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:
\[
P_{\max} = |E||V|
\]
In the Wheatstone bridge shown below, the sensitivity of the bridge in terms of change in balancing voltage \( E \) for unit change in the resistance \( R \), in V/Ω, is __________ (round off to two decimal places).
