An AC voltage source has internal voltage V S and internal impedance Z S . A load impedance Z L is connected across the source terminals. Z L has the following form:
Z L = 5 e j θ − π / 2 ≤ θ ≤ π / 2
The active power (in watts) dissipated by the load at a particular angle θ is P L ( θ ) . Determine the following integral:
∫ − π / 2 π / 2 P L ( θ ) d θ
Bonus: Make a plot of P L vs. θ . Which θ value yields maximum P L , and what is notable about it?
Details and Assumptions:
1)
V
S
=
1
0
+
j
0
2)
Z
S
=
1
+
j
2
3)
j
=
−
1
4)
Source voltage is given in RMS (root mean square value)
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Solution edited slightly.
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I just read your comment to my solution to your previous problem. Now it makes sense. Thanks!
That optimal angle corresponds to Z L = 1 − j 2 , which is the complex conjugate of the source impedance.
I am attempting your latest problem and I have wound up with a rather expensive optimization problem in 5 variables (the three real parts of impedances and the two imaginary parts). To solve this problem, I could honestly use a hint as to how to approach this in a time efficient manner.
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Indeed, this one can be as hard as you want. The easy way is:
1) Calculate the currents from the reference case
2) Sweep the real part of ZA from zero to some upper bound (determined by RB and RC not allowed to be negative)
3) For each RA, take a voltage drop using the known current to calculate VN
4) Knowing VN and the required currents for IB and IC, calculate the impedances for ZB and ZC
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Your suggestion is a really neat method. Unfortunately, I got the wrong answer. Could you give feedback? Hoping that my code is readable.
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@Karan Chatrath – Do your currents add to zero in the base case?
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@Steven Chase – Yes, they do add to zero
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@Karan Chatrath – Here are mine:
(76.6144161503+6.9101055907j)
(-45.2927204974-17.1998571452j)
(-31.3216956529+10.2897515545j)
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@Steven Chase – I obtain the same.
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@Karan Chatrath – Strange. I don't see any real difference. I have attached my code:
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@Karan Chatrath – Do you need to say Vmin = abs(VN)?
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@Steven Chase – Nice catch. I just reran the code and I get the answer you obtained. Thank you for the feedback. Bummer that I could not get this one right. It was fun
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@Karan Chatrath – I would delete and repost, but somebody has already solved
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@Steven Chase – Oh it is okay. I would not expect you to repost anyway. I got it wrong fair and square. Plus I see this as a lesson in presence of mind. This tiny mistake was not easy to spot for me.
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@Karan Chatrath – Alright, glad you enjoyed it despite the unfortunate luck
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Solution outline only provided.
I = Z S + Z L V S ⟹ P L = r e a l ( I Z L I ∗ )
Plugging in the expressions and given values gives the required function P L ( θ ) . Here, the angle is deliberately plotted in degrees. From this point, it is easy to numerically compute the required integral (it can probably be done analytically too, but I did not compute the exact integrand to be sure) . The required answer is: ∫ − π / 2 π / 2 P L ( θ ) d θ ≈ 4 4 . 4 4
The value of θ for which P L ( θ ) is maximum is − 6 3 . 4 3 2 ∘ . This happens to be the negative of the phase of the complex number Z S .