What is the Methodology for Solving a Complex Circuit with Thevenin Equivalent?

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In summary, the conversation involves a discussion about solving a circuit with a controlled source and finding the Thevenin equivalents. The main focus of the conversation is on finding the open circuit voltage and short circuit current. One approach is to use frequency domain analysis, while another is to use the voltage divider expression. The conversation also touches on the use of impedance to determine the output voltage. The conversation ends with a question about the behavior of a dependent voltage source when one of its ports is shorted to ground.
  • #1
Learnphysics
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Homework Statement


http://imgur.com/izloBbW

http://imgur.com/izloBbW
Essentially I've been attempting to solve the first question.

Homework Equations


I'm mostly concerned on the methodology to solve such a question; So far I've been attempting the following:

As always with these questions I'm seeking the Open circuit voltage, and the short circuit current and saying V/I=Rthevenin.

The trick is in finding Voc, and Isc

For Voc I first found the voltage at the node connected to the positive of the capacitor; this was a long process involving finding the complementary and particular solutions and adding them. I wasn't sure how to solve the constants that arose from this, so I made the assumption that at time = 0, capacitor voltage will be 0. (Note the question doesn't mention initial conditions)

Then I simply multiplied Vc by 3, because Va=vc+(2*Vc),Va=3vc.

To find Isc, I realized that Va =0 volts, and because Va=(vc*3) then Vc=0. (i'm fairly sure I'm far offtrack with this one)

To find the current through the 6ohm resistor we can simply say Vs/6. (with Vs being a sinusoid). subtract from this the current through the capacitor (KCL at a node).. and I assumed that would be ISC.

Where am I wrong, if I was ever on the right track, and what's the preferred method to solve something like this.

Thanks

Homework Statement


Homework Equations


The Attempt at a Solution

 
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  • #2
Learnphysics said:

Homework Statement


http://imgur.com/izloBbW

http://imgur.com/izloBbW
Essentially I've been attempting to solve the first question.

Homework Equations


I'm mostly concerned on the methodology to solve such a question; So far I've been attempting the following:

As always with these questions I'm seeking the Open circuit voltage, and the short circuit current and saying V/I=Rthevenin.

The trick is in finding Voc, and Isc

For Voc I first found the voltage at the node connected to the positive of the capacitor; this was a long process involving finding the complementary and particular solutions and adding them. I wasn't sure how to solve the constants that arose from this, so I made the assumption that at time = 0, capacitor voltage will be 0. (Note the question doesn't mention initial conditions)

Then I simply multiplied Vc by 3, because Va=vc+(2*Vc),Va=3vc.

To find Isc, I realized that Va =0 volts, and because Va=(vc*3) then Vc=0. (i'm fairly sure I'm far offtrack with this one)

To find the current through the 6ohm resistor we can simply say Vs/6. (with Vs being a sinusoid). subtract from this the current through the capacitor (KCL at a node).. and I assumed that would be ISC.

Where am I wrong, if I was ever on the right track, and what's the preferred method to solve something like this.

Thanks

Okay, a bit of a tricky one here. Since you've got the angular frequency of the source you can determine the impedance of the capacitor. No need to go solving differential equations if you're looking for the steady-state conditions. The controlled source, being ideal, isn't going to care about the load it sees, it'll want to faithfully produce twice the voltages it sees at the top of the capacitor. So intuitively it feels like the Thevenin impedance should be zero... something to confirm by analysis.

One approach to finding Thevenin equivalents when you've got controlled sources involved is to place a load resistor RL across the output and solve for an expression for the output voltage. Now, a Thevenin equivalent with a load attached is just a source and potential divider:

attachment.gif


If you can force your expression for the output voltage into the form of the voltage divider expression, then you can pick out the Thevenin voltage and impedance by inspection.

If the Thevenin impedance turns out to be zero then your expression for the output voltage will not contain the variable RL at all, and you'll be left with just a Thevenin voltage :wink:
 

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  • #3
gneill said:
Okay, a bit of a tricky one here. Since you've got the angular frequency of the source you can determine the impedance of the capacitor. No need to go solving differential equations if you're looking for the steady-state conditions. The controlled source, being ideal, isn't going to care about the load it sees, it'll want to faithfully produce twice the voltages it sees at the top of the capacitor. So intuitively it feels like the Thevenin impedance should be zero... something to confirm by analysis.

One approach to finding Thevenin equivalents when you've got controlled sources involved is to place a load resistor RL across the output and solve for an expression for the output voltage. Now, a Thevenin equivalent with a load attached is just a source and potential divider:

attachment.php?attachmentid=64117&stc=1&d=1384952007.gif


If you can force your expression for the output voltage into the form of the voltage divider expression, then you can pick out the Thevenin voltage and impedance by inspection.

If the Thevenin impedance turns out to be zero then your expression for the output voltage will not contain the variable RL at all, and you'll be left with just a Thevenin voltage :wink:

I would solve for the output voltage by frequency domain analysis right?
 
