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264 ⏐⏐⏐ METHODS OF ANALYSIS AND SELECTED TOPICS (dc)<br />

Step 4: Applying Kirchhoff’s current law at node a (in a two-node network,<br />

the law is applied at only one node),<br />

I1 � I2 � I3 Step 5: There are three equations and three unknowns (units removed<br />

for clarity):<br />

2 � 2I1 � 4I3 � 0 Rewritten: 2I1 � 0 � 4I3 � 2<br />

4I3 � 1I2 � 6 � 0 0 � I2 � 4I3 � 6<br />

I1 � I2 � I3 I1 � I2 � I3 � 0<br />

Using third-order determinants (Appendix C), we have<br />

I 1 �<br />

D �<br />

I 2 �<br />

I 3 �<br />

2 0 4<br />

6 1 4<br />

0 1 �1<br />

2 0 4<br />

0 1 4<br />

1 1 �1<br />

2 2 4<br />

0 6 4<br />

1 0 �1<br />

D<br />

2 0<br />

0 1<br />

1 1<br />

D<br />

2<br />

6<br />

0<br />

� �1 A<br />

� 2 A<br />

� 1 A<br />

A negative sign in front of a<br />

branch current indicates only<br />

that the actual current is<br />

in the direction opposite to<br />

that assumed.<br />

Mathcad Solution: Once you understand the procedure for entering<br />

the parameters, you can use Mathcad to solve determinants such as<br />

FIG. 8.23<br />

Using Mathcad to verify the numerical calculations of Example 8.9.<br />

N A

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