Understanding Kirchhoff's Laws: Solving Circuits with Multiple Voltage Sources

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In summary, the conversation discusses a problem involving calculating work done, power dissipated, and current passing through a circuit with given values for resistors and voltages. The conversation also mentions using Kirchhoff's law to solve the problem, and there is a discussion about units and a possible error.
  • #1
fluidistic
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Homework Statement


See picture for the problem.
1)Calculate the work done to move a charge a= 0.7 x 10 ^(-3)C from A to B, passing by R2.
2)The power dissipated in R3.
3)The current passing by R1.


2. Given equations
R1=R3=100 omhs, R2=200 ohms, R4=300 omhs.
e1=e3= 5 V, e2=10 V and e4=15 V.


The Attempt at a Solution


I realize that the problem is very simple if only I get the current passing through each branch of the circuit. However, applying Kirchhoff's law of voltage, I reach non sense.


More precisely, let i1 be the current passing through e3, let's suppose it in the clockwise direction. Let i3 be the current passing through the e1 branch, suppose its direction as down. Let i2 be the current passing through R3, anticlockwise.
Then I get, according to Kirchhoff's law of voltage:
[tex]\varepsilon _3 - \varepsilon _2 - \varepsilon _1 - i_1 R_2 -i_3 R_1=0[/tex] and [tex]\varepsilon _4 - i_2(R_3+R_4)- \varepsilon _1 - i_3R_1 =0[/tex].
From it I reach [tex]i_1= -20V+400 i_2[/tex]. Of course units cannot match so there's at least an error. But I don't know where. I don't see it in the arithmetic so I guess I've used wrongly Kirchhoff's law, but I don't see it...
Thanks for any help.
 

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  • #2
The equation becomes
200*i1 = -20V + 400*i2.
 
  • #3
rl.bhat said:
The equation becomes
200*i1 = -20V + 400*i2.

Ok thanks, I'm going to check it out right now. However assuming that you're right, I'm still stuck with the same problem. I have that a current is equal to a a constant times another current, plus a voltage. What am I misunderstanding? I mean a current should have at least one unit, and a current units one.
So I guess I made an error writing down Kirchhoff's law?

Edit: Ok, I reached the equation you provided, I forgot the 200 term in the last step.
But I'm still stuck, as stated above, in the same post. :)
 
Last edited:
  • #4
Consider i3 as (i1 + i2). The two equations become
-10 + 200i1 + 100(i1 + i2) =0 ...(1)
10 + 400i2 + 100(i1 + i2) = 0...(2) Solve these two equations to find i1 and i2.
 
  • #5
rl.bhat said:
Consider i3 as (i1 + i2). The two equations become
-10 + 200i1 + 100(i1 + i2) =0 ...(1)
10 + 400i2 + 100(i1 + i2) = 0...(2) Solve these two equations to find i1 and i2.

Ok I will do it. I'm just curious about what I found, that a current is worth something senseless. I'm surprised there is no error in this. So you really confirm there is no error?
 
  • #6
fluidistic said:
Ok I will do it. I'm just curious about what I found, that a current is worth something senseless. I'm surprised there is no error in this. So you really confirm there is no error?
I don't understand what you mean by senseless.
 
  • #7
rl.bhat said:
I don't understand what you mean by senseless.

Ok. I reached the following equation: [tex]i_1=2i_2-\frac{1V}{10}[/tex]. Although I realize I've not reached the final answer for [tex]i_1[/tex], I do realize that the left side of the equation is measured in amperes and that the right side of the equation is something measured in amperes + something measured in volts. It doesn't make sense to me. Could you please explain to me why it is possible? Or I'm missing something obvious?

I thank you for all your help and time, sir. I'm willing to learn as much as possible.
 
  • #8
You can write 1V/10 as 1V/(10 ohm). In that case have you got any problem?
Any way how did you get
i1 = 2*i2 - 1V/10 ?

