To solve this problem, we need to determine the charge on capacitor \(Q\) when equilibrium is established after being connected to a charged capacitor \(P\). Initially, capacitor \(P\) is charged to a potential difference \(V = 6.0\,\text{V}\). The capacitance of \(P\) is \(C_P = 10 \times 10^{-6}\,\text{F}\). Thus, the initial charge on \(P\) is given by:
Initial Charge on \(P\):
\[ q_P = C_P \times V = 10 \times 10^{-6}\,\text{F} \times 6\,\text{V} = 6 \times 10^{-5}\,\text{C} \]
Upon connecting the capacitors \(P\) and \(Q\), they will reach a common potential difference \(V_f\) because they form a series circuit. The total charge is conserved:
\[ q_{\text{total}} = q_P = 6 \times 10^{-5}\,\text{C} \] The total capacitance \(C_{\text{total}}\) for capacitors in parallel is:
\[ C_{\text{total}} = C_P + C_Q = 10 \times 10^{-6}\,\text{F} + 20 \times 10^{-6}\,\text{F} = 30 \times 10^{-6}\,\text{F} \] The final potential difference \(V_f\) across both capacitors is:
\[ V_f = \frac{q_{\text{total}}}{C_{\text{total}}} = \frac{6 \times 10^{-5}\,\text{C}}{30 \times 10^{-6}\,\text{F}} = 2\,\text{V} \] Now, the charge \(q_Q\) on capacitor \(Q\) is given by:
\[ q_Q = C_Q \times V_f = 20 \times 10^{-6}\,\text{F} \times 2\,\text{V} = 4 \times 10^{-5}\,\text{C} \] Therefore, in the form \( \alpha \times 10^{-5}\,\text{C} \), we have \( \alpha = 4 \). The computed value \( \alpha = 4 \) falls within the given range 4,4, confirming the solution's accuracy.
An infinitely long straight wire carrying current $I$ is bent in a planar shape as shown in the diagram. The radius of the circular part is $r$. The magnetic field at the centre $O$ of the circular loop is :

The heat generated in 1 minute between points A and B in the given circuit, when a battery of 9 V with internal resistance of 1 \(\Omega\) is connected across these points is ______ J. 