Solving KVL: Voltage Across All Elements

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Discussion Overview

The discussion revolves around solving for the voltage across all elements in a circuit using Kirchhoff's Voltage Law (KVL) and node-voltage methods. Participants explore various approaches to analyze the circuit, including the identification of essential nodes and the application of KCL (Kirchhoff's Current Law).

Discussion Character

  • Homework-related
  • Mathematical reasoning
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants express uncertainty about which nodes to use for KVL analysis and whether to combine resistors into essential nodes.
  • There are suggestions to sketch closed loops for KVL and write equations based on those loops.
  • One participant mentions the necessity of using supernodes when applying KCL at certain nodes.
  • Confusion arises regarding the treatment of voltage sources at nodes, with questions about the need for multiple supernodes.
  • Participants share their node equations and calculated voltages, with some expressing a desire to verify their answers independently.
  • Discussions include the calculation of currents in the circuit and the verification of power delivered versus power absorbed.
  • Some participants point out potential errors in equations and suggest corrections, particularly regarding the polarity of voltage sources.
  • There is mention of circuit symmetry and its implications for current directions and values.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the best approach to take for the analysis, as there are multiple competing views on the use of KVL, KCL, and the identification of nodes and supernodes. The discussion remains unresolved with varying interpretations and methods proposed.

Contextual Notes

Some participants note the importance of checking the consistency of equations and the implications of circuit symmetry, but there are unresolved mathematical steps and assumptions regarding the node equations and current calculations.

Who May Find This Useful

This discussion may be useful for students and practitioners working on circuit analysis, particularly those interested in applying KVL and KCL methods in their problem-solving approaches.

orangeincup
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Homework Statement


Determine the voltage across all elements

Homework Equations


i=v/r
v1+v2+v3+..=0

The Attempt at a Solution


I'm not sure which of the nodes I should use to take my KVL from. The a and b are labeled, but should I combine the set of 2-6-6 resistors and label that as an essential node? Should I have four essential nodes?
 

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orangeincup said:
I'm not sure which of the nodes I should use to take my KVL from.
You can use KVL ( loops ) or KCL ( nodes ).

So if you use KVL, you must sketch three closed loops ( with a positive direction ), like the two loops, S1 and S2 here:

KCL-and-KVL-example.png

Kirchhoff says that the sum of voltage changes along a closed loop = 0

So as for S1, you could write:

ε1 - S1*R1 - S1*R2 + S2*R2 = 0

Write another equation as for S2.

Having solved the equations, you find: i2 = S1 - S2 , and so on.
 
Last edited:
orangeincup said:

Homework Statement


Determine the voltage across all elements

Homework Equations


i=v/r
v1+v2+v3+..=0

The Attempt at a Solution


I'm not sure which of the nodes I should use to take my KVL from. The a and b are labeled, but should I combine the set of 2-6-6 resistors and label that as an essential node? Should I have four essential nodes?
There are olny unknown three nodes (four if you include ground). at two of the nodes you'll need to do a supernode if you use KCLs

Also you say you need to do node analysis. If that's the case follow Hesche's advice. If you need to do NODAL ANALYSIS as your method, then use KCLs.
 
It says I must use the node-voltage method. I'm confused what to do when there's a voltage source already at the node. Am I suppose to take 3 different super nodes?
 
orangeincup said:
It says I must use the node-voltage method. I'm confused what to do when there's a voltage source already at the node. Am I suppose to take 3 different super nodes?
I don't see any supernode situations here. Just three essential nodes:
Fig2.gif

The ground (reference) node was already provided.

You should be able to write node equations for the three nodes.
 
Okay, I made two formulas with node 1) and node 2)

Node 1)
(v1-12)/2 + (v1-v3)/6 + (v1-v2)/2

Node 2) (v2-v1)/2 + (v2-v3)/6 + (v2-12)/2

Node 3) seems to be (v3-v1)/6+12/6+(v3-v2)/6

Solving...
v1=10
v2=10
v3=4

I set v1 as node 1, v2 as node 2, and v3 as node 3.

