Question:medium

If the wavelength of the first member of the Lyman series of hydrogen is \( \lambda \). The wavelength of the second member will be:

Updated On: Jan 13, 2026
  • \( \frac{27}{32} \lambda \)
  • \( \frac{32}{27} \lambda \)
  • \( \frac{27}{5} \lambda \)
  • \( \frac{5}{27} \lambda \)
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The Correct Option is A

Solution and Explanation

To calculate the wavelength of the second spectral line in the Lyman series, we employ the Rydberg formula for hydrogen. The Lyman series involves electron transitions to the n=1 energy level from higher levels (n=2, n=3, etc.).

The Rydberg formula for spectral line wavelength \( \lambda \) in hydrogen is:

\(\frac{1}{\lambda} = R \left( \frac{1}{n_1^2} - \frac{1}{n_2^2} \right)\)

Where:

  • \(R\) is the Rydberg constant (\(1.097 \times 10^7 \, \text{m}^{-1}\))
  • \(n_1\) is the final energy level (\(n_1 = 1\) for the Lyman series)
  • \(n_2\) is the initial energy level

The first line of the Lyman series results from a transition from \(n_2 = 2\) to \(n_1 = 1\). Its wavelength \( \lambda \) is calculated as:

\(\frac{1}{\lambda} = R \left( \frac{1}{1^2} - \frac{1}{2^2} \right) = R \left( 1 - \frac{1}{4} \right) = R \cdot \frac{3}{4}\)

The second line of the Lyman series originates from a transition from \(n_2 = 3\) to \(n_1 = 1\). Its wavelength is denoted \( \lambda_2 \) and given by:

\(\frac{1}{\lambda_2} = R \left( \frac{1}{1^2} - \frac{1}{3^2} \right) = R \left( 1 - \frac{1}{9} \right) = R \cdot \frac{8}{9}\)

To relate \( \lambda \) and \( \lambda_2 \), we divide the equation for \( \lambda \) by the equation for \( \lambda_2 \):

\(\frac{\frac{1}{\lambda}}{\frac{1}{\lambda_2}} = \frac{R \cdot \frac{3}{4}}{R \cdot \frac{8}{9}}\)

This simplifies to:

\(\frac{\lambda_2}{\lambda} = \frac{\frac{8}{9}}{\frac{3}{4}} = \frac{8}{9} \times \frac{4}{3} = \frac{32}{27}\)

Therefore, the wavelength of the second member, \( \lambda_2 \), is:

\(\lambda_2 = \frac{27}{32} \lambda\)

The result is: \( \frac{27}{32} \lambda \).

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