To determine the ratio of the wavelengths emitted when an electron in a hydrogen atom transitions from the third excited state to the second excited state and then from the second excited to the first excited state, we need to use the formula for the wavelength of the photon emitted during an electron transition in a hydrogen atom:
The change in energy when an electron transitions from a higher energy level \( n_i \) to a lower energy level \( n_f \) is given by:
\(E = -13.6 \left(\frac{1}{n_f^2} - \frac{1}{n_i^2}\right)\text{ eV}\)
Where:
- \( n_i \) = initial energy level (quantum number), - \( n_f \) = final energy level (quantum number), - 13.6 eV is the ionization energy of hydrogen.
The wavelength of the emitted photon can be found using:
\(\lambda = \frac{hc}{E}\)
where \( h \) is Planck's constant and \( c \) is the speed of light. However, since we are looking for a ratio, these constants will cancel out in our calculations.
The ratio of the wavelengths is inversely proportional to the ratio of the energies, because: \(\lambda_1 = \frac{hc}{\Delta E_1}\) and \(\lambda_2 = \frac{hc}{\Delta E_2}\)
Thus, the ratio becomes: \(\frac{\lambda_1}{\lambda_2} = \frac{\Delta E_2}{\Delta E_1} = \frac{\frac{5}{36}}{\frac{7}{144}}\)
By solving this, we get:
Thus, the ratio of the wavelengths \( \lambda_1 : \lambda_2 \) is \(\frac{20}{7}\).