Key relationship
B≈avA−asA^(2/3)−acZ(Z−1)/A^(1/3)−aa(A−2Z)²/A+pairing.
Physics · Class 12
Intermediate nuclei have high binding per nucleon. Light nuclei can release energy by fusion and heavy nuclei by suitable fission when products have greater total binding. The curve is a trend, not a complete stability rule.
Open the interactive experiment →நடுத்தர அணுக்கருக்களில் ஒரு நியூக்ளியானுக்கான பிணைப்பு ஆற்றல் அதிகம். இலகு அணுக்கருக்களின் இணைவும் கனமானவற்றின் பிளவும்ஆற்றல் விடுவிக்கலாம்.
B≈avA−asA^(2/3)−acZ(Z−1)/A^(1/3)−aa(A−2Z)²/A+pairing.
Intermediate nuclei have high binding per nucleon. Light nuclei can release energy by fusion and heavy nuclei by suitable fission when products have greater total binding. The curve is a trend, not a complete stability rule.
Binding per nucleon alone does not provide decay barriers or every isotope’s stability.
Semi-empirical liquid-drop formula; curve uses approximate stable-Z choices. It is inaccurate for very light nuclei and ignores shell structure. Require1≤Z≤A.
Interpret nuclear-energy trends without assuming every reaction is allowed.
Try both scenarios, change one control, and predict the result before checking the graph and readouts.
Change one input while keeping the others fixed, as you would in a controlled experiment.
This liquid-drop parameter set places Fe56 near8.85 MeV/nucleon.
The model connects binding energy per nucleon with an observable reading. Check the equation and assumptions before applying it.
SI units · algebra · graph reading
Energy release is favored when products have?
Greater binding means lower product rest energy.
Course connection: Class XII Chapter 13. Consult the roadmap for CBSE, NEET, JEE Main and Advanced scope.