
The circuit involves resistors in series and parallel. First, the two 4 \(\Omega\) resistors are in parallel. The total resistance of this parallel combination is: \[ \frac{1}{R_{\text{parallel}}} = \frac{1}{4} + \frac{1}{4} = \frac{2}{4} = \frac{1}{2} \] \[ R_{\text{parallel}} = 2 \, \Omega \] Now, this 2 \(\Omega\) combination is in series with the 5 \(\Omega\) resistor, so the total resistance of this combination is: \[ R_{\text{total1}} = 2 + 5 = 7 \, \Omega \] Next, this 7 \(\Omega\) is in parallel with the 10 \(\Omega\) resistor: \[ \frac{1}{R_{\text{total}}} = \frac{1}{7} + \frac{1}{10} \] \[ \frac{1}{R_{\text{total}}} = \frac{10 + 7}{70} = \frac{17}{70} \] \[ R_{\text{total}} = \frac{70}{17} \approx 4.12 \, \Omega \] So the equivalent resistance between A and B is approximately \(4.12 \, \Omega\).
Now, using Ohm's law, the total current in the circuit is: \[ I = \frac{V}{R_{\text{total}}} = \frac{6}{4.12} \approx 1.46 \, \text{A} \] The potential difference across the 5 \(\Omega\) resistor can be found using: \[ V = I \times 5 = 1.46 \times 5 = 7.3 \, \text{V} \]

Find the unknown frequency if 24 is the median of the following frequency distribution:
\[\begin{array}{|c|c|c|c|c|c|} \hline \text{Class-interval} & 0-10 & 10-20 & 20-30 & 30-40 & 40-50 \\ \hline \text{Frequency} & 5 & 25 & 25 & \text{$p$} & 7 \\ \hline \end{array}\]