Given: - Disintegration rate, \( \frac{dN}{dt} = 10^8 \, {s}^{-1} \) - Half-life, \( T_{1/2} = 3.3 \times 10^{12} \, {s} \)
Step 1: Calculate the decay constant \( \lambda \) The decay constant \( \lambda \) is related to the half-life by: \[ \lambda = \frac{\ln 2}{T_{1/2}} = \frac{0.693}{3.3 \times 10^{12}} \approx 2.1 \times 10^{-13} \, {s}^{-1} \]
Step 2: Calculate the number of radioactive atoms \( N \) The disintegration rate is given by: \[ \frac{dN}{dt} = \lambda N \] Solving for \( N \): \[ N = \frac{\frac{dN}{dt}}{\lambda} = \frac{10^8}{2.1 \times 10^{-13}} \approx 4.76 \times 10^{20} \]
Final Answer: \( 4.7 \times 10^{20} \)
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: