Given reaction:
\[ ^3_2\text{He} \longrightarrow ^{12}_6\text{C} + \gamma \text{ rays} \]
Mass defect:
\[ \Delta m = (3m_{\text{He}} - m_{\text{C}}) \]
Calculating:
\[ \Delta m = (3 \times 4.002603 - 12) = 0.007809 \, \text{u} \]
Energy released:
\[ \text{Energy} = 931 \Delta m \, \text{MeV} \] \[ = 7.27 \, \text{MeV} = 727 \times 10^{-2} \, \text{MeV} \]
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:
The largest $ n \in \mathbb{N} $ such that $ 3^n $ divides 50! is:
Let \[ I(x) = \int \frac{dx}{(x-11)^{\frac{11}{13}} (x+15)^{\frac{15}{13}}} \] If \[ I(37) - I(24) = \frac{1}{4} \left( b^{\frac{1}{13}} - c^{\frac{1}{13}} \right) \] where \( b, c \in \mathbb{N} \), then \[ 3(b + c) \] is equal to: