The Semi-Empirical Mass Formula (Liquid-Drop Model)
What it claims: Proposed by Carl Friedrich von Weizsäcker (1935) and refined by Bethe & Bacher (1936), the semi-empirical mass formula models the nucleus as a liquid drop, predicting binding energy per nucleon from five real physical terms: volume (bulk binding), surface (a drop’s “skin” costs energy, same as surface tension), Coulomb (protons electrostatically repel each other), asymmetry (a quantum-statistical penalty for unequal proton/neutron counts, from the Pauli exclusion principle), and pairing (an extra bonus for even-even nuclei).
Catalog status: Proven Systems. This formula, fit against real measured binding energies, remains a standard teaching and working tool in nuclear physics nearly a century later — accurate to a few percent across most of the periodic table. Its known real limitation is that it’s a smooth model with no shell structure, so it systematically misses “magic number” nuclei (closed nuclear shells, e.g. tin-132, lead-208) that are unusually tightly bound — that gap is what motivated the nuclear shell model (Maria Goeppert Mayer & J. Hans D. Jensen, 1949, shared 1963 Nobel Prize), a real, separate, also-proven refinement.
Where PBT touches this: Paper 13 (currently an unpublished draft, not yet live on this site) re-derives this formula’s structure from PBT’s own “equilibrium bubble” pressure premise — reframing the Coulomb term as protons producing extra outward pressure, and offering a partial (explicitly incomplete, by the paper’s own admission) toy derivation of the asymmetry term’s quadratic form from discrete level-filling. The paper is unusually direct about its own limits: it states plainly that it reproduces the form of established terms rather than deriving electric charge or Pauli exclusion from anything deeper, and that its fitted coefficients (validated out-of-sample against 15 real withheld isotopes, RMSE 0.133 MeV) land within about 8% of the real textbook values — expected for using the correct functional form against real data, not an independent rediscovery of nuclear physics.
References
- von Weizsäcker, C.F. (1935). “Zur Theorie der Kernmassen.” Zeitschrift für Physik 96, 431–458.
- Bethe, H.A., Bacher, R.F. (1936). “Nuclear Physics A. Stationary States of Nuclei.” Reviews of Modern Physics 8, 82–229.
- Mayer, M.G. (1949). “On Closed Shells in Nuclei. II.” Phys. Rev. 75, 1969.
- Wang, M. et al. (2021). “The AME 2020 atomic mass evaluation.” Chinese Physics C 45, 030003.