Solution to Question 16
Figure 2: The nodal configuration.
In a capacitor network, the potential of a junction (Node O) is determined by the conservation of charge on the isolated plates connected to that junction. The sum of charges on the plates meeting at O must equal the initial net charge $Q_{net}$ (usually zero if not specified).
Note: The resistor $R$ in branch C does not affect steady-state potential as no DC current flows.
Given $V_A = -10\text{V}$, $V_C = 10\text{V}$, $V_{ground} = 0$, and $C_1=C_2=C_3=C_4=5\mu\text{F}$. The equation becomes:
We have one equation with two unknowns: $V_O$ and $V_B$. Additionally, $Q_{net}$ is technically unknown (though often assumed zero). Because $V_B$ is unknown, we cannot determine $V_O$. This validates statement (b).
If the charge on capacitor $C_2$ ($Q_2$) is specified, we have an additional constraint: $$ |V_O – V_B| = \frac{Q_2}{C_2} $$ This relates $V_B$ directly to $V_O$. If we also assume the standard condition that the junction was initially neutral ($Q_{net}=0$), the system becomes solvable for both $V_O$ and $V_B$. This validates statement (d).
