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Nuclear Equation Balancer

Chemistry

Conserve mass number A and atomic number Z. Solve for a missing particle, follow a decay chain, or count the α and β decays between two nuclides.

One arrow, at most one unknown (?). Try U-238 → ? + α, 238U, uranium-238 or N-14(n,p)?.

Symbols

Examples

23892

U

Uranium-238

solved
23490

Th

Thorium-234

42

He

alpha particle

Balanced: A 238 = 238, Z 92 = 92.

Alpha decay

α

Alpha decay: A − 4, Z − 2. The nucleus loses two protons and two neutrons.

Q-value unavailable: Th-234 isn't in this tool's mass table.

Conservation ledger

Mass number A

Left

238

Right

238

Atomic number Z

Left

92

Right

92

SideSpeciesCountAZ
leftU-238123892
rightTh-234 (solved)123490
rightα142
Left total23892
Right total23892

What did the decay do on the N–Z chart?

143144145146147148149N (neutrons)89909192939495ZαU-238Th-234
Alpha decay
SEMF valley of stability (approximate)
N = Z

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About This Tool

Nuclear Equation Balancer – Conserve A and Z, Name the Decay

This nuclear equation balancer solves the bookkeeping behind alpha, beta, gamma and electron-capture decay. Type an equation with one unknown, such as U-238 → ? + α, and it finds the missing nuclide or particle, shows the conservation of mass number (A) and atomic number (Z), names the process and, when the masses are in its table, gives the Q-value.

Why nuclear equations balance differently

A chemical equation balances atoms of each element, and the elements never change. A nuclear equation balances nucleons and charge. The element can change, because a nucleus that gains or loses protons becomes a different element. The rule is simple: the sum of A and the sum of Z must be equal on both sides. Electrons and positrons count in Z as −1 and +1, with A = 0.

The decay modes and their A/Z rules

  • Alpha decay: A − 4, Z − 2. Example: Ra-226 → Rn-222 + α.
  • Beta-minus decay: A unchanged, Z + 1. Example: C-14 → N-14 + e⁻ + ν̄.
  • Beta-plus decay: A unchanged, Z − 1. Example: F-18 → O-18 + e⁺ + ν.
  • Electron capture: A unchanged, Z − 1. Example: Be-7 + e⁻ → Li-7 + ν.
  • Gamma emission: A and Z unchanged. Example: Tc-99m → Tc-99 + γ.
Tip
β⁻ adds a proton, so Z goes up. It is easy to get the direction wrong because the particle that leaves has a negative charge.

Solving for the missing particle

Add up A and Z for the side that is complete, then subtract the known species on the other side. What is left is the missing species. For U-238 → ? + α the left side has A = 238 and Z = 92, the alpha particle takes A = 4 and Z = 2, so the unknown has A = 234 and Z = 90: thorium-234. A result of A = 0, Z = 0 could be a gamma photon or a neutrino, and the tool offers both. An unknown multiplier such as ?n is solved the same way, as long as one whole number fits.

Transmutation and shorthand notation

When a light projectile hits a target, physicists write the reaction as target(projectile, ejectile)product. Rutherford's 1919 experiment, N-14 + α → O-17 + p, is written ¹⁴N(α,p)¹⁷O. You can type either form, and the tool shows the other.

Decay chains and the four series

Heavy nuclei rarely reach stability in one step. The decay-chain tab applies one step at a time, or loads a natural series. Because an alpha decay changes A by 4 and a beta decay changes it by 0, A mod 4 never changes along a chain, which gives four classes: the thorium series (4n), the neptunium series (4n + 1), the uranium series (4n + 2) and the actinium series (4n + 3). Three end at lead because the closed proton shell at Z = 82 and the closed neutron shell at N = 126 make lead-206, lead-207 and lead-208 especially stable. The neptunium series is extinct in nature and ends at bismuth-209. The α/β counter answers the classic question of how many alpha and beta decays take U-238 to Pb-206: 8 and 6.

The Q-value in one paragraph

The Q-value is the energy released when the products are lighter than the reactants: Q = (m_reactants − m_products) · c². A positive Q means energy is released, and a spontaneous decay needs Q > 0. For the mass-defect detail and the binding-energy curve, use the Nuclear Binding Energy Calculator. For how much of a sample is left after a given time, use the Half-Life Calculator or the Radioactive Decay Simulator.

Frequently Asked Questions

Is the Nuclear Equation Balancer free?

Yes, Nuclear Equation Balancer is totally free :)

Can I use the Nuclear Equation Balancer offline?

Yes, you can install the webapp as PWA.

Is it safe to use Nuclear Equation Balancer?

Yes, any data related to Nuclear Equation Balancer only stored in your browser (if storage required). You can simply clear browser cache to clear all the stored data. We do not store any data on server.

How do you balance a nuclear equation?

Add up the mass numbers (A) on each side and the atomic numbers (Z) on each side. Both totals must match. If one species is missing, subtract the known A and Z of one side from the other side's totals to get the A and Z of the missing nucleus or particle, then look it up: A = 4, Z = 2 is an alpha particle, A = 234, Z = 90 is thorium-234.

What happens to A and Z in alpha, beta-minus, beta-plus and gamma decay?

Alpha decay lowers A by 4 and Z by 2. Beta-minus decay leaves A unchanged and raises Z by 1, because a neutron becomes a proton. Beta-plus decay (and electron capture) leaves A unchanged and lowers Z by 1. Gamma emission changes neither A nor Z; the nucleus only loses excitation energy.

What's the difference between beta-plus decay and electron capture?

Both turn a proton into a neutron and lower Z by 1, and both emit a neutrino. In beta-plus decay the nucleus emits a positron, which needs at least 1.022 MeV (two electron masses) of extra energy. In electron capture the nucleus absorbs an inner-shell electron instead, so it can happen when beta-plus decay is energetically forbidden.

Why does every natural decay chain end at lead?

Alpha and beta decays move a heavy nucleus toward the valley of stability, and nuclei near Z = 82 (lead) and N = 126 have closed proton and neutron shells that make them unusually stable. The uranium, thorium and actinium series end at lead-206, lead-208 and lead-207. The neptunium series ends at bismuth-209, which is effectively stable.

Why do some nuclear equations include a neutrino or antineutrino?

Beta decay conserves lepton number as well as A and Z. Beta-minus decay creates an electron, so it also creates an electron antineutrino to keep the lepton number at zero. Beta-plus decay and electron capture involve a neutrino. Textbook equations often leave them out because they carry no A or Z, so the A and Z balance is unaffected.