How Do You Solve Complex Circuits Using Kirchhoff's Laws?

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Homework Help Overview

The discussion revolves around solving a circuit problem using Kirchhoff's Laws, specifically focusing on determining the values of various currents in a complex circuit configuration. The original poster provides specific current values and attempts to apply Kirchhoff's Current Law (KCL) to analyze the circuit.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants discuss the application of KCL to both outer and inner nodes, questioning the identification of nodes and the inclusion of certain currents in the equations. There is an exploration of whether multiple connection points represent distinct nodes or a single node.

Discussion Status

The discussion is ongoing, with participants providing insights into the nature of nodes in the circuit and clarifying misunderstandings about current flow. Some guidance has been offered regarding the interpretation of nodes and the relationships between currents, but no consensus has been reached on the specific calculations.

Contextual Notes

There is a noted confusion regarding the identification of nodes and the implications of continuous conducting paths in the circuit. Participants are also considering the impact of missing currents on their calculations.

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Homework Statement


Determine the values of the other currents in Figure P1.37, given that ia = 2 A, ic =−3 A,
ig = 6A,and ih= 1A.

ealHzUE.png



Homework Equations


∑currents entering a node = ∑currents exiting the node


The Attempt at a Solution



I used Kirchoff's Circuit Law on each of the outer nodes:

if = ig + ih = 6 + 1 = 7A

ia + id = if
2 + id = 7
id = 5A

ic + ih= ie
-3 + 1 = ie
ie = -2A

ib = ia + ic = 2 - 3 = -1A

I think I may have went wrong somewhere, because when I apply KCL to one of the inner nodes I get this:

ie + ig = id (?)
-2 + 6 ≠ 5
 
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yaro99 said:

Homework Statement


Determine the values of the other currents in Figure P1.37, given that ia = 2 A, ic =−3 A,
ig = 6A,and ih= 1A.

ealHzUE.png



Homework Equations


∑currents entering a node = ∑currents exiting the node


The Attempt at a Solution



I used Kirchoff's Circuit Law on each of the outer nodes:

if = ig + ih = 6 + 1 = 7A

ia + id = if
2 + id = 7
id = 5A

ic + ih= ie
-3 + 1 = ie
ie = -2A

ib = ia + ic = 2 - 3 = -1A

I think I may have went wrong somewhere, because when I apply KCL to one of the inner nodes I get this:

ie + ig = id (?)
-2 + 6 ≠ 5

There's only one "inner node" where B, D, G, and E meet; despite there being two connection dots there, they are all one single conducting path with no components in between.

So, your node equation needs to account for ##i_b##, too.
 
gneill said:
There's only one "inner node" where B, D, G, and E meet; despite there being two connection dots there, they are all one single conducting path with no components in between.

So, your node equation needs to account for ##i_b##, too.

Aha, in that case it will be
-2 + 6 = -1 + 5
4 = 4

How do I know that the node includes ##i_b##, is that current not affected by the current ##i_d##?

Is the point connecting B and D not a node?
 
The two inner nodes are actually one node.
You missed a current: two currents go into the node and two currents go out of the node.

[edit]gah: too slow!
 
yaro99 said:
How do I know that the node includes ##i_b##, is that current not affected by the current ##i_d##?

Is the point connecting B and D not a node?

So long as there is a continuous conducting path it is all one node. A node is not a dot on the diagram, it's the entire continuous conducting path.

To make it more clear, you can shift component E over a bit as follows:

attachment.php?attachmentid=65959&stc=1&d=1390527029.gif


The wiring in green is continuously connected, so it's all one node.
 

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gneill said:
So long as there is a continuous conducting path it is all one node. A node is not a dot on the diagram, it's the entire continuous conducting path.

To make it more clear, you can shift component E over a bit as follows:

attachment.php?attachmentid=65959&stc=1&d=1390527029.gif


The wiring in green is continuously connected, so it's all one node.

Ah, yes that confused me a bit. It makes sense now thanks!
 
Great - the other way to look at it is to add an extra current arrow ##\small{i_0}## in the gap between the "two" center nodes. You can tell which direction it has to point in by looking at the other currents - but it actually doesn't matter:

Current in = current out:
... so on the left node you get ##i_0 = i_b+i_d##
... and for the right node you get ##i_0=i_g+i_e##

... eliminate the ##\small{i_0}## term gives you ##i_b+i_d = i_g+i_e##

and it all comes out in the wash ;)

It's just easier to realize that the nodes for Kirkoffs laws actually include the entire wire between components. Thus two drawn node-symbols, on the diagram, that have no components between them, are one and the same.
 

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