Using the mass-energy equivalence \( E = \Delta m c^2 \), the mass defect \( \Delta m \) is calculated as:
\[ \Delta m = \frac{E}{c^2}. \]
Substituting the values:
\[ E = 18 \times 10^8 \, \text{J}, \, c = 3 \times 10^8 \, \text{m/s}, \]
\[ \Delta m = \frac{18 \times 10^8}{(3 \times 10^8)^2} = \frac{18 \times 10^8}{9 \times 10^{16}} = 2 \times 10^{-8} \, \text{kg}. \]
Converting \( \Delta m \) to micrograms (\( \mu g \)):
\[ \Delta m = 2 \times 10^{-8} \, \text{kg} = 20 \, \mu g. \]
Final Answer: 20 \( \mu g \)
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: