\( f \)
Using the Rydberg formula for the frequencies of lines in the hydrogen spectrum: \[ f = R \left( \frac{1}{n_1^2} - \frac{1}{n_2^2} \right) \] For a jump from the third excited state (n=4) to the first excited state (n=2), the frequency is: \[ f = R \left( \frac{1}{2^2} - \frac{1}{4^2} \right) = R \left( \frac{1}{4} - \frac{1}{16} \right) = R \left( \frac{3}{16} \right) \] Comparing this with the frequency for the transition from the second orbit to the first, which is based on \( n_1 = 1, n_2 = 2 \), we find the ratio is \( \frac{1}{4} \).
Match the devices given in List I with their uses given in List II:
