An electron revolving in the \( n^{th} \) Bohr orbit has magnetic moment \( \mu \). If \( \mu_n \) is the value of \( \mu \), the value of \( x \) is:
2
1
3
0
The magnetic moment \( \mu \) of an electron in the \( n^{th} \) Bohr orbit is calculated using the formula:
\[ \mu = \frac{e}{2m} r^2, \]
with the following definitions:
- \( e \) represents the electron's charge.
- \( m \) denotes the electron's mass.
- \( r \) is the radius of the electron's orbit.
For a hydrogen atom, the radius of the \( n^{th} \) Bohr orbit is determined by:
\[ r_n = n^2 \frac{h^2}{4\pi^2 ke^2m}, \]
where \( h \) is Planck’s constant and \( k \) is Coulomb’s constant.
Substituting the expression for \( r_n \) into the magnetic moment formula yields:
\[ \mu_n = \frac{e}{2m} \left( n^2 \frac{h^2}{4\pi^2 ke^2m} \right) = \frac{eh^2n^2}{8\pi^2 ke^2m^2}. \]
This equation simplifies to:
\[ \mu_n = n^2 \left( \frac{eh^2}{8\pi^2 ke^2m^2} \right). \]
Using \( \mu_1 \) (the magnetic moment for the first orbit) as a reference, the ratio can be determined as:
\[ \frac{\mu_n}{\mu_1} = n^2. \]
Consequently, for \( n = 1 \):
\[ \frac{\mu_n}{\mu_1} = 1^2 = 1. \]
Therefore, the value of \( x \) is: 1
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. 