The Balmer series of the hydrogen atom corresponds to electron transitions where the final energy level is \(n_f = 2\). The general formula for the wave number \(\bar{\nu}\) for transitions in hydrogen is given by:
\(\bar{\nu} = R \left( \frac{1}{n^2_f} - \frac{1}{n^2_i} \right)\)
Where \(R\) is the Rydberg constant, \(n_i\) is the initial energy level, and \(n_f\) is the final energy level.
For the Balmer series, \(n_f = 2\). Given the possible values of \(\bar{\nu}\):
We need to check which values correspond to transitions to \(n_f = 2\).
Calculating the values for different \(n_i\) for \(n_f = 2\):
The values \(\frac{5R}{36}\), \(\frac{3R}{16}\), and \(\frac{21R}{100}\) correspond to transitions in the Balmer series as calculated above.
Therefore, the correct set of wave numbers that belong to the Balmer series is:
\(\frac{5R}{36}, \frac{3R}{16}, \frac{21R}{100}\)
The wavelength of spectral line obtained in the spectrum of Li$^{2+}$ ion, when the transition takes place between two levels whose sum is 4 and difference is 2, is
Spherical node shown in figure-1 is best represented by which point in figure-2. 