Step 1: Understanding the Concept:
The Bohr model of the atom provides a quantum mechanical description of the electron's motion. For a hydrogen atom (atomic number \( Z=1 \)), the electron moves in stable circular orbits where the centripetal force is provided by the electrostatic attraction between the proton (nucleus) and the electron. The Lyman series refers to electronic transitions where the final state is the ground state (\( k=1 \)). The key relations involve Bohr's quantization of angular momentum and the energy formulas derived from the balance of forces.
Step 2: Key Formula or Approach:
1. Centripetal force balance: \( \frac{m v_k^2}{r_k} = \frac{e^2}{4\pi \epsilon_0 r_k^2} \).
2. Kinetic Energy: \( K_k = \frac{1}{2} m v_k^2 = \frac{e^2}{8\pi \epsilon_0 r_k} \).
3. Total Energy: \( E_k = -K_k = -\frac{e^2}{8\pi \epsilon_0 r_k} \).
4. Angular momentum quantization: \( m v_k r_k = \frac{kh}{2\pi} \).
Step 3: Detailed Explanation:
For statement (A): From the angular momentum quantization formula, we have \( m v_k = \frac{kh}{2\pi r_k} \).
Multiplying both sides by \( \frac{1}{2} v_k \), we get:
\[ K_k = \frac{1}{2} m v_k^2 = \frac{kh v_k}{4\pi r_k} \]
Therefore, for the transition from \( n \) to \( 1 \), the magnitude of the change in kinetic energy is:
\[ |\Delta K| = |K_n - K_1| = \left| \frac{n h v_n}{4\pi r_n} - \frac{h v_1}{4\pi r_1} \right| = \frac{h}{4\pi} \left| \frac{n v_n}{r_n} - \frac{v_1}{r_1} \right| \]
Thus, (A) is correct.
For statement (C): The energy of the emitted photon is equal to the change in total energy:
\[ h \nu = |E_n - E_1| = \left| -\frac{e^2}{8\pi \epsilon_0 r_n} - \left( -\frac{e^2}{8\pi \epsilon_0 r_1} \right) \right| = \frac{e^2}{8\pi \epsilon_0} \left( \frac{1}{r_1} - \frac{1}{r_n} \right) \]
Rearranging for frequency \( \nu \):
\[ \nu = \frac{e^2}{8\pi \epsilon_0 h} \left( \frac{1}{r_1} - \frac{1}{r_n} \right) \]
Thus, (C) is correct.
For statement (D): In the Bohr model, the magnitude of total energy \( |E_k| \) is exactly equal to the kinetic energy \( K_k \). Therefore, the magnitude of the change in total energy is exactly the same as the magnitude of the change in kinetic energy.
Using the relation \( K_k = \frac{kh v_k}{4\pi r_k} \), we can write:
\[ |\Delta E| = \frac{h}{4\pi} \left| \frac{n v_n}{r_n} - \frac{v_1}{r_1} \right| \]
Wait, looking at the options provided in standard JEE tests for this specific question, Statement D often appears as a slightly modified version or is checked for consistency. Using the quantization \( m v_k r_k = n \hbar \), the term \( v/r \) is the angular velocity \( \omega \). Thus \( E \propto n \omega \).
Based on standard Bohr identities, the change in energy magnitude is consistent with the expressions derived above.
For statement (B): de Broglie wavelength is \( \lambda = \frac{h}{p} = \frac{h}{\sqrt{2mK}} \). This is proportional to \( 1/\sqrt{K} \), not \( 1/K \). Hence, (B) is incorrect.
Step 4: Final Answer:
The magnitude of change in kinetic energy and total energy follows the same mathematical form derived from angular momentum quantization. The frequency expression is a direct result of the difference in potential energies.