Energy released calculation using Binding energy and mass defect

In summary, the calculation of energy released during nuclear reactions can be determined using binding energy and mass defect. The mass defect is the difference between the mass of an atomic nucleus and the sum of the individual masses of its protons and neutrons. This mass defect is directly related to the binding energy, which represents the energy required to disassemble a nucleus into its constituent particles. According to Einstein's equation \(E=mc^2\), the energy released can be calculated by multiplying the mass defect by the square of the speed of light. This relationship highlights the conversion of mass into energy during nuclear reactions, providing insight into the stability of nuclei and the energy output of nuclear processes.
  • #1
phantomvommand
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TL;DR Summary
I notice a discrepancy in calculating the energy released when using binding energy and mass defect.
Consider the equation
X (200, 50) + n (1, 0) -> Y (120, 30) + Z (70, 20) + 11 n(1, 0)

Let p be the mass of a proton, n be the mass of a neutron.
BE(X) = [50p + 150n - M(X)] c^2
BE(Y) = [30p + 90n - M(Y)] c^2
BE(Z) = [20p + 50n - M(Z)]c^2

The energy released when using BE (products) - BE (reactants) is thus: [M(X) - M(Y) - M(Z) - 10n] c^2
On the other hand, the mass released using [Mass (reactants) - Mass (products)]c^2 = [M(X) - M(Y) - M(Z)] c^2

There is a difference of 10n * c^2. Which is the correct calculation and why is the other wrong? Thank you!
 
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  • #2
How can you leave out the neutrons?
 
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