Is there a way I can verify my answer by myself?
 
orangeincup said:
Okay, I made two formulas with node 1) and node 2)

Node 1)
(v1-12)/2 + (v1-v3)/6 + (v1-v2)/2

Node 2) (v2-v1)/2 + (v2-v3)/6 + (v2-12)/2

Node 3) seems to be (v3-v1)/6+12/6+(v3-v2)/6
Check that middle term. It should involve v3.
Is there a way I can verify my answer by myself?
Usually one would insert the values and confirm consistency, say by verifying that KCL is satisfied at each node using the voltages solved for, or, using another method entirely to see if you get the same results (mesh analysis perhaps).
 
I'm trying to solve for all the currents in the ciruit and prove power delivered=power absorbed

(v1-12)/2 =-1 a
(v1-v3)/6 =1 a
(v1-v2)/2 = 0 a(?)

(v2-v1)/2 =0 a
(v2-v3)/6=1 a
(v2-12)/2= -1 a

(v3-v1)/6=-1 a
12/6=2 a
(v3-v2)/6=-1 a

I have two values of zero for the resistor between v1 and v2.

power delivered = 12*1a + 12*1a + 12*2a = 48 W
power absorbed = 1^2*2ohm + 1a^2*6ohm + 1^2a*6ohm + 2a^2*6ohm+1^2*2ohm +2a^2*2ohm = 48 W

I reuploaded the picture with all the values labeled , does this look correct?
 

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Zero volts and zero current for the resistor between nodes 1 and 2 is to be expected by the symmetry of the circuit. Symmetry should also tell you something about the directions of certain current pairs.

You still haven't fixed that middle term in the node 3 equation. Fix it and re-solve.
 
  • #10
(v1-12)/2 + (v1-v3)/6 + (v1-v2)/2
(v2-v1)/2 + (v2-v3)/6 + (v2-12)/2
(v3-v1)/6+(v3-12)/6+(v3-v2)/6

Solving...
v1=v2=v3=12VI also tried solving another way,

(v1-12)/2 + (v1-v3)/6 + (v1-v2)/2
(v2-v1)/2 + (v2-v3)/6 + (v2-12)/2
(v3-v1)/6+(v3+12)/6+(v3-v2)/6v1=48/5, v2=48/5, v3=12/5

I think I did something wrong, I'm suppose to be calculating the current for the entire circuit so I can solve for power absorbed=power deliveredpower delivered = 12*1a + 12*1a + 12*1a = 36 W
power absorbed = ? I'm not sure how to get the currents/voltages for the individual pieces. According to my equations most of them will be zero now, since they are all 12-12.
 
  • #11
orangeincup said:
(v1-12)/2 + (v1-v3)/6 + (v1-v2)/2
(v2-v1)/2 + (v2-v3)/6 + (v2-12)/2
(v3-v1)/6+(v3-12)/6+(v3-v2)/6

Solving...
v1=v2=v3=12V
The (v3-12)/6 term is not correct; be careful with the polarity of the source in that leg! It's not the same as that of the other voltage sources. (I see that you've fixed that in your next attempt below)
I also tried solving another way,

(v1-12)/2 + (v1-v3)/6 + (v1-v2)/2
(v2-v1)/2 + (v2-v3)/6 + (v2-12)/2
(v3-v1)/6+(v3+12)/6+(v3-v2)/6v1=48/5, v2=48/5, v3=12/5
Those values look good :smile:
I think I did something wrong, I'm suppose to be calculating the current for the entire circuit so I can solve for power absorbed=power deliveredpower delivered = 12*1a + 12*1a + 12*1a = 36 W
power absorbed = ? I'm not sure how to get the currents/voltages for the individual pieces. According to my equations most of them will be zero now, since they are all 12-12.
The individual terms in your node equations represent the currents in the branches that they were written for. So you can plug in your v1, v2, v3 values to those terms and pull out the individual branch currents. Use those currents to calculate the powers produced or consumed by each of the components.
 
  • #12
Have you considered simplifying the circuit using symmetry? Sorry if this has already been discussed. The internet connection from this hospital bed isn't great so I type in haste.
 

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