The Rydberg formula is employed to determine the frequency of emitted radiation during electron transitions in hydrogen-like ions: \[ u = RZ^2\left(\frac{1}{n_1^2} - \frac{1}{n_2^2}\right) \] Here, \( u \) represents frequency, \( R \) is the Rydberg constant (\(1.097 \times 10^7 \, \text{m}^{-1}\)), \( Z \) denotes the atomic number, and \( n_1 \) and \( n_2 \) are the principal quantum numbers of the involved energy levels.
Given \( u_{2 \to 1} = 3 \times 10^{15} \, \text{Hz} \), the following is obtained:
\[ u_{2 \to 1} = RZ^2\left(\frac{1}{1^2} - \frac{1}{2^2}\right) = RZ^2\left(\frac{3}{4}\right) \]
Using this relationship, we calculate \( u_{3 \to 1} \):
\[ u_{3 \to 1} = RZ^2\left(\frac{1}{1^2} - \frac{1}{3^2}\right) = RZ^2\left(\frac{8}{9}\right) \]
From the given \( u_{2 \to 1} = 3 \times 10^{15} \, \text{Hz} \), we have:
\[ 3 \times 10^{15} = RZ^2\left(\frac{3}{4}\right) \]
Solving for \( RZ^2 \), we get:
\[ RZ^2 = \frac{4 \times 3 \times 10^{15}}{3} = 4 \times 10^{15} \]
Substituting this value into the equation for \( u_{3 \to 1} \):
\[ u_{3 \to 1} = 4 \times 10^{15}\left(\frac{8}{9}\right) = \frac{32}{9} \times 10^{15} \, \text{Hz} \]
To match the requested format \(\frac{x}{9} \times 10^{15}\text{ Hz}\), \(x = 32\). Therefore, \(x = 32\).
