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

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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?
 
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.