The binding energy per nucleon in a nucleus is a measure of how strongly the nucleons (protons and neutrons) are bound together. This energy is dependent on the mass number \( A \) of the nucleus, and its trend as a function of \( A \) shows an interesting pattern.
As a function of mass number \( A \), the binding energy per nucleon increases with \( A \) up to iron (\( A \approx 56 \)) and then decreases as \( A \) increases further. This is because:
The correct graph representing this behavior is one that shows a peak at \( A = 56 \) (for iron) with the binding energy per nucleon increasing initially as \( A \) increases and then decreasing for heavier nuclei.
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:
Bittu and Chintu were partners in a firm sharing profit and losses in the ratio of 4 : 3. Their Balance Sheet as at 31st March, 2024 was as follows:
On 1st April, 2024, Diya was admitted in the firm for \( \frac{1}{7} \)th share in the profits on the following terms:
Prepare Revaluation Account and Partners' Capital Accounts.