Two passive two-port networks \( P \) and \( Q \) are connected as shown in the figure. The impedance matrix of network \( P \) is \( Z_P = \begin{bmatrix} 40 \, \Omega & 60 \, \Omega \\ 80 \, \Omega & 100 \, \Omega \end{bmatrix} \). The admittance matrix of network \( Q \) is \( Y_Q = \begin{bmatrix} 5 \, S & -2.5 \, S \\ -2.5 \, S & 1 \, S \end{bmatrix} \). Let the ABCD matrix of the two-port network \( R \) in the figure be \( \begin{bmatrix} \alpha & \beta \\ \gamma & \delta \end{bmatrix} \). The value of \( \beta \) in \( \Omega \) is ______ (rounded off to 2 decimal places).
Step 1: Analyze the network connection
For cascaded two-port networks, the overall ABCD parameters are obtained by multiplying the ABCD matrices of the individual networks.
Given:
Z-parameter matrix of network P:
\[ Z_P = \begin{bmatrix} 40 & 60 \\ 80 & 100 \end{bmatrix} \; \Omega \]
Admittance matrix of network Q:
\[ Y_Q = \begin{bmatrix} 5s & -2.5s \\ -2.5s & 1s \end{bmatrix} \]
Step 2: Convert Z-parameters of P to ABCD parameters
Standard Z-parameter equations:
\[ V_1 = Z_{11}I_1 + Z_{12}I_2 \] \[ V_2 = Z_{21}I_1 + Z_{22}I_2 \]
Substituting values:
\[ V_1 = 40I_1 + 60I_2 \quad (i) \] \[ V_2 = 80I_1 + 100I_2 \quad (ii) \]
From (ii):
\[ I_1 = \frac{V_2}{80} - \frac{100}{80}I_2 \]
Substitute in (i):
\[ V_1 = 40\left(\frac{V_2}{80} - \frac{100}{80}I_2\right) + 60I_2 \] \[ V_1 = \frac{V_2}{2} + 10I_2 \]
Comparing with standard ABCD equations:
\[ V_1 = AV_2 - BI_2,\quad I_1 = CV_2 - DI_2 \]
ABCD matrix of P:
\[ \begin{bmatrix} A & B \\ C & D \end{bmatrix}_P = \begin{bmatrix} \frac{1}{2} & -10 \\ \frac{1}{80} & \frac{100}{80} \end{bmatrix} \]
Step 3: Convert Y-parameters of Q to ABCD parameters
Standard Y-parameter equations:
\[ I_1 = Y_{11}V_1 + Y_{12}V_2 \] \[ I_2 = Y_{21}V_1 + Y_{22}V_2 \]
Substituting values:
\[ I_1 = 5V_1 - 2.5V_2 \quad (v) \] \[ I_2 = -2.5V_1 + V_2 \quad (vi) \]
From (vi):
\[ V_1 = \frac{V_2}{2.5} - \frac{I_2}{2.5} \]
Substitute into (v):
\[ I_1 = 5\left(\frac{V_2}{2.5} - \frac{I_2}{2.5}\right) - 2.5V_2 \] \[ I_1 = -\frac{1}{2}V_2 - 2I_2 \]
Thus, ABCD matrix of Q:
\[ \begin{bmatrix} A & B \\ C & D \end{bmatrix}_Q = \begin{bmatrix} \frac{2}{5} & \frac{2}{5} \\ -\frac{1}{2} & 2 \end{bmatrix} \]
Step 4: Find ABCD parameters of cascaded network R
\[ \begin{bmatrix} A & B \\ C & D \end{bmatrix}_R = \begin{bmatrix} A & B \\ C & D \end{bmatrix}_P \begin{bmatrix} A & B \\ C & D \end{bmatrix}_Q \]
\[ = \begin{bmatrix} \frac{1}{2} & -10 \\ \frac{1}{80} & \frac{10}{8} \end{bmatrix} \begin{bmatrix} \frac{2}{5} & \frac{2}{5} \\ -\frac{1}{2} & 2 \end{bmatrix} \]
\[ = \begin{bmatrix} 5.2 & -19.8 \\ 0.005 & -2.495 \end{bmatrix} \]
Step 5: Final ABCD parameters
\[ \alpha = 5.2,\quad \beta = -19.9~\Omega,\quad \gamma = 0.005,\quad \delta = 2.49 \]
Given an open-loop transfer function \(GH = \frac{100}{s}(s+100)\) for a unity feedback system with a unit step input \(r(t)=u(t)\), determine the rise time \(t_r\).
Consider a linear time-invariant system represented by the state-space equation: \[ \dot{x} = \begin{bmatrix} a & b -a & 0 \end{bmatrix} x + \begin{bmatrix} 1 0 \end{bmatrix} u \] The closed-loop poles of the system are located at \(-2 \pm j3\). The value of the parameter \(b\) is: