The problem involves the physics of a radioactive nucleus emitting a photon and experiencing recoil, a situation that can be analyzed using the principles of conservation of momentum and energy.
Concept: When a nucleus emits a photon, it undergoes a recoil to conserve momentum. The photon carries momentum away, and by Newton's Third Law, the nucleus moves in the opposite direction.
Let’s break down the solution:
Conservation of Momentum: When the nucleus emits a photon of frequency $\upsilon$, it carries momentum $p = \frac{h\upsilon}{c}$, where $h$ is Planck’s constant and $c$ is the speed of light.
The nucleus must recoil with momentum $p_{\text{recoil}} = \frac{h\upsilon}{c}$ to conserve momentum.
Recoil Energy: The kinetic energy (recoil energy) of the nucleus can be expressed using the formula for kinetic energy:
$\text{KE} = \frac{p^2}{2M}$
Substitute $p = \frac{h\upsilon}{c}$:
$E_{\text{recoil}} = \frac{(\frac{h\upsilon}{c})^2}{2M} = \frac{h^2\upsilon^2}{2Mc^2}$
Thus, the recoil energy of the nucleus is $E_{\text{recoil}} = \frac{h^2\upsilon^2}{2Mc^2}$, which corresponds to the correct answer.
Conclusion: Among the given options, the correct answer is $h^2\upsilon^2 /2 Mc^2$. This option describes the energy associated with the recoil of the nucleus, aligning with the conservation laws and kinematic principles applicable to the emission of a photon by a nucleus.
The electric potential at the surface of an atomic nucleus \( (z = 50) \) of radius \( 9 \times 10^{-13} \) cm is \(\_\_\_\_\_\_\_ \)\(\times 10^{6} V\).
In a nuclear fission reaction of an isotope of mass \( M \), three similar daughter nuclei of the same mass are formed. The speed of a daughter nuclei in terms of mass defect \( \Delta M \) will be: