Assertion (A): The binding energy per nucleon is practically independent of the atomic number for nuclei of mass number in the range 30 to 170. This is true because for medium and heavy nuclei, the binding energy per nucleon remains approximately constant and stable in this mass range.
Reason (R): Nuclear force is short-ranged. This is true because nuclear forces act only within a very short range (of the order of a few femtometers) and are responsible for binding nucleons together. Since the stability of the binding energy per nucleon is a consequence of the short-ranged nature of nuclear forces, the reason (R) correctly explains the assertion (A).
Thus, the correct answer is \( \boxed{(1)} \).
Mass Defect and Energy Released in the Fission of \( ^{235}_{92}\text{U} \)
When a neutron collides with \( ^{235}_{92}\text{U} \), the nucleus gives \( ^{140}_{54}\text{Xe} \) and \( ^{94}_{38}\text{Sr} \) as fission products, and two neutrons are ejected. Calculate the mass defect and the energy released (in MeV) in the process.
Given:
Let $ P_n = \alpha^n + \beta^n $, $ n \in \mathbb{N} $. If $ P_{10} = 123,\ P_9 = 76,\ P_8 = 47 $ and $ P_1 = 1 $, then the quadratic equation having roots $ \alpha $ and $ \frac{1}{\beta} $ is: