The wavelengths of radiation emitted when an electron transitions between energy levels in a hydrogen atom can be derived from the Rydberg formula:
\[
\frac{1}{\lambda} = R_H \left( \frac{1}{n_1^2} - \frac{1}{n_2^2} \right)
\]
where:
- \( \lambda \) is the wavelength of the radiation emitted,
- \( R_H \) is the Rydberg constant for hydrogen (\( R_H = 1.097 \times 10^7 \ \text{m}^{-1} \)),
- \( n_1 \) and \( n_2 \) are the principal quantum numbers of the initial and final energy levels, respectively.
Maximum Wavelength:
The maximum wavelength corresponds to the transition from the first excited state (\( n_2 = 2 \)) to the ground state (\( n_1 = 1 \)):
\[
\frac{1}{\lambda_{\text{max}}} = R_H \left( \frac{1}{1^2} - \frac{1}{2^2} \right) = R_H \left( 1 - \frac{1}{4} \right) = \frac{3}{4} R_H
\]
Thus,
\[
\lambda_{\text{max}} = \frac{4}{3 R_H}
\]
Minimum Wavelength:
The minimum wavelength corresponds to the transition from the highest possible energy state to the ground state. As \( n_2 \to \infty \), the equation becomes:
\[
\frac{1}{\lambda_{\text{min}}} = R_H \left( \frac{1}{1^2} - \frac{1}{\infty^2} \right) = R_H
\]
Thus,
\[
\lambda_{\text{min}} = \frac{1}{R_H}
\]
Ratio of Minimum to Maximum Wavelength:
The ratio of the minimum to maximum wavelength is:
\[
\frac{\lambda_{\text{min}}}{\lambda_{\text{max}}} = \frac{\frac{1}{R_H}}{\frac{4}{3 R_H}} = \frac{3}{4}
\]
Final Answer: The ratio of the minimum to maximum wavelength is \( \boxed{\frac{3}{4}} \).