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Let’s examine some steps in this procedure more closely. When locating the junctions in the circuit, do not be concerned about the direction of the currents. If the direction of current flow is not obvious, choosing any direction is sufficient as long as at least one current points into the junction and at least one current points out of the junction. If the arrow is in the opposite direction of the conventional current flow, the result for the current in question will be negative but the answer will still be correct.

The number of nodes depends on the circuit. Each current should be included in a node and thus included in at least one junction equation. Do not include nodes that are not linearly independent, meaning nodes that contain the same information.

Consider [link] . There are two junctions in this circuit: Junction b and Junction e . Points a , c , d , and f are not junctions, because a junction must have three or more connections. The equation for Junction b is I 1 = I 2 + I 3 , and the equation for Junction e is I 2 + I 3 = I 1 . These are equivalent equations, so it is necessary to keep only one of them.

The figure shows a circuit with positive terminal of voltage source V connected to resistor R subscript 1 connected to two parallel resistors R subscript 2 and R subscript 3 through junction b. The two resistors are connected to voltage source through junction e.
At first glance, this circuit contains two junctions, Junction b and Junction e , but only one should be considered because their junction equations are equivalent.

When choosing the loops in the circuit, you need enough loops so that each component is covered once, without repeating loops. [link] shows four choices for loops to solve a sample circuit; choices (a), (b), and (c) have a sufficient amount of loops to solve the circuit completely. Option (d) reflects more loops than necessary to solve the circuit.

The figure has four parts showing different loop combinations for a circuit with positive terminal of voltage source V connected to resistor R subscript 1 connected to two parallel resistors R subscript 2 and R subscript 3.
Panels (a)–(c) are sufficient for the analysis of the circuit. In each case, the two loops shown contain all the circuit elements necessary to solve the circuit completely. Panel (d) shows three loops used, which is more than necessary. Any two loops in the system will contain all information needed to solve the circuit. Adding the third loop provides redundant information.

Consider the circuit in [link] (a). Let us analyze this circuit to find the current through each resistor. First, label the circuit as shown in part (b).

Part a shows a circuit with two horizontal branches and three vertical branches. The first horizontal branch has two resistors of 3 Ω each and the second branch has two voltage sources of 24 V with positive terminal on the left and 29 V with positive terminal on the right. The left vertical branch is directly connected, the middle branch has a resistance of 3 Ω and the right branch has a resistance of 4 Ω. Part b shows the same circuit as part a with labelled junctions
(a) A multi-loop circuit. (b) Label the circuit to help with orientation.

Next, determine the junctions. In this circuit, points b and e each have three wires connected, making them junctions. Start to apply Kirchhoff’s junction rule ( I in = I out ) by drawing arrows representing the currents and labeling each arrow, as shown in [link] (b). Junction b shows that I 1 = I 2 + I 3 and Junction e shows that I 2 + I 3 = I 1 . Since Junction e gives the same information of Junction b , it can be disregarded. This circuit has three unknowns, so we need three linearly independent equations to analyze it.

The figure shows positive terminal of voltage source V connected to resistor R subscript 1 connected in series to two parallel resistors, R subscript 2 and R subscript 3.
(a) This circuit has two junctions, labeled b and e , but only node b is used in the analysis. (b) Labeled arrows represent the currents into and out of the junctions.

Next we need to choose the loops. In [link] , Loop abefa includes the voltage source V 1 and resistors R 1 and R 2 . The loop starts at point a , then travels through points b , e , and f , and then back to point a . The second loop, Loop ebcde , starts at point e and includes resistors R 2 and R 3 , and the voltage source V 2 .

Practice Key Terms 3

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Source:  OpenStax, University physics volume 2. OpenStax CNX. Oct 06, 2016 Download for free at http://cnx.org/content/col12074/1.3
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