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NEET PHYSICSEasy

If M(A, Z), M_p, and M_n denote the masses of the nucleus ZAX_{Z}^{A}X, proton, and neutron respectively in units of u (1 u = 931.5 MeV/c^2) and BE represents its binding energy in MeV. Then:

A

M(A, Z) = Z M_p + (A-Z) M_n - BE/c^2

B

M(A, Z) = Z M_p + (A-Z) M_n + BE

C

M(A, Z) = Z M_p + (A-Z) M_n - BE

D

M(A, Z) = Z M_p + (A-Z) M_n + BE/c^2

Step-by-Step Solution

  1. Definition of Mass Defect (Δm\Delta m): The mass of a stable nucleus, M(A,Z)M(A, Z), is always less than the sum of the masses of its constituent nucleons (protons and neutrons) in their free state. This difference is called the mass defect. Δm=[ZMp+(AZ)Mn]M(A,Z)\Delta m = [Z M_p + (A-Z) M_n] - M(A, Z)
  2. Binding Energy Relation: This mass defect is converted into binding energy (BEBE) according to Einstein's mass-energy equivalence relation (E=mc2E = mc^2): BE=Δm×c2BE = \Delta m \times c^2 BE=([ZMp+(AZ)Mn]M(A,Z))c2BE = \left( [Z M_p + (A-Z) M_n] - M(A, Z) \right) c^2
  3. Rearrangement: To find the mass of the nucleus M(A,Z)M(A, Z), rearrange the equation: BEc2=ZMp+(AZ)MnM(A,Z)\frac{BE}{c^2} = Z M_p + (A-Z) M_n - M(A, Z) M(A,Z)=ZMp+(AZ)MnBEc2M(A, Z) = Z M_p + (A-Z) M_n - \frac{BE}{c^2}
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