If you add the two equations
-10 + 200i1 + 100(i1 + i2) =0 ...(1)
10 + 400i2 + 100(i1 + i2) = 0...(2)
you get
2*i1 + 3*i2 = 0
 
  • #9
rl.bhat said:
You can write 1V/10 as 1V/(10 ohm). In that case have you got any problem?
Any way how did you get
i1 = 2*i2 - 1V/10 ?
Ah yes, you're right! I totally missed this part, I should have carried the units.
I reached this from
rl.bhat said:
The equation becomes
200*i1 = -20V + 400*i2.

rl.bhat said:
If you add the two equations
-10 + 200i1 + 100(i1 + i2) =0 ...(1)
10 + 400i2 + 100(i1 + i2) = 0...(2)
you get
2*i1 + 3*i2 = 0
I was about to do this :smile:.

Thanks a lot for all. If I have any further problem I'll let you know.
 
  • #10
I still have some problems.

rl.bhat said:
If you add the two equations
-10 + 200i1 + 100(i1 + i2) =0 ...(1)
10 + 400i2 + 100(i1 + i2) = 0...(2)
you get
2*i1 + 3*i2 = 0
Are you sure you didn't make any error? In my first post I reached
[tex]\varepsilon _3 - \varepsilon _2 - \varepsilon _1 - i_1 R_2 -i_3 R_1=0[/tex], and
[tex]\varepsilon _4 - i_2(R_3+R_4)- \varepsilon _1 - i_3R_1 =0[/tex].
When I plug the values, I get these 2 equations:
[tex]-100(i_1+i_2)-10-200i_1=0[/tex], and
[tex]10-100i_2-100(i_1+i_2)-300i_2=0[/tex], which differ from your equations.
Solving for [tex]i_1[/tex], I reached [tex]i_1=-\frac{5i_2}{4}[/tex].

While I had reached [tex]i_1=2i_2-\frac{1V}{10 \Omega}[/tex].
So I can solve for [tex]i_2[/tex]. I get [tex]i_2=\frac{2}{65}A[/tex]. And thus [tex]i_1=-\frac{1}{26}A[/tex]. Did I do something wrong?

How did you get -10 + 200i1 + 100(i1 + i2) =0 ...(1)
10 + 400i2 + 100(i1 + i2) = 0...(2) ?
 
  • #11
How did you get -10 + 200i1 + 100(i1 + i2) =0 ...(1)
10 + 400i2 + 100(i1 + i2) = 0...(2) ?

Yes. You are right.
It should be
+10 + 200i1 + 100(i1 + i2) =0 ...(1)
-10 + 400i2 + 100(i1 + i2) = 0...(2) ?
 
  • #12
rl.bhat said:
How did you get -10 + 200i1 + 100(i1 + i2) =0 ...(1)
10 + 400i2 + 100(i1 + i2) = 0...(2) ?

Yes. You are right.
It should be
+10 + 200i1 + 100(i1 + i2) =0 ...(1)
-10 + 400i2 + 100(i1 + i2) = 0...(2) ?

We are still not in agreement. :rolleyes: This problem is a headache!
 
  • #13
I am getting i1 = 3/70 A and i2 = 2/70 A.
I think there is a problem in your sign convention. Will you state your sign conventions for Ε and I*R.
You have taken i1 in the clockwise direction. You have traversing the loop in the direction of i1. You have taken I*R product negative assuming here is a drop of potential. you have taken E3 positive, where as you are crossing it from positive terminal to negative terminal. Is it not a drop in potential?
 
  • #14
rl.bhat said:
I am getting i1 = 3/70 A and i2 = 2/70 A.
I think there is a problem in your sign convention. Will you state your sign conventions for Ε and I*R.
You have taken i1 in the clockwise direction. You have traversing the loop in the direction of i1. You have taken I*R product negative assuming here is a drop of potential. you have taken E3 positive, where as you are crossing it from positive terminal to negative terminal. Is it not a drop in potential?

Right about the clockwise direction for [tex]i_1[/tex]. I might be wrong of course, but as you said, I took [tex]\varepsilon _3[/tex] as a "climb of potential", i.e. not a drop. Should it be a drop of potential?
If so, then I should take [tex]\varepsilon _1[/tex] and [tex]\varepsilon _2[/tex] as a climb of potential instead of a drop of potential as I took.
 
