To find the energy acquired by the alpha particle, we need to analyze the motion of both the proton and the alpha particle under the influence of a uniform magnetic field. Both particles move in circular orbits due to the magnetic force acting as the centripetal force. The radius of the circular motion is given by the formula:
R = \frac{mv}{qB}
Where:
Since the radii of both particles' orbits are equal, we can equate their radii:
\frac{m_p v_p}{q_p} = \frac{m_{\alpha} v_{\alpha}}{q_{\alpha}}
Where the subscripts p and \alpha refer to the proton and the alpha particle, respectively.
Given that the proton has a kinetic energy of 1 \, \text{MeV}, the velocity of the proton is:
K_p = \frac{1}{2} m_p v_p^2
Solving for v_p:
v_p = \sqrt{\frac{2K_p}{m_p}}
Substituting for v_p in terms of K_p in the radii equation:
\frac{m_p \sqrt{\frac{2K_p}{m_p}}}{q_p} = \frac{m_{\alpha} v_{\alpha}}{q_{\alpha}}
And rearranging gives:
v_{\alpha} = \frac{q_{\alpha}}{m_{\alpha}} \frac{v_p q_p}{m_p}
Considering that an alpha particle consists of 2 protons and 2 neutrons (with mass approximately 4 times that of a proton and charge twice that of a proton), the relationship becomes:
v_{\alpha} = \frac{2q_p}{4m_p} v_p = \frac{1}{2} v_p
The kinetic energy for the alpha particle K_{\alpha} is given by:
K_{\alpha} = \frac{1}{2} m_{\alpha} v_{\alpha}^2
Substituting m_{\alpha} = 4m_p and v_{\alpha} = \frac{1}{2} v_p:
K_{\alpha} = \frac{1}{2} \cdot 4m_p \cdot \left(\frac{1}{2} v_p\right)^2 = \frac{1}{2} \cdot 4m_p \cdot \frac{1}{4} v_p^2
K_{\alpha} = m_p v_p^2 = 2K_p
As the proton's kinetic energy was 1 MeV, the alpha particle's energy is also:
K_{\alpha} = 1 \, \text{MeV}
Hence, the energy acquired by the alpha particle is 1 \, \text{MeV}. Thus, the correct answer is:
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: