To solve this problem, we need to understand the relationship between the radius of the circular path, the kinetic energy of the charged particle, and the magnetic field.
When a charged particle moves in a magnetic field, it experiences a centripetal force that makes it move in a circular path. The centripetal force is provided by the magnetic Lorentz force. Therefore, for a proton moving in a circular path:
F_{\text{centripetal}} = F_{\text{magnetic}}The expression for centripetal force is:
F_{\text{centripetal}} = \frac{mv^2}{R}where:
The magnetic force is given by:
F_{\text{magnetic}} = qvBwhere:
Setting F_{\text{centripetal}} = F_{\text{magnetic}} gives:
\frac{mv^2}{R} = qvBSimplifying this expression for velocity, v:
v = \frac{qBR}{m}The kinetic energy (K.E) of the particle is related to its velocity by:
\text{K.E} = \frac{1}{2}mv^2Substituting v = \frac{qBR}{m} in the kinetic energy:
\text{K.E} = \frac{1}{2}m\left(\frac{qBR}{m}\right)^2 = \frac{q^2B^2R^2}{2m}Let's compare the kinetic energies of the proton and the alpha particle. For the same radius (R) and magnetic field (B), the equation becomes:
\frac{q^2}{m}_{\text{proton}} = \frac{q^2}{m}_{\alpha\text{-particle}}For a proton: charge (q_p = e), mass (m_p = m)
For an alpha particle: charge (q_{\alpha} = 2e), mass (m_{\alpha} = 4m).
Simplifying it, the kinetic energy of the alpha particle:
\text{K.E}_{\alpha} = \frac{(2e)^2B^2R^2}{2 \cdot 4m} = \text{K.E}_pNow, solving for \text{K.E}_{\alpha}:
\text{K.E}_{\alpha} = \text{K.E}_{\text{proton}} = 1 \text{ MeV}Thus, the energy of the alpha particle needed to describe a circle of the same radius in the same field is 1 MeV.
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: