The radius of an electron's orbit in Bohr's model is given by the formula: \[ r_n = \frac{n^2 h^2 \epsilon_0}{\pi m e^2 Z} \] Where:
- \( n \) is the principal quantum number,
- \( h \) is Planck's constant,
- \( \epsilon_0 \) is the permittivity of free space,
- \( m \) is the mass of the electron,
- \( e \) is the charge of the electron, and
- \( Z \) is the atomic number of the ion. We are asked to compare the Bohr radius of the 2nd orbit of \( \text{Be}^{3+} \) and various orbits of other atoms. For \( \text{Be}^{3+} \), the atomic number is \( Z = 4 \), and for the second orbit, \( n = 2 \). For hydrogen, \( Z = 1 \), and for the first orbit, \( n = 1 \).
The formula shows that the radius of the orbit is inversely proportional to \( Z \), and directly proportional to \( n^2 \).
Thus, the Bohr radius for the second orbit of \( \text{Be}^{3+} \) can be compared with the first orbit of hydrogen, as they both satisfy the relationship of proportionality when adjusted for their respective values of \( n \) and \( Z \).
Therefore, the Bohr radius of the 2nd orbit of \( \text{Be}^{3+} \) is equal to the Bohr radius of the 1st orbit of hydrogen.
Thus, the correct answer is 1st orbit of hydrogen.
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
A solid cylinder of mass 2 kg and radius 0.2 m is rotating about its own axis without friction with angular velocity 5 rad/s. A particle of mass 1 kg moving with a velocity of 5 m/s strikes the cylinder and sticks to it as shown in figure.
The angular velocity of the system after the particle sticks to it will be: