The energy levels in a hydrogen-like ion are described by \( E_n = - \frac{13.6 \, \text{eV} \times Z^2}{n^2} \), where \( E_n \) denotes the energy of the \( n^{th} \) level, \( Z \) is the atomic number, and \( n \) is the principal quantum number (taking values 1, 2, 3, etc.). The energy difference between the 2nd excitation state (\( n = 3 \)) and the ground state (\( n = 1 \)) is provided as 108.8 eV. The energy for the \( n = 3 \) state is \( E_3 = - \frac{13.6 Z^2}{9} \), and the energy for the \( n = 1 \) state (ground state) is \( E_1 = - 13.6 Z^2 \). The energy difference \( \Delta E \) is calculated as \( \Delta E = E_1 - E_3 = - 13.6 Z^2 - \left( - \frac{13.6 Z^2}{9} \right) = 13.6 Z^2 \left( 1 - \frac{1}{9} \right) = \frac{108.8 Z^2}{9} \). Given \( \Delta E = 108.8 \, \text{eV} \), we set up the equation \( \frac{108.8 Z^2}{9} = 108.8 \), which simplifies to \( Z^2 = 9 \). Therefore, the atomic number \( Z \) is 3.
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. 