A heavy nucleus splits; the two fragments sit higher on the binding-energy curve than the parent, closer to the iron peak, and the mass they shed comes out as ~200 MeV — mostly the Coulomb recoil of two positive fragments flying apart. The freed neutrons can start the next split. Rendered, not quoted.
source Bohr & Wheeler, The Mechanism of Nuclear Fission, Phys. Rev. 56, 426 (1939) — doi:10.1103/PhysRev.56.426
The nucleus is a charged liquid drop. Its binding energy follows the semi-empirical mass formula (Weizsaecker): volume minus surface minus Coulomb minus asymmetry, plus pairing. Fission is the ledger entry when a drop splits.
B(Z,A) = aVA − aSA2/3 − aCZ²/A1/3 − aA(A−2Z)²/A + δ. The Q of a split is just B(fragments) − B(parent).
Bohr & Wheeler 1939 gave fission its first worked theory: the drop deforms, the Coulomb term wins over surface tension past the saddle, and it snaps. The fragments climb toward the the-binding-energy Fe-56 peak, releasing ~200 MeV. The multiplication factor k sets criticality. This is the downhill mirror of the-nuclear-fusion — both cash in the same binding curve, one from above the peak, one from below.
Re-runs the full selfcheck live, including the planted tamper. Flips red if any invariant is broken.
A parent (U-236* = U-235 + n) and one representative split: Ba-141 + Kr-92 + 3 neutrons. Prompt neutrons per fission ν. Multiplication factor k.
"Fission energy is stored chemical energy released fast."
→ It is nuclear: ~106× chemical, from the mass difference B(frag)−B(parent).
"A single neutron guarantees a chain reaction."
→ Only if k≥1. Below critical mass most neutrons leak or are captured; k<1 dies out.
"Splitting any nucleus releases energy."
→ Only above the Fe-56 peak. Below it, splitting COSTS energy — that is fusion territory.
Planted void: force the fragment binding LOWER than the parent, so Q<0 and fission would ABSORB energy. The witness (7) catches it.