  • #15
fluidistic said:
Right about the clockwise direction for [tex]i_1[/tex]. I might be wrong of course, but as you said, I took [tex]\varepsilon _3[/tex] as a "climb of potential", i.e. not a drop. Should it be a drop of potential?
If so, then I should take [tex]\varepsilon _1[/tex] and [tex]\varepsilon _2[/tex] as a climb of potential instead of a drop of potential as I took.
According to the convention, current moves from positive terminal to negative terminal in the external circuit, and from negative terminal to positive terminal inside the cell. So we are assuming that +ve terminal is at the higher potential.
So if you cross the cell from +ve to -ve terminal then it is a fall in potential.
 
  • #16
rl.bhat said:
According to the convention, current moves from positive terminal to negative terminal in the external circuit, and from negative terminal to positive terminal inside the cell. So we are assuming that +ve terminal is at the higher potential.
So if you cross the cell from +ve to -ve terminal then it is a fall in potential.

Ok thank you for all. I have to restart the whole problem. :smile:
 
  • #17
I get [tex]i_1=\frac{3}{70}A[/tex] as you, but I get [tex]i_2=-\frac{1}{35}A[/tex] which differs from your value. The most extraneous thing is that I got [tex]i_1[/tex] via [tex]i_2[/tex].
I have that [tex]i_1=\frac{1}{10}+2i_2[/tex].

Anyway, let's assume you are right.
To answer the first question, is the work done [tex]q(\varepsilon _2 - i_1 R_2)[/tex]?

2)Is the power dissipated in [tex]R_3[/tex] worth [tex]i_2 ^2 R_3[/tex]?

In my result of a negative current, does that mean that it is positive but in the other than assumed direction?
 
  • #18
i2 = 2/70 A = 1/35 A. I have not considered the sign of the current.
Other results are correct.
The negative sign indicates that the assumed direction of the current not correct.
 
  • #19
rl.bhat said:
i2 = 2/70 A = 1/35 A. I have not considered the sign of the current.
Other results are correct.
The negative sign indicates that the assumed direction of the current not correct.

Thank you very much for all, once again. Problem solved! :biggrin:
 

Related to Understanding Kirchhoff's Laws: Solving Circuits with Multiple Voltage Sources

What is Kirchhoff's circuit laws?

Kirchhoff's circuit laws are two fundamental principles that govern the behavior of electric circuits. The first law, also known as Kirchhoff's current law, states that the total current entering a junction in a circuit is equal to the total current exiting the junction. The second law, also known as Kirchhoff's voltage law, states that the sum of the voltage drops in a closed loop circuit is equal to the sum of the voltage sources in that same loop.

What are the applications of Kirchhoff's laws?

Kirchhoff's laws are used in the analysis and design of electric circuits, including circuits in electronic devices such as computers, televisions, and smartphones. They are also applied in power systems, telecommunications, and other areas of electrical engineering.

What is the problem with Kirchhoff's laws?

The main problem with Kirchhoff's laws is that they assume ideal conditions, which may not always be the case in real-world circuits. For example, Kirchhoff's voltage law assumes that there is no resistance in the connecting wires, which is not always true. This can lead to inaccuracies in the predicted values of currents and voltages in a circuit.

How can the problem with Kirchhoff's laws be addressed?

One way to address the problem with Kirchhoff's laws is to use more advanced circuit analysis techniques, such as nodal analysis or mesh analysis, which take into account the resistance of the connecting wires. Another approach is to use circuit simulators, which use numerical methods to solve complex circuits and can provide more accurate results.

Are Kirchhoff's laws still relevant in modern electrical engineering?

Yes, Kirchhoff's laws are still relevant in modern electrical engineering. While they may not always provide exact results, they are still valuable for understanding the basic principles of electric circuits and are often used as a starting point for more advanced analysis methods. They are also incorporated into many circuit analysis and simulation software programs.

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