Jugami Physics

High School · Physics · Unit 15

Nuclear and Particle Physics: Decay, Fission and Quarks

What holds the center of an atom together, why some nuclei break apart and what protons are made of.

Almost all of an atom's mass sits in a nucleus about 100 000 times smaller than the atom itself. Packed in there are protons that repel each other with enormous electric force, yet most nuclei around us are stable. Something stronger holds them together, and when that grip shifts, the energy released can power the Sun or a city.

On this page you'll learn what isotopes are, how the strong force works, where nuclear energy comes from, the three main kinds of radioactive decay and what half-life means. Then you'll look at fission and fusion, the particles of the Standard Model and the machines used to find them. After that you can try the half-life and E = mc² calculator, read how the ideas developed and take the quiz. Relativity, photons and the structure of the atom are covered in Unit 9: Modern Physics.

A cluster of protons and neutrons forming a nucleus, giving off a particle and a wavy ray of energy.

On this page

Key words first

Nucleon

A proton or a neutron, the two kinds of particle in a nucleus.

Atomic number (Z)

The number of protons. It decides which element an atom is.

Mass number (A)

The total number of protons and neutrons.

Isotopes

Atoms of the same element with different numbers of neutrons, like carbon-12 and carbon-14.

Binding energy

The energy needed to pull a nucleus completely apart into separate protons and neutrons.

Half-life

The time it takes for half of the nuclei in a radioactive sample to decay.

Quark

A particle inside protons and neutrons. Each proton or neutron is made of three.

Lepton

A matter particle not made of quarks, such as the electron or a neutrino.

Idea 1: The nucleus and isotopes

A nucleus is written with its mass number on top and its atomic number below, like ¹⁴₆C for carbon-14. The atomic number Z counts the protons, and the mass number A counts protons plus neutrons, so the number of neutrons is N = A − Z.

Every carbon atom has 6 protons, but the number of neutrons can vary. Carbon-12, with 6 neutrons, makes up about 99% of carbon. Carbon-14, with 8, is rare and radioactive. Isotopes of an element behave the same way in chemical reactions, because chemistry depends on electrons, but their nuclei can behave very differently.

A nucleus is about 10⁻¹⁵ m across, a femtometer, while a whole atom is about 10⁻¹⁰ m.

Two carbon nuclei side by side. Carbon-12 has 6 protons and 6 neutrons; carbon-14 has 6 protons and 8 neutrons. Same element, different mass.carbon-126 protons + 6 neutronscarbon-146 protons + 8 neutronsprotonneutronTwo isotopes of carbon
Carbon-12 and carbon-14 have the same 6 protons. The two extra neutrons make carbon-14 heavier and unstable.

Idea 2: The strong force and binding energy

Protons repel each other, and inside a nucleus they're so close that the push is huge. What holds them together is the strong nuclear force. It attracts protons and neutrons to each other, and at distances of about a femtometer it's far stronger than the electric repulsion. But it fades to almost nothing beyond a few femtometers, so it only acts between close neighbors. Neutrons add attraction without adding repulsion, which is why heavy nuclei need more neutrons than protons.

Here's a surprise: a nucleus weighs less than the separate protons and neutrons that make it up. The missing mass is the mass defect. It was released as energy when the nucleus formed, following Einstein's E = mc². That energy is the binding energy. Nuclear masses are measured in atomic mass units (u), and 1 u of mass is equivalent to 931.5 MeV of energy.

Binding energy per nucleon tells you how tightly a nucleus is held. It peaks near iron-56 at about 8.8 MeV. Joining light nuclei, or splitting very heavy ones, moves toward that peak and releases energy.

Binding energy per nucleon plotted against mass number. It rises steeply from hydrogen-2 to helium-4, peaks near iron-56 at about 8.8 MeV, then slowly falls to about 7.6 MeV for uranium-238. Fusing light nuclei or splitting heavy ones moves toward the peak.02468050100150200250²H⁴He¹²C⁵⁶Fe²³⁸Ufusionfissionmass number Abinding energy per nucleon (MeV)
Binding energy per nucleon. Nuclei near iron are the most tightly bound, so energy comes out of fusing light nuclei or splitting heavy ones.

