Monday, March 12, 2012

S1E8: KCL

In the circuit shown there are six unknown elements.


By measurements we have values for three of the branch currents: , , and .
[Note: The courseware wants the expression on the right-hand side of the equals; leave off the "i4 =" on the left hand side, and be careful of the case of i vs. I]

Again, we need to pick two conventions:
  • The sign of the term given the direction of the current arrow
  • The direction for tracing the branches
To make things simple, we'll follow the same convention as last time:
  • We'll trace the branch from the far node toward the chosen node.
  • Traversing a current arrow from tail to head will be a positive term in the equation
  • Traversing a current arrow from head to tail will be a negative term in the equation
In terms of the known currents, write an algebraic expression for the current

i4 is connected to two nodes, and the one on the right (middle of the circuit) has two other knowns, so that makes it a good candidate for the node.

(+i4) + (-i2) + (+i3) = 0

And now we solve in terms of i4:

i4 = i2 - i3

Write an algebraic expression for the current ?
i5 is also connected to two nodes. Because we just solved for i4, the node on the left otherwise has a known and a solved current, making it a good candidate.

(-i1) + (-i4) + (-i5) = 0

And now we solve in terms of i5:

(-i5) = i1 + i4

i5 = (-i1) + (-i4)

And we substitute for i4:

i5 = (-i1) + (-(i2 - i3))
i5 = (-i1) + (i3 + (-i2))
i5 = i3 - i2 - i1

Write an algebraic expression for the current ?

i6 is also connected to two nodes. The one on the left has two known currents, making it a good candidate for the choice of node.

i1 + i2 + i6 = 0

And now we solve in terms of i6:

i6 = -i1 - i2

No comments:

Post a Comment