Find current with source transforms

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The discussion revolves around solving a circuit problem involving current and voltage source transformations. The user initially combines various circuit components but makes mistakes in the calculations, particularly when transitioning between Norton and Thevenin equivalents. Key advice emphasizes the importance of adjusting the source values as components are absorbed and ensuring correct impedance calculations. After several iterations and corrections, the user arrives at a final current value of -0.067 - 1.9i A, which is confirmed as accurate by others in the discussion. The thread highlights the significance of meticulous source transformations and impedance calculations in circuit analysis.
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Homework Statement


Mgf1aK7.png


Homework Equations


V=IR

The Attempt at a Solution


First I combined the -j3 capacitor and 4ohm resistor to get:
\frac{32-j48}{25}.
Then I combined that with the j4 ohm inductor to get:
\frac{32+j52}{25}.
Then I combined that with the -j2 ohm capacitor to get:
\frac{104-72j}{36+j2}
My circuit now looks something like:
2B5XjUC.png


I then transform the Current Source into a voltage source:
3<30° -> \frac{3\sqrt{3}}{2} + 1.5i
Z total = \frac{36-28j}{13}
V=I * Z = \frac{84+103\sqrt3}{26} + \frac{54-84sqrt3j}{26}

I now have something like this:
upload_2016-10-12_22-45-51.jpeg

Have I been doing everything right so far? How do I find I?
 
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eehelp150 said:

The Attempt at a Solution


First I combined the -j3 capacitor and 4ohm resistor to get:
\frac{32-j48}{25}.
You might want to check that result.

As you "absorb" components you must modify the source value, too. Effectively you are converting between current and voltage sources as you progress, doing a Norton → Thevenin → Norton shuffle.
 
gneill said:
You might want to check that result.

As you "absorb" components you must modify the source value, too. Effectively you are converting between current and voltage sources as you progress, doing a Norton → Thevenin → Norton shuffle.
What is wrong with the result? Am I not supposed to combine those two parts?
 
eehelp150 said:
What is wrong with the result? Am I not supposed to combine those two parts?
No, combining them is fine. Check your calculated result.
 
eehelp150 said:

The Attempt at a Solution


First I combined the -j3 capacitor and 4ohm resistor to get:
\frac{32-j48}{25}.
Then I combined that with the j4 ohm inductor to get:
\frac{32+j52}{25}.
Then I combined that with the -j2 ohm capacitor to get:
\frac{104-72j}{36+j2}

The two steps in red are where you made your mistake. You must combine the j4 and -j2 in series, and then that equivalent combines in parallel with what you have up to that point.
 
The Electrician said:
The two steps in red are where you made your mistake. You must combine the j4 and -j2 in series, and then that equivalent combines in parallel with what you have up to that point.
upload_2016-10-13_11-54-8.png

this is what my circuit looks like now, with Z3 = (96-72j)/(36+2j)
Everything good?
how do I solve for current I
 
Not good. Your current source has to evolve as you absorb the components. Think of it as taking successive Thevenin or Norton equivalents as you go.

You started by reducing the -j3 capacitor and 4 Ohm resistor to a single impedance, then took it and the current source as a Norton model. All good so far. Then you wanted to absorb the j4 inductor. To do that you have to convert the Norton circuit into its Thevenin equivalent first. So the Norton impedance becomes the series impedance for the Thevenin model and you also have to convert the current source to a Thevenin voltage by multiplying it by that impedance. Then you can include the j4 inductor. The same thing goes for absorbing the -j2 capacitor. You need to convert your new Thevenin model back to a Norton model (source current and parallel impedance). The original current source will be "buried" behind a set of multipliers that it accumulates during the switching back and forth between model types.

Your first change of source goes like this:
upload_2016-10-13_15-37-12.png
 
gneill said:
Not good. Your current source has to evolve as you absorb the components. Think of it as taking successive Thevenin or Norton equivalents as you go.

You started by reducing the -j3 capacitor and 4 Ohm resistor to a single impedance, then took it and the current source as a Norton model. All good so far. Then you wanted to absorb the j4 inductor. To do that you have to convert the Norton circuit into its Thevenin equivalent first. So the Norton impedance becomes the series impedance for the Thevenin model and you also have to convert the current source to a Thevenin voltage by multiplying it by that impedance. Then you can include the j4 inductor. The same thing goes for absorbing the -j2 capacitor. You need to convert your new Thevenin model back to a Norton model (source current and parallel impedance). The original current source will be "buried" behind a set of multipliers that it accumulates during the switching back and forth between model types.

Your first change of source goes like this:
View attachment 107409
upload_2016-10-13_13-11-10.png


I = 4.47515-2.2127j
Z = (4-72j)/(36-48j)

To get the current, can I use a current divider here or do I need another conversion?
I ended up getting
I = 1.32 - 1.44i
 
Last edited:
Practically speaking you can do it either way. If they are expecting you to use source changes though, you might want to follow through to the end.

You should check your results using another method when you're done. Perhaps using Nodal analysis.
 
  • #10
gneill said:
Practically speaking you can do it either way. If they are expecting you to use source changes though, you might want to follow through to the end.

You should check your results using another method when you're done. Perhaps using Nodal analysis.
I ended up getting
1.32 - 1.44i Amps
 
  • #11
eehelp150 said:
I ended up getting
1.32 - 1.44i Amps
Not what I'm seeing. I did the whole series of source changes down to a final Thevenin model in series with the 2 Ohm load, and I checked using nodal analysis to find the voltage at the output node then determined the current through the load from that. The results agreed, and they weren't the same as your result above :frown:
 
  • #12
gneill said:
Not what I'm seeing. I did the whole series of source changes down to a final Thevenin model in series with the 2 Ohm load, and I checked using nodal analysis to find the voltage at the output node then determined the current through the load from that. The results agreed, and they weren't the same as your result above :frown:
My Vth is 3-5.2i
is that off as well?
 
  • #13
gneill said:
Not what I'm seeing. I did the whole series of source changes down to a final Thevenin model in series with the 2 Ohm load, and I checked using nodal analysis to find the voltage at the output node then determined the current through the load from that. The results agreed, and they weren't the same as your result above :frown:
Is it right up to here?
upload_2016-10-13_13-11-10-png.107410.png


I = 4.47515-2.2127j
Z = (4-72j)/(36-48j)
 
  • #14
I don't believe so, no. In that configuration your Z should match my final Thevenin impedance and it doesn't.

Your Z:
upload_2016-10-13_17-47-48.png


Mine:
upload_2016-10-13_17-48-26.png
 
  • #15
gneill said:
I don't believe so, no. In that configuration your Z should match my final Thevenin impedance and it doesn't.

Your Z:
View attachment 107414

Mine:
View attachment 107415
So your Z is 2.769 - 2.154j at the point in my picture?
 
  • #16
eehelp150 said:
So your Z is 2.769 - 2.154j at the point in my picture?

That would be my understanding, yes.

Perhaps we need to go through the transformations one at a time from the beginning?
 
  • #17
gneill said:
That would be my understanding, yes.

Perhaps we need to go through the transformations one at a time from the beginning?
I know where I screwed up.
Final I should be:
-0.067 - 1.9i A
 
  • #18
eehelp150 said:
I know where I screwed up.
Final I should be:
-0.067 - 1.9i A
Yes, that looks good. :approve:
 

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