To determine the principal quantum number \( n \) of the excited state from which a hydrogen atom transitions to the ground state, emitting a photon of wavelength \( \lambda \), we can use the Rydberg formula for hydrogen. This formula is given by:
\(\frac{1}{\lambda} = R \left( \frac{1}{1^2} - \frac{1}{n^2} \right)\)
Here:
Given that the atom transitions from an excited state to the ground state (n = 1), the formula simplifies to:
\(\frac{1}{\lambda} = R \left( 1 - \frac{1}{n^2} \right)\)
We need to solve for \( n \), so we rearrange the equation:
\(\frac{1}{\lambda} = R - \frac{R}{n^2}\)
Rearranging gives:
\(\frac{R}{n^2} = R - \frac{1}{\lambda}\)
Solving for \( n^2 \), we get:
\(n^2 = \frac{R}{R - \frac{1}{\lambda}} = \frac{R}{\frac{R\lambda - 1}{\lambda}} = \frac{\lambda R}{\lambda R - 1}\)
Taking the square root, we find:
\(n = \sqrt{\frac{\lambda R}{\lambda R - 1}}\)
Thus, the principal quantum number \( n \) of the excited state is \(\sqrt{\frac{\lambda R}{\lambda R - 1}}\), which matches the provided correct answer.