Step 1: Understanding the Concept:
Frequency of hydrogen spectral lines is given by \( \nu = RcZ^2 \left( \frac{1}{n_1^2} - \frac{1}{n_2^2} \right) \). We need to find the difference in frequencies for specified transitions in Lyman and Balmer series and relate them.
Step 2: Key Formula or Approach:
Lyman Series (\( n_1=1 \)):
1st line: \( 2 \to 1 \). 2nd line: \( 3 \to 1 \).
Balmer Series (\( n_1=2 \)):
1st line: \( 3 \to 2 \). 2nd line: \( 4 \to 2 \).
Step 3: Detailed Explanation:
Let \( K = Rc \).
For Lyman Series:
Frequency of 1st line (\( \nu_{L1} \)): \( K(1 - \frac{1}{4}) = \frac{3K}{4} \).
Frequency of 2nd line (\( \nu_{L2} \)): \( K(1 - \frac{1}{9}) = \frac{8K}{9} \).
Difference \( f = \nu_{L2} - \nu_{L1} = K\left(\frac{8}{9} - \frac{3}{4}\right) = K\left(\frac{32-27}{36}\right) = \frac{5K}{36} \).
So, \( K = \frac{36f}{5} \).
For Balmer Series:
Frequency of 1st line (\( \nu_{B1} \)): \( K(\frac{1}{4} - \frac{1}{9}) = K(\frac{5}{36}) \).
Frequency of 2nd line (\( \nu_{B2} \)): \( K(\frac{1}{4} - \frac{1}{16}) = K(\frac{3}{16}) \).
Difference \( \Delta \nu_B = \nu_{B2} - \nu_{B1} = K\left(\frac{3}{16} - \frac{5}{36}\right) \).
LCM of 16 and 36 is 144.
\( \frac{3 \times 9}{144} - \frac{5 \times 4}{144} = \frac{27 - 20}{144} = \frac{7K}{144} \).
Substitute \( K = \frac{36f}{5} \):
\( \Delta \nu_B = \frac{7}{144} \times \frac{36f}{5} \)
\( = \frac{7f}{4 \times 5} \) (since \( 144/36 = 4 \))
\( = \frac{7f}{20} \).
Step 4: Final Answer:
The difference is \( \frac{7f}{20} \).