The angular momentum of an electron in a stationary state of \(Li^{2+}\) (\(Z=3\)) is \( \frac{3h}{\pi} \). The radius and energy of that stationary state are respectively.
We are given that the angular momentum of an electron in a stationary state of \( Li^{2+} \) (\( Z = 3 \)) is \( \frac{3h}{\pi} \). To find the radius and energy of this state, we will use the Bohr model equations.
The angular momentum in the Bohr model is: \[ L = n \cdot \frac{h}{2\pi} \] Given: \[ \frac{3h}{\pi} = n \cdot \frac{h}{2\pi} \] Solving for \( n \): \[ n = 6 \]
The Bohr radius formula for a hydrogen-like atom is: \[ r_n = \frac{n^2 h^2}{4\pi^2 m_e k Z e^2} \] Where:
Substitute values: \[ r_n \approx 6.348 \, \text{Å} \]
Energy of an electron in Bohr model: \[ E_n = -\frac{Z^2 m_e e^4}{8 \epsilon_0^2 h^2} \cdot \frac{1}{n^2} \] Substituting: \[ E_n \approx -5.45 \times 10^{-19} \, \text{J} \]
The radius and energy of the stationary state for \( Li^{2+} \) are: