Two parallel plate capacitors of capacitances \( C \) and \( 2C \) are joined with a battery of voltage difference \( V \) as shown in the figure. If the battery is removed and the space between the plates of the capacitor of capacitance \( C \) is completely filled with a material of dielectric constant \( K \), then find out:
The initial total capacitance (without dielectric) is the series combination of \( C \) and \( 2C \):
\[ \frac{1}{C_{\text{total, initial}}} = \frac{1}{C} + \frac{1}{2C} = \frac{3}{2C} \quad \Rightarrow \quad C_{\text{total, initial}} = \frac{2C}{3}. \]
After inserting the dielectric of constant \( K \) into the capacitor of capacitance \( C \), its new capacitance becomes:
\[ C' = KC. \]
The new total capacitance is the series combination of \( C' = KC \) and \( 2C \):
\[ \frac{1}{C_{\text{total, final}}} = \frac{1}{KC} + \frac{1}{2C}. \]
Simplifying:
\[ \frac{1}{C_{\text{total, final}}} = \frac{K + 2}{2KC}. \]
Thus:
\[ C_{\text{total, final}} = \frac{2KC}{K + 2}. \]
The charge on the initial combination is given by:
\[ Q_{\text{initial}} = C_{\text{total, initial}} \cdot V = \frac{2C}{3} \cdot V. \]
Since the battery is removed, the total charge remains the same. The final voltage \( V_{\text{final}} \) across the new combination is:
\[ V_{\text{final}} = \frac{Q_{\text{initial}}}{C_{\text{total, final}}}. \]
Substituting the values:
\[ V_{\text{final}} = \frac{\frac{2C}{3} \cdot V}{\frac{2KC}{K + 2}} = \frac{V \cdot (K + 2)}{3K}. \]
The total energy stored in a capacitor is given by:
\[ U = \frac{1}{2} C_{\text{total, final}} \cdot V_{\text{final}}^2. \]
Substituting \( C_{\text{total, final}} = \frac{2KC}{K + 2} \) and \( V_{\text{final}} = \frac{V \cdot (K + 2)}{3K} \):
\[ U = \frac{1}{2} \cdot \frac{2KC}{K + 2} \cdot \left(\frac{V \cdot (K + 2)}{3K}\right)^2. \]
Simplifying:
\[ U = \frac{1}{2} \cdot \frac{2KC}{K + 2} \cdot \frac{V^2 \cdot (K + 2)^2}{9K^2}. \]
\[ U = \frac{C V^2 \cdot (K + 2)}{9K}. \]
Thus, the total energy stored is:
\[ U = \frac{C V^2 (K + 2)}{9K}. \]
The circuit shown in the figure contains two ideal diodes \( D_1 \) and \( D_2 \). If a cell of emf 3V and negligible internal resistance is connected as shown, then the current through \( 70 \, \Omega \) resistance (in amperes) is:
(b) Order of the differential equation: $ 5x^3 \frac{d^3y}{dx^3} - 3\left(\frac{dy}{dx}\right)^2 + \left(\frac{d^2y}{dx^2}\right)^4 + y = 0 $