Idea 3: Radioactive decay

An unstable nucleus eventually changes into a more stable one by giving off radiation. The three main kinds are:

  • Alpha (α) decay: the nucleus throws out a helium-4 nucleus, 2 protons and 2 neutrons. Z drops by 2 and A drops by 4. Uranium-238 becomes thorium-234 this way.
  • Beta (β⁻) decay: a neutron turns into a proton, giving off an electron and an antineutrino. Z goes up by 1 and A stays the same. Carbon-14 becomes nitrogen-14 this way. In β⁺ decay, a proton becomes a neutron and gives off a positron.
  • Gamma (γ) decay: a nucleus with extra energy releases a high-energy photon. Z and A don't change.

In every decay, the totals of Z and A on each side of the equation match. Alpha particles are heavy and slow and are stopped by paper or skin, but they're dangerous if swallowed or breathed in. Beta particles get through more, and gamma rays need thick lead or concrete to block.

Alpha particles are stopped by a sheet of paper, beta particles by a few millimeters of aluminum, and gamma rays are only reduced by thick lead.paperaluminumleadalpha αbeta βgamma γreducedHow far each kind of radiation gets
The more massive and charged the radiation, the sooner it's stopped.

Idea 4: Half-life

You can't predict when one particular nucleus will decay, but a large sample follows a strict rule: in each half-life, half of whatever is left decays. After n half-lives, the amount left is

N = N₀ × (½)t/t½

Half-lives range enormously. Iodine-131, used in medicine, has a half-life of about 8 days. Carbon-14's is about 5 730 years, which is why it's used to date things that were once alive. Uranium-238's is about 4.5 billion years, close to the age of Earth.

A decay curve. After one half-life 50% of the nuclei remain, after two 25%, after three 12.5% and after four 6.25%.0100%150%225%312.5%4time, in half-livesHalf the nuclei decay in each half-life
Each half-life cuts the remaining amount in half, so it never quite reaches zero.

Idea 5: Fission and fusion

In fission, a heavy nucleus such as uranium-235 absorbs a neutron and splits into two medium-sized nuclei plus two or three neutrons, releasing about 200 MeV. Those neutrons can split more nuclei, setting off a chain reaction. In a nuclear power plant, control rods soak up spare neutrons so the reaction runs at a steady rate.

In fusion, light nuclei join to make a heavier one. Fusing deuterium and tritium, two isotopes of hydrogen, gives helium-4, a neutron and 17.6 MeV. Fusion powers the Sun, which turns about 4 million tonnes of mass into energy every second. On Earth it's hard to do, because the nuclei must be heated to about 100 million °C before they move fast enough to get past their electric repulsion.

Top: a neutron hits uranium-235, which splits into barium-141, krypton-92 and three neutrons, releasing about 200 MeV. Bottom: deuterium and tritium fuse into helium-4 and a neutron, releasing 17.6 MeV.Fissionuranium-235barium-141krypton-923 neutrons≈200 MeVFusiondeuterium+tritiumhelium-4+neutron+ 17.6 MeV
Fission splits a heavy nucleus; fusion joins light ones. Both move toward the most tightly bound nuclei and release energy.

Idea 6: The Standard Model and accelerators

Protons and neutrons aren't the smallest pieces. Each is made of three quarks. A proton is two up quarks and a down quark (uud); a neutron is one up and two downs (udd). Up quarks carry a charge of +⅔ and down quarks −⅓, so the proton's charge adds to +1 and the neutron's to 0.

The Standard Model lists all the known building blocks. There are six quarks and six leptons: the electron, the muon, the tau and three kinds of neutrino. Forces are carried by bosons: the photon carries the electromagnetic force, gluons the strong force, and the W and Z bosons the weak force behind beta decay. The Higgs boson goes with the field that gives many particles their mass. Gravity isn't part of the Standard Model.

