Mesh Method and Node Method Check

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Discussion Overview

The discussion revolves around solving a circuit problem using both mesh and node voltage methods to determine the power of a dependent source. Participants are exploring the application of these methods, addressing issues related to sign conventions, equations, and the implementation of super mesh and KCL (Kirchhoff's Current Law).

Discussion Character

  • Homework-related
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant presents equations derived from the mesh method, including Vx = 4I_1 and a mesh equation, but expresses uncertainty about the correctness of their sign conventions.
  • Another participant suggests that the equations for the mesh method may contain sign errors and provides corrections, indicating that Vx should be -4I_1.
  • Concerns are raised about how to choose nodes and apply KCL, particularly regarding the middle branch and the correct polarity of devices.
  • Some participants discuss the concept of super mesh and its application to dependent sources, with varying levels of familiarity with the concept.
  • There is a question about the correct approach to label polarities based on loop direction versus device direction.
  • One participant asks if the power of the dependent source can be calculated using P_ds = I^2R, specifying a resistance of 6 ohms.
  • A later reply indicates that the power can be calculated based on the voltage across the dependent source and the current through it.
  • One participant mentions arriving at a current of -1A for the dependent source and questions its validity.

Areas of Agreement / Disagreement

Participants express uncertainty regarding the sign conventions and the application of KCL and mesh methods. There is no clear consensus on the correctness of the initial equations or the approach to the node voltage method, indicating multiple competing views and unresolved issues.

Contextual Notes

Participants highlight potential sign errors in the mesh equations and express confusion about the correct application of conventions in their calculations. The discussion includes various assumptions about the circuit configuration and the methods being used.

IronBrain
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Homework Statement


Given the following circuit using mesh's method to solve for the power of the dependent source.
Using the same circuit and using the node voltage method solve for the power of the dependent source.

Circuit:
5nlpw5.png


Homework Equations


Noting that I have to implement a super mesh for the dependent source to solve the unknown currents. I have arrived to the following equations

Vx = 4I_1

3Vx = I_2 - I_1

The Mesh equation:

-4I_1-12I_2+30-8I_1-20 = 0

Simplifying:

-12I_1-12I_2+10 = 0

The Attempt at a Solution


Solving the simulatenous equations by doing various substitutions of

Vx = 4I_1

3Vx = I_2 - I_1

By solving the mesh equations for I_1 = \frac{10}{12} - I_2

I have arrived at the following solutions

I_1 = \frac{5}{84}

I_2 = \frac{65}{84}

Vx = \frac{5}{21}

3Vx = \frac{5}{7}

Checking by Kirchoff's voltage law to see if all voltages within the outter loop it does equate to 0.

I need a check to see if this is right and I have no idea how to properly implement the node voltage method because the equations do not seem to come out right. I think my trouble is properly putting the correct polarity/sign convention of all devices

Help! Thanks!
 
Last edited:
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Sigh bump...
 
Dammit! I need this checked by tomorrw morning!
 
IronBrain said:
Dammit! I need this checked by tomorrw morning!

Watch the attitude please. The PF is a volunteer help site, so you won't always get help in a timely fashion. The right way to check your problem is for you to do it the two ways the problem asks you -- if the answers are the same, then you probably got it right.

Can you be more specific about what part of the KCL equation writing is bothering you?
 
Well I am not entirely sure if my sign convention for all devices is correct. And which or how many nodes to pick when implementing the node method and what to use when using KCL for node for the middle branch, would I just put the current down that branch as 3Vx, and I just want to see if my first solutions using Mesh is correct
 
IronBrain said:
Well I am not entirely sure if my sign convention for all devices is correct. And which or how many nodes to pick when implementing the node method and what to use when using KCL for node for the middle branch, would I just put the current down that branch as 3Vx, and I just want to see if my first solutions using Mesh is correct

On your KVL work, I'm not sure I understand why you wrote an equation around the whole outside loop, instead of writing the 2 equations for the left and right loops. Also, be sure to label the +/- assumed voltage drop direction on R3, so you can keep it consistent in later equations.

For the KCL, I would put ground at the bottom of R4, and write equations for nodes on each side of the V1 source, and the top node at the top end of the dependent current source.
 
Thanks
Im in my originating equations I believe when doing super mesh you "pretend" as if the current source in a common branch is there hence the equation for my mesh.

Also thanks for the tips on the node method, ill try that out
 
IronBrain said:
Thanks
Im in my originating equations I believe when doing super mesh you "pretend" as if the current source in a common branch is there hence the equation for my mesh.

Also thanks for the tips on the node method, ill try that out

To be honest, I'm not familiar with the super mesh concept. I'd just write the two loop equations for the KVL. But I hardly ever use KVL, so I'm probably not a great help on that. The KCL should be fine, and a good check against your answer for the KVL.
 
Thanks for help, so do I label the polarities of the devices based on the direction of each loop I have chosen or based of the direction of the device?

I believe super mesh is used for a dependent source or any device shared between a common branch of currents.

Also would I put a node on top of V2?
 
  • #10
IronBrain said:
Well I am not entirely sure if my sign convention for all devices is correct. And which or how many nodes to pick when implementing the node method and what to use when using KCL for node for the middle branch, would I just put the current down that branch as 3Vx, and I just want to see if my first solutions using Mesh is correct

You've got a sign error here:

The Mesh equation:

-4I_1-12I_2+30-8I_1-20 = 0

It should be:

-4I_1-12I_2-30-8I_1+20 = 0

And you have a sign error here:

Vx = 4I_1

3Vx = I_2 - I_1

You should have:

Vx = -4I_1

3Vx = I_2 - I_1

Combine them to get:

-12I_1 = I_2 - I_1

Now if you solve your simultaneous equations, you should get:

I1 = 1/12
I2 = -11/12

From which the voltage at the top middle node = 19 volts, assuming the bottom of R4 is the reference, or ground.

For the nodal method, I would move R2 to a position between R1 and the middle node; then the negative terminal of V1 is grounded and the whole thing is easier to conceptualize.
 
Last edited:
  • #11
Thanks!
I always have a problem with getting the right sign convention here, I've been working on this for multiple hours trying to find a comprehendable explainable solution to my mess. Being that the original direction gets confused with the direction I am trying to take. How do you know which convention of the device is correct, I can never seem to get them correct. Also one minor detail left.

To find the power of the dependent source can I simply use the fact that

P_ds = I^2R

Which R is the resistance of 6 ohms
 
  • #12
IronBrain said:
Thanks!
I always have a problem with getting the right sign convention here, I've been working on this for multiple hours trying to find a comprehendable explainable solution to my mess. Being that the original direction gets confused with the direction I am trying to take. How do you know which convention of the device is correct, I can never seem to get them correct. Also one minor detail left.

To find the power of the dependent source can I simply use the fact that

P_ds = I^2R

Which R is the resistance of 6 ohms

You know the current in R4, so you can calculate the voltage across R4. Then the voltage across the dependent source is (19 - voltage across R4). Then the power delivered by the dependent source is (voltage across the source)*(current through the source).
 
  • #13
I got -1A for the current dependent source, does that seem right?
 

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