Step 1: Analyze the error in Topology-A.
In Topology-A, the pressure coil is connected across the load, measuring \(V_L\). The current coil carries \(I_L\). The power measured is approximately \(P_W \approx V_L I_L \cos \phi_L + I_L^2 R_C\). The error is due to the power loss in the current coil, \(I_L^2 R_C\). To minimize this error, \(I_L^2 R_C \ll V_L I_L \cos \phi_L\), which implies \(I_L R_C \ll V_L \cos \phi_L\), or \(V_C \ll V_L\) (assuming \(\cos \phi_L\) is not very small).
Step 2: Analyze the error in Topology-B.
In Topology-B, the pressure coil is connected across the source, measuring \(V_S = V_L + V_C\). The current coil carries \(I_L\). The power measured is approximately \(P_W \approx V_S I_L \cos \phi'\). The error arises because the pressure coil measures \(V_S\) instead of \(V_L\). Another source of error is the current through the pressure coil (\(I_P\)) flowing through the current coil. The total current in the current coil is \(I_L + I_P\). To minimize the error due to \(I_P\), we need \(I_P \ll I_L\). The current \(I_P = V_S / Z_P \approx V_S / R_P\). Thus, we need \(V_S / R_P \ll I_L\), or \(I_L \gg I_P\).
Combining the conditions for low error in both topologies, we need \(V_L \gg V_C\) for Topology-A and \(I_L \gg I_P\) for Topology-B.