Mesh Analysis KVL: Homework Solutions

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Discussion Overview

The discussion revolves around the application of mesh analysis and Kirchhoff's Voltage Law (KVL) in solving a circuit problem. Participants share their attempts at formulating loop equations, addressing potential drops and rises, and clarifying current directions. The scope includes homework-related problem-solving and technical explanations of circuit analysis.

Discussion Character

  • Homework-related
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant presents their loop equations but expresses uncertainty about the correctness of their answers.
  • Another participant questions the details of the second loop equation, asking for clarification on the components involved and the direction of potential changes.
  • There is a discussion about the current I2 and its relationship to the total current of 7A, with some participants seeking clarification on its definition.
  • Participants discuss the importance of closing the loop in KVL and the implications of the direction of travel around the loop on the signs of potential changes.
  • One participant revises their equations after considering feedback, leading to a new set of calculated currents.
  • There is a question about the arbitrariness of current direction choices, with a consensus that while current directions can be arbitrary, consistency is crucial once chosen.

Areas of Agreement / Disagreement

Participants generally agree on the necessity of closing loops in KVL and the importance of consistent current direction. However, there are multiple viewpoints regarding the specifics of the loop equations and the interpretation of potential changes, indicating that the discussion remains somewhat unresolved.

Contextual Notes

Some participants express confusion regarding the inclusion of certain resistors in their loop equations and the correct accounting of potential changes, suggesting that there may be missing assumptions or unresolved steps in their reasoning.

Who May Find This Useful

Students and individuals studying circuit analysis, particularly those interested in mesh analysis and KVL applications in electrical engineering contexts.

TheRedDevil18
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Homework Statement



KVL.jpg


Homework Equations

The Attempt at a Solution



I'm not getting the correct answers, this is what I tried

Loop 1: 150 - 14*i1 - 6(i1+i2) = 0

Loop 2: -24 + 3*i3 = 0
Therefore i3 = 8A

7A = i2 + i3
Therefore i2 = 7-8 = -1A

Plugging that in equation 1, I get i1 = 7.8A
 
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Your Loop 1 looks good. Can you explain your Loop 2 equation in more detail? What components are in the Loop 2 path, and are you summing potential drops or potential rises?

The arrows on your figure hint that you are traversing the loop counterclockwise, and along with the assumed direction of I3 that you've indicated would make the change in potential across the 3 Ohm resistor positive, which your equation indicates, but it also shows the contribution from the 24 V supply to be negative. So, a contradiction there. There should be at least one more term in the equation, because you've just passed the 3 Ohm resistor and haven't made it back to the bottom of the 24 V supply yet...
 
What is I2 in that diagram? Is it the current in the branch with the current source?
 
milesyoung said:
What is I2 in that diagram? Is it the current in the branch with the current source?

I2 forms part of the 7A current. The 7A splits into I2 and I3, so 7A = I2 + I3
 
gneill said:
Your Loop 1 looks good. Can you explain your Loop 2 equation in more detail? What components are in the Loop 2 path, and are you summing potential drops or potential rises?

The arrows on your figure hint that you are traversing the loop counterclockwise, and along with the assumed direction of I3 that you've indicated would make the change in potential across the 3 Ohm resistor positive, which your equation indicates, but it also shows the contribution from the 24 V supply to be negative. So, a contradiction there. There should be at least one more term in the equation, because you've just passed the 3 Ohm resistor and haven't made it back to the bottom of the 24 V supply yet...

I am summing potential drops across the resistors

I thought the voltage would be negative on the 24V battery because I am moving opposite to the current flow. By one more term, do you mean I should include the 6 ohm resistor in loop 2 ?, or maybe their should be 3 loop equations and I am missing one ?
 
TheRedDevil18 said:
I am summing potential drops across the resistors
But you haven't closed the loop. You have a term for the 24 V supply and another for the 3 Ohm resistor. How do you get back to the 24 V supply?
I thought the voltage would be negative on the 24V battery because I am moving opposite to the current flow. By one more term, do you mean I should include the 6 ohm resistor in loop 2 ?, or maybe their should be 3 loop equations and I am missing one ?
Always count the potential change across a voltage supply in terms of your direction of travel around the loop, not the current direction. Current direction will influence the sign of the potential change across a resistor, but voltage supplies are fixed regardless of the current direction.

You could include the 6 Ohm resistor in the path, or continue on around via the 14 Ohm resistor and 150 V supply. Either is fine, the important thing is you must close a loop for the sum to be zero.
 
gneill said:
But you haven't closed the loop. You have a term for the 24 V supply and another for the 3 Ohm resistor. How do you get back to the 24 V supply?

Always count the potential change across a voltage supply in terms of your direction of travel around the loop, not the current direction. Current direction will influence the sign of the potential change across a resistor, but voltage supplies are fixed regardless of the current direction.

You could include the 6 Ohm resistor in the path, or continue on around via the 14 Ohm resistor and 150 V supply. Either is fine, the important thing is you must close a loop for the sum to be zero.

Ok, thanks. I included the 6 ohm resistor in the path and here are my equations now

Loop 1, same as before
150 - 14*i1 - 6(i1+i2) = 0

Loop 2: 24 + 3*i3 - 6(i1+i2) = 0 (I subbed 7-i2 for i3)

Solving these two equations I get i1 = 7.5 and i2 = 0

Therefore the 150V source = i1 = 7,5A
The 6 ohm resistor = i1+i2 = 7.5A
The 24V source = i3 = 7-i2 = 7A

Yay, got the correct answers, thanks for your help :)

One more question, I sometimes get confused with choosing the current directions and this leads to the incorrect signs. I heard the current directions are arbitrary, is that the case ?
 
TheRedDevil18 said:
One more question, I sometimes get confused with choosing the current directions and this leads to the incorrect signs. I heard the current directions are arbitrary, is that the case ?
Yes, current directions are arbitrary (except for current sources which are defined to have a particular direction). You must, however, be consistent in their use once you've chosen them.
 
gneill said:
Yes, current directions are arbitrary (except for current sources which are defined to have a particular direction). You must, however, be consistent in their use once you've chosen them.

Cool, thanks
 

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