Help to write Kirchhoff's equations for a circuit

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In summary, Homework statement says that the student needs to write equations for current sources and Kirchhoff's laws. The student has attempted to do so, but is having difficulty with the first law.
  • #1
amiras
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Homework Statement



Help me to write Kirchhoff's equations for this circuit. I'd like to think that I do understand this method, however Current sources giving me some problems.

attachment.php?attachmentid=32712&stc=1&d=1299040955.jpg


Homework Equations



Currents:
Sum = 0For closed loop:
[itex]\sum IR = \sum E[/itex]

The Attempt at a Solution



Since I am free to choose the currents directions, i choosed them in the picture with red arrows and named junctions and edges.

According to instructions, I need to write (junctions-1) = 7-1 = 6 equations for first Kirchhoff's law. And (all branches-(branches with current sources)-junctions-1) = 11-2-6=3 with second law. (is it really 3?, or some branches should be excluded)

Work:

I start with second law, because I am not sure how to use first one with current sources, I know that using second law, I can't pick contour with current sources.

So I take ABFGA: (I assume that current index is the same as rezistor)

R3*I3 + R5*I5 + I3*R3 = E3

Another contour BCEFB:

R6*I6 + R1*I1 - R5*I5 - R3*I3 = 0

And let's say BCDHB:

R6*I6 + I2*R2 - R3*I3 = E2

Is this is ok?

Please help to write equations for current.(Picture attached)
 

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  • #2
I would be tempted to turn J2 and R2, and J3 and R3 into their Thvenin equivalents and then write three simple KVL loop equations.
 
  • #3
hi amiras! :smile:

(try using the X2 icon just above the Reply box :wink:)
amiras said:
So I take ABFGA: (I assume that current index is the same as rezistor)

R3*I3 + R5*I5 + I3*R3 = E3

Another contour BCEFB:

R6*I6 + R1*I1 - R5*I5 - R3*I3 = 0

And let's say BCDEB:

R6*I6 + I2*R2 - R3*I3 = E2

correct so far (except you keep writing "3" instead of "4") :wink:

(and yes, there's only 3 loops since the loops with a current source don't count)
Please help to write equations for current.

first you need to name an extra current between AB (or, easier, is to treat AB as a single point with 4 wires, instead of two points with 3 wires each)

similarly you need to name a current through E2 and E3

then you need a current (KCL) equation at every node (except of course where you're joining two nodes into one, as at AB) :smile:
 
  • #4
gneill said:
I would be tempted to turn J2 and R2, and J3 and R3 into their Thvenin equivalents and then write three simple KVL loop equations.

I understand that, however I would like to try without it :)

tiny-tim said:
hi amiras! :smile:

(try using the X2 icon just above the Reply box :wink:)correct so far (except you keep writing "3" instead of "4") :wink:

(and yes, there's only 3 loops since the loops with a current source don't count)first you need to name an extra current between AB (or, easier, is to treat AB as a single point with 4 wires, instead of two points with 3 wires each)

similarly you need to name a current through E2 and E3

then you need a current (KCL) equation at every node (except of course where you're joining two nodes into one, as at AB) :smile:

Ok added currents Iab and Ie2 Ie3. Let's try without joining nodes, I now see that it would be very helpful. (question: we also can join nodes at D and M?)

And what could the 4th contour I am missing, could it be for example: HDEF?

So this is it, I assume positive is the currents that go in, and negative that goes out.

A: I3+J3-Iab=0
B: Iab-I4-I6=0
D: (Do i need to add current I_dm? Or I_dm=Ie2?)
M: (Same thing, I am not sure)
F: I1+I5-Ie3=0
K: Ie3-I3-J3=0
H: I4+Ie2-I5=0
 
  • #5
hi amiras! :smile:

(just got up :zzz: …)
amiras said:
question: we also can join nodes at D and M?

yes :smile:
And what could the 4th contour I am missing, could it be for example: HDEF?

you're not missing anything …

there are 4 loops, yes, but only three (any three) of them are independent …

if you add the KVL equations for three of them, it comes to minus the fourth, so the fourth one gives you no new information

the number of loops in a diagram (once you've removed the current-source loops) is the "obvious" number, the number of lines you have to cut to make it loopless :wink:
I assume positive is the currents that go in, and negative that goes out.

i'm not sure what you mean by that :confused:

positive is the same direction as the arrow, which as you said earlier you are free to choose
A: I3+J3-Iab=0
B: Iab-I4-I6=0
F: I1+I5-Ie3=0
K: Ie3-I3-J3=0
H: I4+Ie2-I5=0

yes, that's correct, but you also need one for node N :wink:
D: (Do i need to add current I_dm? Or I_dm=Ie2?)
M: (Same thing, I am not sure)

no, Idm is not Ie2

you do need an extra Idm (or preferably make D and M the same node) :smile:
 

FAQ: Help to write Kirchhoff's equations for a circuit

What are Kirchhoff's equations for a circuit?

Kirchhoff's equations are two laws that govern the behavior of electric circuits. The first law, known as Kirchhoff's Current Law, states that the algebraic sum of currents entering a node (or junction) in a circuit must equal zero. The second law, known as Kirchhoff's Voltage Law, states that the algebraic sum of voltages around a closed loop in a circuit must equal zero.

How do I write Kirchhoff's equations for a circuit?

To write Kirchhoff's equations for a circuit, you first need to identify the nodes and loops in the circuit. Then, for each node, write an equation that sets the sum of all currents entering the node equal to zero. For each loop, write an equation that sets the sum of all voltages around the loop equal to zero. These equations can then be solved simultaneously to determine the values of currents and voltages in the circuit.

What is the purpose of Kirchhoff's equations in circuit analysis?

Kirchhoff's equations are used to analyze and solve complex circuits by applying the laws of conservation of charge and energy. By writing and solving these equations, we can determine the values of currents and voltages in a circuit, which can help us understand the behavior of the circuit and make predictions about its performance.

Can Kirchhoff's equations be applied to all types of circuits?

Yes, Kirchhoff's equations can be applied to any type of circuit, whether it is a simple series or parallel circuit, or a more complex circuit with multiple loops and nodes. However, they are most commonly used in DC circuits and may need to be modified for circuits with varying currents or time-varying components.

Are there any limitations to using Kirchhoff's equations in circuit analysis?

While Kirchhoff's equations are useful for solving many types of circuits, they do have some limitations. For example, they assume ideal conditions and do not take into account factors such as resistance, capacitance, and inductance of components. They also cannot be used to analyze circuits with non-linear components. In these cases, more advanced techniques may be necessary for accurate analysis and prediction of circuit behavior.

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