\( f \)
Using the Rydberg formula for the frequencies of lines in the hydrogen spectrum: \[ f = R \left( \frac{1}{n_1^2} - \frac{1}{n_2^2} \right) \] For a jump from the third excited state (n=4) to the first excited state (n=2), the frequency is: \[ f = R \left( \frac{1}{2^2} - \frac{1}{4^2} \right) = R \left( \frac{1}{4} - \frac{1}{16} \right) = R \left( \frac{3}{16} \right) \] Comparing this with the frequency for the transition from the second orbit to the first, which is based on \( n_1 = 1, n_2 = 2 \), we find the ratio is \( \frac{1}{4} \).
In Bohr model of hydrogen atom, if the difference between the radii of \( n^{th} \) and\( (n+1)^{th} \)orbits is equal to the radius of the \( (n-1)^{th} \) orbit, then the value of \( n \) is:
Given the function:
\[ f(x) = \frac{2x - 3}{3x - 2} \]
and if \( f_n(x) = (f \circ f \circ \ldots \circ f)(x) \) is applied \( n \) times, find \( f_{32}(x) \).