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

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To solve complex circuits using Kirchhoff's Laws, it's essential to correctly identify nodes, which are defined by continuous conducting paths rather than just connection points. The discussion highlights the calculation of various currents in a circuit, revealing an error in the initial application of Kirchhoff's Current Law (KCL) due to misunderstanding the node structure. The participants clarify that two connection dots can represent a single node if there are no components between them, leading to the conclusion that all currents entering and exiting must be accounted for. This understanding corrects the calculations, ensuring that all currents are balanced according to KCL. Proper identification of nodes is crucial for accurate circuit analysis.
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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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