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Fundamentals of Electric Circuits

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3.2 Nodal Analysis 87<br />

Substituting Eq. (3.2.5) into Eq. (3.2.4) yields<br />

2v 2 v 2 2.4 1 v 2 2.4, v 1 2v 2 4.8 V<br />

From Eq. (3.2.3), we get<br />

Thus,<br />

■ METHOD 2 To use Cramer’s rule, we put Eqs. (3.2.1) to (3.2.3)<br />

in matrix form.<br />

From this, we obtain<br />

Similarly, we obtain<br />

¢ 1 <br />

¢ 2 <br />

<br />

<br />

<br />

<br />

<br />

<br />

¢ 3 <br />

<br />

<br />

<br />

v 3 3v 2 2v 1 3v 2 4v 2 v 2 2.4 V<br />

v 1 4.8 V, v 2 2.4 V, v 3 2.4 V<br />

£<br />

12 2 1<br />

0 7 1<br />

5 0 3 15<br />

12 2 1<br />

0 7 1<br />

3 12 1<br />

4 0 1<br />

5 2 0 15<br />

3 12 1<br />

4 0 1<br />

3 2 12<br />

4 7 0<br />

5 2 3 05<br />

3 2 12<br />

4 7 0<br />

3 2 1<br />

4 7 1<br />

2 3 1<br />

v 1<br />

§ £ v 2 § £<br />

v 3<br />

12<br />

0 §<br />

0<br />

(3.2.6)<br />

v 1 ¢ 1<br />

¢ , v 2 ¢ 2<br />

¢ , v 3 ¢ 3<br />

¢<br />

where ¢, ¢ 1 , ¢ 2 , and ¢ 3 are the determinants to be calculated as<br />

follows. As explained in Appendix A, to calculate the determinant <strong>of</strong><br />

a 3 by 3 matrix, we repeat the first two rows and cross multiply.<br />

3 2 1<br />

3 2 1 4 7 1<br />

¢ 3 4 7 1 3 5 2 3 15<br />

2 3 1 3 2 1 <br />

4 7 1 <br />

<br />

<br />

21 12 4 14 9 8 10<br />

84 0 0 0 36 0 48<br />

<br />

<br />

<br />

0 0 24 0 0 48 24<br />

<br />

<br />

<br />

0 144 0 168 0 0 24

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