As show in the figure, in the steady state, the charge stored in the capacitor is _________ × 10–6 C.

In the steady state, the capacitor is fully charged, and no current flows through it. This means the voltage across the capacitor, \( V_c \), is equal to the voltage across the resistor \( R \) because they are in parallel.
The total voltage \( V \) across the entire circuit is 10 V (given by the battery). The current, \( I \), flowing through resistors \( r \) and \( R \) can be determined by the voltage divider rule:
\( V_R = V \cdot \frac{R}{R + r} = 10 \cdot \frac{100}{100 + 10} = 9.09\,\text{V} \)
Now, the voltage across the capacitor is \( V_c = V_R = 9.09 \, \text{V} \).
The charge \( Q \) stored in a capacitor is given by \( Q = C \cdot V_c \), where \( C \) is the capacitance:
\( Q = 1.1 \times 10^{-6} \, \text{F} \cdot 9.09 \, \text{V} = 10 \times 10^{-6}\,\text{C} \)
This value, \( 10 \times 10^{-6}\,\text{C} \), is within the range (10, 10).
A circuit consisting of a capacitor C, a resistor of resistance R and an ideal battery of emf V, as shown in figure is known as RC series circuit. 
As soon as the circuit is completed by closing key S₁ (keeping S₂ open) charges begin to flow between the capacitor plates and the battery terminals. The charge on the capacitor increases and consequently the potential difference Vc (= q/C) across the capacitor also increases with time. When this potential difference equals the potential difference across the battery, the capacitor is fully charged (Q = VC). During this process of charging, the charge q on the capacitor changes with time t as
\(q = Q[1 - e^{-t/RC}]\)
The charging current can be obtained by differentiating it and using
\(\frac{d}{dx} (e^{mx}) = me^{mx}\)
Consider the case when R = 20 kΩ, C = 500 μF and V = 10 V.