5000 A/m
Using the magnetic flux \( \Phi \) and the cross-sectional area \( A \), we first calculate the flux density \( B \): \[ B = \frac{\Phi}{A} = \frac{22 \times 10^{-6} \, \text{Wb}}{2 \times 10^{-5} \, \text{m}^2} = 1.1 \, \text{T} \] Given the susceptibility \( \chi = 699 \), we find the relative permeability \( \mu_r \): \[ \mu_r = 1 + \chi = 700 \] The absolute permeability \( \mu \) is then: \[ \mu = \mu_0 \mu_r = (4\pi \times 10^{-7}) \times 700 = 0.879 \, \text{H/m} \] Now, solve for \( H \): \[ H = \frac{B}{\mu} = \frac{1.1}{0.879} \approx 1250 \, \text{A/m} \]
The magnetic moment is associated with its spin angular momentum and orbital angular momentum. Spin only magnetic moment value of Cr^{3+ ion (Atomic no. : Cr = 24) is:
In Bohr model of hydrogen atom, if the difference between the radii of \( n^{th} \) and\( (n+1)^{th} \)orbits is equal to the radius of the \( (n-1)^{th} \) orbit, then the value of \( n \) is:
Given the function:
\[ f(x) = \frac{2x - 3}{3x - 2} \]
and if \( f_n(x) = (f \circ f \circ \ldots \circ f)(x) \) is applied \( n \) times, find \( f_{32}(x) \).