In a Bohr orbit, the total energy \( E \) of an electron is the sum of its kinetic energy \( K \) and potential energy \( U \): \[ E = K + U \] For a hydrogen atom, the potential energy \( U \) is given by: \[ U = -2K \] Thus, the total energy \( E \) is: \[ E = K - 2K = -K \] The ratio of kinetic energy to total energy is: \[ \frac{K}{E} = \frac{K}{-K} = -1 \] Therefore, the ratio is \(1: -1\).
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: