The binding energy (\(B.E.\)) of a nucleus is given by:
\[B.E. = \Delta m c^2,\]
where \(\Delta m\) is the mass defect.
The mass defect for the isotope \({}^{12}_5 B\) is:
\[\Delta m = (5M_p + 7M_n) - M_0.\]
Substituting \(\Delta m\) into the binding energy equation:
\[B.E. = (5M_p + 7M_n - M_0)c^2.\]
Thus, the nuclear binding energy of the isotope is:
\[B.E. = (5M_p + 7M_n - M_0)c^2.\]
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: