Cambridge A-Level Physics 9702 – Mass Defect and Nuclear Binding Energy
Mass Defect and Nuclear Binding Energy
Learning Objective
By the end of this lesson you will be able to calculate the energy released in nuclear reactions using the relation \$E = c^{2}\,\Delta m\$ where \$\Delta m\$ is the mass defect.
Key Concepts
Atomic mass unit (u):\$1\ \text{u}=1.660539\times10^{-27}\ \text{kg}\$.
Mass defect (\$\Delta m\$): The difference between the sum of the masses of the separate nucleons and the actual mass of the nucleus.
Binding energy (\$Eb\$): The energy equivalent of the mass defect, \$Eb = \Delta m\,c^{2}\$.
Binding energy per nucleon:\$E_b/A\$, useful for comparing the stability of different nuclei.
Why Mass Defect Occurs
When protons and neutrons combine to form a nucleus, part of their total rest mass is converted into the energy that holds the nucleons together. This loss of mass is the mass defect.
Suggested diagram: A nucleus formed from separate protons and neutrons showing the mass defect as the difference between the total mass of free nucleons and the mass of the bound nucleus.
Calculating Mass Defect
Write the nuclear reaction and identify the reactants and products.
Obtain the atomic masses (in u) of all reactants and products from a reliable table.
Calculate the total mass of reactants (\$M{\text{react}}\$) and products (\$M{\text{prod}}\$).
Find the mass defect:
\$\Delta m = M{\text{react}} - M{\text{prod}}\$
(positive \$\Delta m\$ indicates mass loss and energy release).
This energy appears as kinetic energy of the fragments, gamma radiation, and the kinetic energy of the emitted neutrons.
Summary Checklist
Identify all reactants and products and write the balanced nuclear equation.
Use a reliable atomic mass table (in atomic mass units).
Calculate the mass defect \$\Delta m\$ in u, then convert to kg.
Apply \$E = c^{2}\Delta m\$ and convert the result to MeV.
Interpret the binding energy per nucleon to assess nuclear stability.
Common Pitfalls
Forgetting to include the mass of the incident neutron in fission calculations.
Using the mass of the neutral atom instead of the nuclear mass; the electron masses cancel when both sides contain the same number of electrons, but be consistent.
Neglecting to convert the mass defect from atomic mass units to kilograms before applying \$E = c^{2}\Delta m\$.
Practice Questions
Calculate the energy released when two deuterium nuclei (\$^{2}\!H\$) fuse to form a helium‑3 nucleus (\$^{3}\!He\$) and a neutron.
Determine the binding energy per nucleon for \$^{56}\!Fe\$ given its atomic mass is \$55.934937\ \text{u}\$.
A sample of \$^{239}\!Pu\$ undergoes alpha decay: \$^{239}\!Pu \rightarrow \,^{235}\!U + \,^{4}\!He\$. Compute the energy released.
Further Reading
Consult the Cambridge International AS & A Level Physics syllabus (9702) for additional examples and the recommended tables of nuclear masses.