Step 1: Understanding the Lyman Series
The Lyman series corresponds to the transitions of electrons in a hydrogen atom from higher energy levels (for \( n = 2, 3, 4, \dots \)) to the \( n = 1 \) energy level. The wavelengths of these transitions can be calculated using the
Rydberg formula for hydrogen:
\[
\frac{1}{\lambda} = R_H \left( \frac{1}{n_1^2} - \frac{1}{n_2^2} \right)
\]
Where:
- \( \lambda \) is the wavelength of the emitted radiation,
- \( R_H \) is the Rydberg constant for hydrogen,
- \( n_1 = 1 \) (since it's the Lyman series),
- \( n_2 \) is the higher energy level (2, 3, 4, ...).
Step 2: Maximum and Minimum Wavelengths
1. Minimum Wavelength:
The minimum wavelength corresponds to the transition from \( n_2 \to \infty \) (since the energy difference is the greatest when the electron falls to the ground state, \( n = 1 \)):
\[
\frac{1}{\lambda_{\text{min}}} = R_H \left( \frac{1}{1^2} - \frac{1}{\infty^2} \right) = R_H \left( 1 \right)
\]
Therefore, the minimum wavelength \( \lambda_{\text{min}} \) is given by:
\[
\lambda_{\text{min}} = \frac{1}{R_H}
\]
2. Maximum Wavelength:
The maximum wavelength corresponds to the transition from \( n_2 = 2 \to n_1 = 1 \):
\[
\frac{1}{\lambda_{\text{max}}} = R_H \left( \frac{1}{1^2} - \frac{1}{2^2} \right) = R_H \left( 1 - \frac{1}{4} \right) = R_H \left( \frac{3}{4} \right)
\]
Therefore, the maximum wavelength \( \lambda_{\text{max}} \) is:
\[
\lambda_{\text{max}} = \frac{4}{3R_H}
\]
Step 3: Relating the Maximum Wavelength to the Minimum Wavelength
Given that the minimum wavelength is \( P \), we can write:
\[
\lambda_{\text{min}} = P = \frac{1}{R_H}
\]
From the above formula, the maximum wavelength \( \lambda_{\text{max}} \) is:
\[
\lambda_{\text{max}} = \frac{4}{3} \times \lambda_{\text{min}} = \frac{4}{3} \times P
\]
Step 4: Conclusion
The maximum wavelength of the Lyman series lines is \( \frac{4P}{3} \).
Thus, the correct answer is:
\[
\boxed{(A)} \, \frac{4P}{3}
\]