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:
A hydrogen atom consists of an electron revolving in a circular orbit of radius r with certain velocity v around a proton located at the nucleus of the atom. The electrostatic force of attraction between the revolving electron and the proton provides the requisite centripetal force to keep it in the orbit. According to Bohr’s model, an electron can revolve only in certain stable orbits. The angular momentum of the electron in these orbits is some integral multiple of \(\frac{h}{2π}\), where h is the Planck’s constant.
Ion | Q4+ | Xb+ | Yc+ | Zd+ |
---|---|---|---|---|
Radius (pm) | 53 | 66 | 40 | 100 |
Q4+, Xb+, Yc+, Zd+ are respectively
Match the pollination types in List-I with their correct mechanisms in List-II:
List-I (Pollination Type) | List-II (Mechanism) |
---|---|
A) Xenogamy | I) Genetically different type of pollen grains |
B) Ophiophily | II) Pollination by snakes |
C) Chasmogamous | III) Exposed anthers and stigmas |
D) Cleistogamous | IV) Flowers do not open |