How can I solve a multiloop circuit using Kirchhoff's laws?

In summary: I(1) = .848A, I(2) = 2.14A, I(3) = .171A, I(4) = .21A, I(5) = .848A, I(6) = .0214AIn summary, the conversation discusses different methods for solving multiloop problems, including using nodes and loops and using Kirchhoff's current rule. The conversation also addresses labeling and simplifying the circuit, as well as potential approaches for solving systems of equations. The final solution for the current in each loop is I(1) = .848A, I(2) = 2.14A, I(3) = .171A, I(
  • #1
gills
116
0

Homework Statement


YF-26-61.jpg


What is the current in I(1), I(2), and I(3)?

Homework Equations



At nodes [tex]\sum[/tex]I = 0

Loops [tex]\sum[/tex]V = 0

The Attempt at a Solution



Ok, I'm definitely new to this multiloop stuff so I'm not quite sure what the best way to work these problems is.

Here's what i have for nodes:

I(4) + I(6) - I(5) = 0
I(2) - I(4) - I(3) = 0
I(1) + I(3) - I(6) = 0and loops:

12 - I(4)5 + I(6)8 - 9 + I(1)1 - I(2)1 = 0
12 - I(3)10 - 9 + I(1)1 - I(2)1 = 0
9 - I(6)8 - I(1) = 0
12 - I(4)5 - I(2)1 = 0Any help on the best and easiest way to work these would be great. Thanks
 
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  • #2
Are there labels missing on the diagram. I(4), I(5), I(6)
 
  • #3
montoyas7940 said:
Are there labels missing on the diagram. I(4), I(5), I(6)

they aren't on the diagram. I just ended up putting them in myself because it seems like i would need them. However, i probably overcomplicated it as i always tend to do. Do i even need an I(4), I(5), and I(6)?
 
  • #4
IMO the most efficient way to solve these is the following method.

1. replace series and parallel resistances (doesn't work in this one)

2. give an arbitrary point a potential of 0. I'd take the node in the middle here between
the four resistances. If you need an equivalent resistance, call the 2 connections to the circuit 0 and V.

3. guess the potential at all points where more than 2 wires meet and call them V_1, V_2 etc. There are two such points here

4. use ohms law to work out all currents as a function of these potentials.

5. Use kirchhof's current rule in each of the points from step 3. This will give you as
many equations as unknowns.

6. Now that you found the potentials, compute the currents you need.

The loop rule is completely redundant here.
 
  • #5
Though kamerling gives an excellent approach, there's nothing wrong with your original method using nodes and loops. For this problem I would use three independent loop equations (because I see three loops) and two node equations.

Since your I(5) just runs through a piece of bare wire, I would not have defined it. (You can always shrink a bare wire down to a point.) Thus I would only have 5 currents and thus only need 5 equations.
gills said:
Here's what i have for nodes:

I(4) + I(6) - I(5) = 0
I(2) - I(4) - I(3) = 0
I(1) + I(3) - I(6) = 0
I would just drop your first equation. (Forget I(5).)

and loops:

12 - I(4)5 + I(6)8 - 9 + I(1)1 - I(2)1 = 0
12 - I(3)10 - 9 + I(1)1 - I(2)1 = 0
9 - I(6)8 - I(1) = 0
12 - I(4)5 - I(2)1 = 0
You really only have three independent loops. Your first equation is just the sum of the last two (or it should be--you have some errors).

So I would drop your first equation. The last two need to be corrected: You have the sign in front of the I(1) and I(2) terms wrong.

Once you have your corrected 5 equations, it's just a matter of turning the crank. 5 equations and 5 unknowns. Start by eliminating one variable--I(4) say--in all your equations. Then eliminate another--I(6) say. And so on until you've solved for one of the currents. Then go back and find the others.
 
  • #6
Doc Al said:
Though kamerling gives an excellent approach, there's nothing wrong with your original method using nodes and loops. For this problem I would use three independent loop equations (because I see three loops) and two node equations.

Since your I(5) just runs through a piece of bare wire, I would not have defined it. (You can always shrink a bare wire down to a point.) Thus I would only have 5 currents and thus only need 5 equations.

I would just drop your first equation. (Forget I(5).)


You really only have three independent loops. Your first equation is just the sum of the last two (or it should be--you have some errors).

So I would drop your first equation. The last two need to be corrected: You have the sign in front of the I(1) and I(2) terms wrong.

Once you have your corrected 5 equations, it's just a matter of turning the crank. 5 equations and 5 unknowns. Start by eliminating one variable--I(4) say--in all your equations. Then eliminate another--I(6) say. And so on until you've solved for one of the currents. Then go back and find the others.


Ok, I've rewritten my equations and my diagram because I've made the wire in between a node where there's no component like you said.

nodes:
I(2) - I(3) - I(5) = 0
I(1) + I(3) - I(4) = 0

loops:
12 - 5I(5) - I(2) = 0
9 - 8I(4) - I(1) = 0
12 - 10I(3) - 9 + I(1) - I(2) = 0

5 eq, 5 unknowns. Unfortunately (and fortunately ;)) I've plugged these into MATlab to check and see if it would be right and it was:

I(1) = 0.848
I(2) = 2.14
I(3) = 0.171

However, i need to try and solve these on my own. What is usually the most effective way for systems of equations, substitution or elimination? Just such a tedious task...

Thanks Doc and everyone else
 
  • #7
While I'm sure there are clever ways of solving systems of equations (using matrix methods or whatever), I suggest using the simple method of Gaussian elimination. Just systematically eliminate the variables until you have one left. Keep all your intermediate equations, since once you get one value you'll be able to quickly get the others just by plugging in.

Tedius? You bet! Get busy. :smile:
 
  • #8
Doc Al said:
While I'm sure there are clever ways of solving systems of equations (using matrix methods or whatever), I suggest using the simple method of Gaussian elimination. Just systematically eliminate the variables until you have one left. Keep all your intermediate equations, since once you get one value you'll be able to quickly get the others just by plugging in.

Tedius? You bet! Get busy. :smile:

thanks Doc. Tedious indeed, but i got it.
 

1. What is a multiloop circuit and how does it differ from a single loop circuit?

A multiloop circuit is a type of electrical circuit that contains more than one closed loop. This means that the electrical current has multiple paths to flow through. In contrast, a single loop circuit only has one closed loop for the current to flow through.

2. What is Kirchhoff's voltage law and how is it applied in a multiloop circuit?

Kirchhoff's voltage law states that the sum of all voltage drops around a closed loop in a circuit must equal the sum of all voltage rises. In a multiloop circuit, this law is applied by considering the voltage drops and rises in each individual loop and ensuring that they add up to zero for the overall circuit.

3. How do you calculate the total resistance in a multiloop circuit?

The total resistance in a multiloop circuit can be calculated by using Kirchhoff's laws and Ohm's law. First, use Kirchhoff's voltage law to determine the voltage drops and rises in each loop. Then, use Ohm's law (V=IR) to calculate the current in each loop. Finally, use the formula R=V/I to calculate the total resistance by taking the total voltage and dividing it by the total current.

4. Can Kirchhoff's laws be applied to both DC and AC circuits?

Yes, Kirchhoff's laws can be applied to both DC (direct current) and AC (alternating current) circuits. However, the calculations may differ slightly for AC circuits due to the added complexity of dealing with changing voltages and currents.

5. Are there any limitations or assumptions when using Kirchhoff's laws in a multiloop circuit?

Yes, there are a few limitations and assumptions when using Kirchhoff's laws in a multiloop circuit. One limitation is that the laws assume that the circuit is in a steady state, meaning that the current and voltages are not changing over time. Additionally, the laws assume that all components in the circuit are ideal, with no resistance or other factors that may affect the flow of current.

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