In the figure shown, self-impedances of the two transmission lines are 1.5j p.u each, and $Z_m = 0.5j$ p.u is the mutual impedance. Bus voltages shown in the figure are in p.u. Given that $\delta > 0$, the maximum steady-state real power that can be transferred in p.u from Bus-1 to Bus-2 is

Step 1: Compute the net transfer reactance.
Each line reactance = $1.5j$ p.u.
Mutual reactance = $0.5j$ p.u.
For two coupled parallel lines, the positive-sequence transfer reactance is:
\[
X_{\text{eq}} = X - X_m = 1.5 - 0.5 = 1.0 \text{ p.u}
\]
Step 2: Use the standard power transfer formula.
The steady-state real power transferred is:
\[
P = \frac{|E||V|}{X_{\text{eq}}}\sin \delta
\]
Given $\delta > 0$, the maximum power occurs at $\delta = 90^\circ$:
\[
P_{\max} = \frac{|E||V|}{X_{\text{eq}}}
\]
Step 3: Substitute $X_{\text{eq} = 1$.}
\[
P_{\max} = |E||V|
\]
Step 4: Conclusion.
Thus the maximum real power transferred from Bus-1 to Bus-2 is:
\[
P_{\max} = |E||V|
\]
The incremental cost curves of two generators (\( \text{Gen A} \) and \( \text{Gen B} \)) in a plant supplying a common load are shown. If the incremental cost of supplying the common load is \( \lambda = 7400 \, \text{Rs/MWh} \), the common load in MW is ________________ (rounded to the nearest integer).
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: