The Lyman and Balmer series in the hydrogen spectrum correspond to transitions in the hydrogen atom that result in the emission of light in the ultraviolet and visible regions, respectively.
The frequency of the \( n \to 1 \) transition in the Lyman series is given by:
\[ \nu_1 = R_H \left( \frac{1}{1^2} - \frac{1}{2^2} \right) \]where \( R_H \) is the Rydberg constant for hydrogen.
The second Lyman line corresponds to the transition from \( n = 3 \) to \( n = 1 \), and the frequency is:
\[ \nu_2 = R_H \left( \frac{1}{1^2} - \frac{1}{3^2} \right) \]Thus, the difference in frequencies between the first and second Lyman lines is:
\[ \Delta \nu_{\text{Lyman}} = \nu_2 - \nu_1 = R_H \left( \frac{1}{1^2} - \frac{1}{3^2} \right) - R_H \left( \frac{1}{1^2} - \frac{1}{2^2} \right) \]Simplifying:
\[ \Delta \nu_{\text{Lyman}} = R_H \left( \frac{1}{1} - \frac{1}{9} - \frac{1}{1} + \frac{1}{4} \right) \] \[ \Delta \nu_{\text{Lyman}} = R_H \left( \frac{4}{9} - \frac{1}{4} \right) \] \[ \Delta \nu_{\text{Lyman}} = R_H \left( \frac{16}{36} - \frac{9}{36} \right) = R_H \times \frac{7}{36} \]The second Balmer line corresponds to the transition from \( n = 4 \) to \( n = 2 \), and the frequency is:
\[ \nu_{\text{Balmer}} = R_H \left( \frac{1}{2^2} - \frac{1}{4^2} \right) \] \[ \nu_{\text{Balmer}} = R_H \left( \frac{1}{4} - \frac{1}{16} \right) = R_H \times \frac{3}{16} \]We are given that the difference in frequencies of the first and second Lyman lines is equal to the frequency of the second Balmer line:
\[ \Delta \nu_{\text{Lyman}} = \nu_{\text{Balmer}} \]Substituting the expressions for the frequencies:
\[ R_H \times \frac{7}{36} = R_H \times \frac{3}{16} \]Thus, we see that this corresponds to the First Balmer line (which is the transition from \( n = 2 \) to \( n = 3 \)).
Thus, the correct answer is Option (4), First Balmer line.