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A nucleus X of mass M. intially at rest ...

A nucleus X of mass M. intially at rest undergoes alpha decay according to the equation
`_(Z)^(A)Xrarr._(Z-2)^(A-4)Y+._(2)^(4)He`
The alpha particle emitted in the above proces is found to move in a circular track of radius r in a uniform magnetic field B. Then (mass and charge of `alpha` particle are m and q respectively)

A

The ratio of kinetic energies of the alpha particle and (doughether nucleus Y approximately equals `(M-m)/(m)`

B

the ratio of kinetic energies of the alpha particle and the doughter nucleus Y apporximately `(m)/(M)`

C

The enetgy relased in the process approximately equals `(M)/(M-m)(r^(2)q^(2)B^(2))/(2m)`

D

The energy released in the process apporximately equals `(M)/(M-m)((r^(2)q^(2)B^(2))/(2m))`

Text Solution

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The correct Answer is:
To solve the problem of the alpha decay of nucleus X and the motion of the emitted alpha particle in a magnetic field, we can follow these steps: ### Step 1: Understand the decay process The alpha decay process can be represented as: \[ _{Z}^{A}X \rightarrow _{Z-2}^{A-4}Y + _{2}^{4}He \] Here, nucleus X emits an alpha particle (which is a helium nucleus) and transforms into nucleus Y. ### Step 2: Identify the forces acting on the alpha particle When the alpha particle moves in a magnetic field, it experiences a magnetic force that acts as the centripetal force required for circular motion. The magnetic force \( F_B \) is given by: \[ F_B = qvB \] where \( q \) is the charge of the alpha particle, \( v \) is its velocity, and \( B \) is the magnetic field strength. ### Step 3: Set up the centripetal force equation The centripetal force required to keep the alpha particle moving in a circular path is given by: \[ F_C = \frac{mv^2}{r} \] where \( m \) is the mass of the alpha particle and \( r \) is the radius of the circular path. ### Step 4: Equate the forces Since the magnetic force provides the centripetal force, we can set the two equations equal to each other: \[ qvB = \frac{mv^2}{r} \] ### Step 5: Solve for velocity \( v \) Rearranging the equation to solve for \( v \): \[ v = \frac{qBr}{m} \] ### Step 6: Calculate the kinetic energy of the alpha particle The kinetic energy \( E \) of the alpha particle can be expressed as: \[ E = \frac{1}{2}mv^2 \] Substituting the expression for \( v \) into the kinetic energy formula: \[ E = \frac{1}{2}m\left(\frac{qBr}{m}\right)^2 \] This simplifies to: \[ E = \frac{1}{2} \frac{q^2B^2r^2}{m} \] ### Step 7: Interpret the result This equation gives us the kinetic energy of the alpha particle in terms of its charge \( q \), the magnetic field \( B \), the radius of the circular path \( r \), and its mass \( m \).
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