\(\frac{40}{3}V\)
To find the reading on the voltmeter connected across the 200 \((\Omega)\) resistor, we must first calculate the total resistance in the series circuit. The total resistance \(R_{\text{total}}\) is given by the sum of the individual resistances:
\(R_{\text{total}} = 100\,\Omega + 200\,\Omega = 300\,\Omega\)
Using Ohm's Law, the total current \(I\) flowing through the circuit is calculated as follows:
\(I = \frac{V_{\text{battery}}}{R_{\text{total}}} = \frac{20\,V}{300\,\Omega} = \frac{1}{15}\,A\)
Now, calculate the voltage drop across the 200 \((\Omega)\) resistor using Ohm's Law:
\(V_{200} = I \times 200\,\Omega = \frac{1}{15}\,A \times 200\,\Omega = \frac{200}{15}\,V = \frac{40}{3}\,V\)
The voltmeter reading is therefore \(\frac{40}{3}\,V\).
Thus, the correct answer is \(\frac{40}{3}\,V\).
Two cells of emf 1V and 2V and internal resistance 2 \( \Omega \) and 1 \( \Omega \), respectively, are connected in series with an external resistance of 6 \( \Omega \). The total current in the circuit is \( I_1 \). Now the same two cells in parallel configuration are connected to the same external resistance. In this case, the total current drawn is \( I_2 \). The value of \( \left( \frac{I_1}{I_2} \right) \) is \( \frac{x}{3} \). The value of x is 1cm.