Kirchhoff Rules

There are circuits, such as the one on the right, that cannot be reduced to an equivalent series or parallel resistance. What to do? Fortunately, there are two rules, named after Kirchhoff, that enable us to solve all circuits containing any arbitrary arrangement of resistors and batteries (or, more generally, sources of external potential differences). Kirchhoff's rules, in the form they are stated here, do not apply to circuits containing "active components" (e.g. transistors that amplify), or "non Ohmic" components -- they work only with so called "linear", (or "passive") components.

Rule 1:

The net current flowing into any junction must equal to the net current flowing out of that junction.
Ii = 0

This tells us that the sum of all currents Ii, i = 1, ..., n, at any given junction is 0, where we count currents flowing into a point as positive, and currents flowing out of the point as negative. Basically, this tells us that "what goes in must come out" -- that's just the principle of conservation of charge.

Rule 2:

The sum over all potential differences around any closed loop must sum to zero.
Vk - Ii Ri = 0

where the individual Vk, k = 1, ..., m, are the potentials supplied by the batteries in a given loop; and Ii, i = 1, ..., n are the currents flowing through the resistors Ri, resulting in voltage drops across the resistors in that same loop.

If you multiply both of these quantities with the current flowing in the respective arms of the loop, you realize that the first is the power generated in the batteries or other sources of external potential difference, and the second is just the power dissipated. So this rule is basically a statement of the principle of conservation of energy.

How can one use Kirchhoff rules?

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