  • #4
Learnphysics said:
I would solve for the output voltage by frequency domain analysis right?

Sure, but the only frequency involved is 5 rad/sec as determined by the argument to the cosine function of the voltage source. In other words, s = ωj, and ω = 5 rad/sec.

This let's you determine the impedance (complex value) of the capacitor. Then proceed as you would for any circuit where you know the impedances.
 
  • #5
I see..Say that I wanted to solve this by finding Voc/Isc.. When I short the two ports. It makes one side of the dependent voltage source = 0 (directly connected to ground)...

So how does that work? If the equation governing the top of the capacitor and the other side of the dependent source is

V2 = 3*V1,
(with V1 being the top of the capacitor, and V2 being port A)

If V2 is 0 (because it's shorted directly to the ground)... what does that make V1? 0 aswell? Or does the dependent circuit take priority, and make port a equal to 2x whatever v1 is despite being connected to ground.
 
  • #6
http://imgur.com/ExHKGB0

Here's my working, where have I gone wrong.

A bit of an explanation of what I've done is basically considering a supernode across the dependent source, and then performing KCL on that node.

Relating V1 and V2, then solving for V1. solving for V2, and declaring V2 and my Voc.

Shorting the ports, calculating Isc (this is the part I'm least sure about). (I've assumed current going through the capacitor in the event of a short circuit across the ports is 0, as both ports of the capacitor are at 0volts.)
Then saying Zth = Voc/Isc
 
  • #7
Learnphysics said:
http://imgur.com/ExHKGB0

Here's my working, where have I gone wrong.
It looks as though you've reached the correct values, if I'm reading your work correctly.

A bit of an explanation of what I've done is basically considering a supernode across the dependent source, and then performing KCL on that node.

Relating V1 and V2, then solving for V1. solving for V2, and declaring V2 and my Voc.

Shorting the ports, calculating Isc (this is the part I'm least sure about). (I've assumed current going through the capacitor in the event of a short circuit across the ports is 0, as both ports of the capacitor are at 0volts.)
Then saying Zth = Voc/Isc

That's the idea. If you write KVL around the second loop (output shorted) you have v1 + 2v1 = 0, which means v1 is zero. In order for v1 to be zero, the mesh current in loop 2 must be equal to the mesh current in loop 1 (that is, i2 = i1, where i1 and i2 are the mesh currents for the two loops).
 
  • #8
It looks to me like the angle of Zth is -15.945°, not -74°.
 
  • #9
The Electrician said:
It looks to me like the angle of Zth is -15.945°, not -74°.

You're right. I missed that in the fine print Good catch.
 
  • #10
The Electrician said:
It looks to me like the angle of Zth is -15.945°, not -74°.

Hmm? Does this mean I've done something wrong with my phase angle on the thevenin resistance?
How are you reaching -15.945?
 
  • #11
Learnphysics said:
Hmm? Does this mean I've done something wrong with my phase angle on the thevenin resistance?
How are you reaching -15.945?

Calculate (1.166666 +.33333 j) in polar coordinates; what angle do you get?
 
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  • #12
The Electrician said:
Calculate (1.166666 +.33333 j) in polar coordinates; what angle do you get?

Oh right,

No idea how I ended up with -74.

Thanks guys, this helped out a lot.
 

Related to What is the Methodology for Solving a Complex Circuit with Thevenin Equivalent?

1. What is a Long Winded Thevenin question?

A Long Winded Thevenin question is a type of problem in electrical engineering that involves finding the Thevenin equivalent circuit for a complex network. It requires a thorough understanding of circuit analysis and can be time-consuming to solve.

2. What is the Thevenin theorem?

The Thevenin theorem states that any linear electrical network with voltage and current sources can be replaced by a single voltage source in series with a single resistor. This simplified circuit is known as the Thevenin equivalent circuit.

3. How do you solve a Long Winded Thevenin question?

To solve a Long Winded Thevenin question, you first need to find the Thevenin resistance by short-circuiting all voltage sources and open-circuiting all current sources in the original circuit. Then, you can use this resistance to find the Thevenin voltage by applying Kirchhoff's voltage law to the original circuit. Finally, the Thevenin equivalent circuit can be drawn using the Thevenin voltage and resistance values.

4. Why is the Thevenin equivalent circuit useful?

The Thevenin equivalent circuit is useful because it simplifies a complex network into a single voltage source and resistor. This makes analysis and calculations much easier and can save time in solving circuit problems. It also allows for the prediction of a network's behavior without having to analyze the entire original circuit.

5. What are some applications of the Thevenin theorem?

The Thevenin theorem is used in many fields, including electrical engineering, electronics, and telecommunications. It is commonly used to analyze and design circuit networks, determine power dissipation, and predict the behavior of circuits under different conditions. It is also an important tool in troubleshooting and repairing faulty circuits.

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