Concept:
Solving complex resistor networks involves identifying series and parallel combinations and applying Ohm's Law ($V = IR$) step-by-step.
• Parallel Resistance: For identical resistors $R$ in parallel, $R_{eq} = R/n$.
• Current Distribution: In parallel branches, current divides inversely to resistance. In series, current remains constant.
• Potential Drop: Total potential is the sum of drops across series components ($V = V_1 + V_2 + \dots$).
Step 1: Analyze the rightmost section near XY.
The potential across the $4\ \Omega$ resistor (XY) is given as $4\text{ V}$.
Using Ohm's Law ($I = V/R$), the current through this branch is:
\[ I_{XY} = \frac{4\text{ V}}{4\ \Omega} = 1\text{ A} \]
Since there are two $4\ \Omega$ resistors in parallel at the end, each carries $1\text{ A}$, making the total current entering that junction $2\text{ A}$.
Step 2: Simplify the central parallel network.
The two $8\ \Omega$ resistors are in parallel. Their equivalent resistance is:
\[ R_p = \frac{8 \times 8}{8 + 8} = 4\ \Omega \]
The current of $2\text{ A}$ from the previous step passes through this $4\ \Omega$ equivalent resistance, creating a potential drop of:
\[ V = 2\text{ A} \times 4\ \Omega = 8\text{ V} \]
This $8\text{ V}$ is also across the vertical $4\ \Omega$ resistor on the left of that section. The current through it is $I = 8\text{ V} / 4\ \Omega = 2\text{ A}$.
Step 3: Calculate total input potential AB.
The total current coming from point A is the sum of the branch currents: $2\text{ A} + 2\text{ A} = 4\text{ A}$.
Potential drop across input $2\ \Omega$ resistors at both top and bottom: $V = 4\text{ A} \times (2\ \Omega + 2\ \Omega) = 16\text{ V}$.
The potential across the central parallel bridge was determined to be $4\text{ V}$ based on the XY output.
\[ V_{AB} = 16\text{ V} + 4\text{ V} = 20\text{ V} \]