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:
\[ U = \frac{C V^2 (K + 2)}{9K}. \]
Define the coefficient of mutual inductance.
The coefficient of mutual inductance (\(M\)) is a measure of the ability of one coil to induce an electromotive force (EMF) in a nearby coil due to a changing current in the first coil. It is given by: \[ e = -M \frac{di}{dt} \]
If a current \( i = 10 \sin(100 \pi t) \, \mathrm{A} \) is flowing in a primary coil, and the maximum induced electromotive force in the secondary coil placed near it is \( 5 \pi \, \mathrm{volt} \), then the coefficient of mutual induction between these coils needs to be determined.
State the conclusions of Rutherford's \( \alpha \)-particle scattering experiment.
Differentiate between interference and diffraction of light. Explain qualitatively the diffraction phenomenon of light by a single slit. Light of 6000 Ã… wavelength is incident normally on a single slit of width \( 3 \times 10^{-4} \, \text{cm} \). Find out the angular width of the central maxima.
Show that the circumference of the orbit of an electron revolving in the \( n \)-th orbit is equal to \( n\lambda \) with the help of Bohr's quantum theory. Also, show the emission and absorption spectral lines between energy levels \( n = 1 \) and \( n = 3 \) of hydrogen atom.
What do you mean by the current sensitivity of a moving coil galvanometer? Resistance of a galvanometer is \( 50 \, \Omega \) and for full-scale deflection, the current is \( 0.05 \, \mathrm{A} \). What would be the required length of a wire to convert it into an ammeter of 5 A range? (Area of cross-section of wire = \( 2.7 \times 10^{-6} \, \mathrm{m^2} \), specific resistance of the wire material = \( 5.0 \times 10^{-7} \, \Omega \cdot \mathrm{m} \))
Obtain the formula for the internal resistance of a cell in terms of \( E \), \( V \), and \( R \), where \( E \), \( V \), and \( R \) are the electromotive force of the cell, potential difference across the external resistance, and external resistance, respectively.