would the answer be if the voltage source was connected directly across the load resistor without the cable in between? Here is a supplementary article on the Ferranti Effect

Details and Assumptions:
1) R L = 360 Ω R_L = 360 \,\, \Omega
2) Z = 8 + j 40 Ω Z = 8 + j 40 \,\, \Omega
3) Z C = 0 j 400 Ω Z_C = 0 - j 400 \,\, \Omega


The answer is 111.78.

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2 solutions

Steven Chase
Mar 11, 2021

My approach was similar to that of @Karan Chatrath , in that I swept V S V_S and calculated the load power each time. I solved the following node equation for the load resistor voltage V L V_L (sum of currents out of the node is zero).

V L V S Z + V L Z C + V L R L = 0 \frac{V_L - V_S}{Z} + \frac{V_L}{Z_C} + \frac{V_L}{R_L} = 0

Then the load power is:

P L = V L 2 R L P_L = \frac{|V_L|^2}{R_L}

Cables or transmission lines with significant parasitic capacitance can see the voltage rise from the sending end toward the load. This is because a capacitive current is drawn through an inductive series impedance. In order to dissipate 40 40 watts, the resistor needs 120 120 volts across it. And because of this voltage rise (the Ferranti Effect), we only have to apply 111.78 111.78 volts at the sending end in order for the load resistor to get 120 120 volts.

@Steven Chase Upvoted.
Here is a question for you.

Please provide me the solution and answer of this question 1.(both part (a) and (b)).
Whenever you will be free.
The question contains total 6 marks.
Let's see how much you score :)

Talulah Riley - 3 months ago

One thing forgot to say , please solve analytically.

Talulah Riley - 3 months ago
Karan Chatrath
Mar 11, 2021

Currents are indicated in the diagram. Using Kichhoff's current and voltage laws yields the following equations in a matrix form:

[ 1 1 0 1 0 0 0 1 1 1 0 Z C 0 0 0 0 Z C Z C Z 0 0 0 Z C 0 R L ] [ I I C 1 I C 2 I Z I L ] = [ 0 0 V S 0 0 ] \left[\begin{matrix} 1 & -1 & 0 & -1 & 0\\0 & 0 & -1 & 1 & -1\\0 & Z_C & 0&0&0\\0& -Z_C& Z_C&Z&0\\0&0&Z_C&0&-R_L \end{matrix} \right] \left[\begin{matrix} I\\I_{C1}\\I_{C2}\\I_Z\\I_L \end{matrix} \right] = \left[\begin{matrix} 0\\0\\V_S\\0\\0 \end{matrix} \right]

A I = b \implies AI = b I L = [ 0 0 0 0 1 ] A 1 b \implies I_L = \left[\begin{matrix} 0&0&0&0&1 \end{matrix} \right]A^{-1} b

P A = r e a l ( I L R L I L ) \implies P_A = \mathrm{real} \left(I_LR_L I_L^{*}\right)

To solve for V S V_S I used brute force. I simply swept through different values of V S V_S until I found the solution to some numerical tolerance.

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clear all
clc

% GIven parameters:
RL       = 360;
Z        = 8 + j*40;
ZC       = -j*400;

% A matrix as shown in the solution description:
A        = [1 -1 0 -1 0;0 0 -1 1 -1;0 ZC 0 0 0;0 -ZC ZC Z 0;0 0 ZC 0 -RL];

% Varying VS in small increments:
for VS  = 0:0.0001:120

% b vector as shown in the solution description:
b        = [0;0;VS;0;0];

% Computation of load current:
IL       = [0 0 0 0 1]*inv(A)*b;

% Active power consumed by load:
PA       = real(IL*RL*conj(IL));

% Checking if active power is close to 40 W to some tolerance:
if abs(PA - 40) <= 1e-4
  ANSWER    =  VS;
end


end

% ANSWER = 111.78

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