1. Electron Energy in Bohr Hydrogen Atom:
The energy of an electron in the \( n \)-th orbit of a Bohr hydrogen atom is described by:
\[ E_n = - \frac{13.6}{n^2} \, \text{eV} \]
Where:
For \( n = 1 \), \( E_1 = -13.6 \, \text{eV} \), which is the ground state energy. Given an energy of \( -3.4 \, \text{eV} \), the electron is in the second orbit (\( n = 2 \)). This is validated by:
\[ E_2 = - \frac{13.6}{2^2} = - \frac{13.6}{4} = - 3.4 \, \text{eV} \]
2. Bohr’s Angular Momentum Quantization:
Bohr’s model states that the angular momentum \( L \) of an electron in the \( n \)-th orbit is quantized as:
\[ L = n \hbar \]
Where:
3. Angular Momentum Calculation:
Using \(n = 2\) and \(\hbar = \frac{6.626 \times 10^{-34}}{2\pi} \, \text{J.s}\) in the angular momentum equation:
\(\quad L = 2 \times \frac{6.626 \times 10^{-34}}{2\pi}\) \(= 2.11 \times 10^{-34} \, \text{J.s}\)
4. Result:
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. 