Question 1.61: Determine the power delivered to the 10 Ω resistor in the ci......

Determine the power delivered to the 10 Ω resistor in the circuit shown in Fig. 1.

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The given circuit has four nodes. Let us choose one of the nodes as reference. Let the voltage of the other three nodes be V_1 ,V_2 and V_3 as shown in Fig. 1. Let I_{s2} be the current delivered by the dependent voltage source.

Now, power delivered to 10 Ω resistor =\frac{V_3^2}{10}

The general node basis matrix equation of a circuit with three nodes excluding the reference is given by equation (1).

\left[\begin{array}{lll}G_{11} & G_{12} & G_{13} \\G_{21} & G_{22} & G_{23} \\G_{31} & G_{32} &G_{33}\end{array}\right]\left[\begin{array}{l}V_1 \\V_2 \\V_3\end{array}\right]=\left[\begin{array}{l}I_{11} \\I_{22} \\I_{33}\end{array}\right]               …..(1)

With reference to Fig. 1, the elements of conductance matrix and source current matrix can be formed as shown below :

\begin{array}{l|l|l}G _{11}=\frac{1}{2}+\frac{1}{5}=0.7 & G _{12}= G _{21}=-\frac{1}{5}=-0.2 & I _{11}=-10 \\G _{22}=\frac{1}{5}+\frac{1}{4}=0.45 & G _{13}= G _{31}=0 & I _{22}= I _{ s 2} \\G _{33}=\frac{1}{4}+\frac{1}{10}=0.35 & G _{23}= G _{32}=-\frac{1}{4}=-0.25 & I _{33}=10+0.3 V _{ x }\end{array}

On substituting the above terms in equation (1), we get,

\left[\begin{array}{rrr}0.7 & -0.2 & 0 \\-0.2 & 0.45 & -0.25 \\0 & -0.25 & 0.35\end{array}\right]\left[\begin{array}{l} V _1 \\V _2 \\V _3\end{array}\right]=\left[\begin{array}{r}-10 \\I _{ s 2} \\10+0.3 V _{ x }\end{array}\right]                             ….. (2)

Let us express the value of dependent sources in terms of node voltages. With reference to Fig. 2, we can write,

\begin{aligned}& V_x=-V_1 \quad \Rightarrow \quad 0.3 V_x=-0.3 V_1 \end{aligned}                    ….. (3)
 I_x=-\frac{V_1}{2}=-0.5 V_1                          ….. (4)
Also, with reference to Fig. 2, we get,

V_2=I_x                     ….. (5)

From equations (4) and (5), we can write,

V_2=-0.5 V_1                 ….. (6)

Using equations (3) and (6), equation (2) can be written as shown in equation (7).

\left[\begin{array}{rrr}0.7 & -0.2 & 0 \\-0.2 & 0.45 & -0.25 \\0 & -0.25 & 0.35\end{array}\right]\left[\begin{array}{r}V _1 \\-0.5 V _1 \\V _3\end{array}\right]=\left[\begin{array}{r}-10 \\I _{ s 2} \\10-0.3 V _1\end{array}\right]                       ….. (7)

From row-1 of equation (5), we get,

0.7 V_1-0.2 \times\left(-0.5 V_1\right)=-10 \quad \Rightarrow \quad 0.8 V_1=-10 \quad \Rightarrow \quad V_1=\frac{-10}{0.8}=-12.5 V

From row-3 of equation (5), we get,

-0.25 \times\left(-0.5 V _1\right)+0.35 V _3=10-0.3 V _1 \\ 0.125 V _1+0.35 V _3=10-0.3 V _1 \\\quad 0.35 V _3=10-0.3 V _1-0.125 V _1 \\ \therefore \quad V_3=\frac{10-0.425 V _1}{0.35}=\frac{10-0.425 \times(-12.5)}{0.35}=43.75 V \\ \therefore \text { Power delivered to } 10 \Omega \text { resistor }=\frac{ V _3^2}{10}=\frac{(43.75)^2}{10}=191.40625 W

 

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