The Standard Model. Six quarks: up, down, charm, strange, top, bottom. Six leptons: electron, muon, tau and their three neutrinos. Force carriers: gluon, photon, Z and W bosons. Plus the Higgs boson.quarks (top two rows), leptons (bottom two rows)uupccharmttopddownsstrangebbottomeelectronμmuonτtauνee neutrinoνμμ neutrinoνττ neutrinothree generations, left to rightforce carriers and the Higgs bosonggluonγphotonZZ bosonWW bosonHHiggs
The particles of the Standard Model: quarks and leptons make up matter, and bosons carry forces.

To see what's inside particles, physicists smash them together at high speed in particle accelerators. Electric fields speed up charged particles and magnets steer them. The Large Hadron Collider at CERN, near Geneva, is a ring 27 km around that collides protons at energies up to 13.6 TeV. By E = mc², the energy of a collision can turn into new, heavy particles, which is how the Higgs boson was found in 2012.

Worked examples

Try each one first, then open the solution. Use c = 3.00 × 10⁸ m/s and 1 u = 931.5 MeV.

1. Inside carbon-14

How many protons and neutrons are in ¹⁴₆C?

Show solution
Protons = Z = 6
Neutrons = 14 − 6 = 8

Every carbon nucleus has 6 protons; only the neutrons change.

2. Alpha decay of uranium-238

What nucleus is left when ²³⁸₉₂U gives off an alpha particle?

Show solution
A: 238 − 4 = 234
Z: 92 − 2 = 90, thorium
²³⁸₉₂U → ²³⁴₉₀Th + ⁴₂He

The mass numbers and atomic numbers balance on both sides.

3. 80 g of iodine-131 after 24 days

Iodine-131 has a half-life of 8.0 days. How much of an 80 g sample is left after 24 days?

Show solution
24 ÷ 8.0 = 3 half-lives
80 → 40 → 20 → 10 g

The rest has turned into xenon-131.

4. Mass defect of helium-4

Two hydrogen-1 atoms (1.007825 u each) and two neutrons (1.008665 u each) have more mass than a helium-4 atom (4.002602 u). Find the binding energy.

Show solution
Parts: 2(1.007825) + 2(1.008665) = 4.032980 u
Defect: 4.032980 − 4.002602 = 0.030378 u
E = 0.030378 × 931.5 ≈ 28.3 MeV, or about 7.07 MeV per nucleon

Using hydrogen atoms instead of bare protons lets the electron masses cancel.

5. Energy in 1.0 g of mass

How much energy would 1.0 g of mass give if all of it turned into energy?

Show solution
E = mc² = 0.0010 × (3.00 × 10⁸)²
= 9.0 × 10¹³ J

That's about 25 million kilowatt-hours. Fission turns only about 0.1% of the fuel's mass into energy.

6. Charge of a proton from quarks

A proton is uud. Find its charge from its quarks.

Show solution
+⅔ + ⅔ − ⅓ = +1

For a neutron, udd: +⅔ − ⅓ − ⅓ = 0.

Try it: half-life and E = mc² calculator

N = N₀(½)^(t/t½) and E = mc² calculator

How the ideas developed

Nuclear physics began with an accident in a drawer of photographic plates. Within fifty years it had produced the first reactor, and within a century, a complete list of the particles that make up ordinary matter.

  1. 1896 Henri Becquerel finds that uranium salts fog photographic plates even in the dark: radioactivity.
  2. 1898 Marie and Pierre Curie discover polonium and radium.
  3. 1911 Ernest Rutherford's gold foil results show that an atom's mass is packed into a tiny nucleus.
  4. 1932 James Chadwick discovers the neutron. The same year, John Cockcroft and Ernest Walton split lithium nuclei with an accelerator.
  5. 1938–39 Otto Hahn and Fritz Strassmann find barium after hitting uranium with neutrons; Lise Meitner and Otto Frisch explain it as fission.
  6. 1942 Chicago Pile-1, led by Enrico Fermi, runs the first self-sustaining chain reaction on 2 December.
  7. 1964 Murray Gell-Mann and George Zweig propose quarks.
  8. 2012 CERN announces the discovery of the Higgs boson on 4 July.
  9. 2022 The National Ignition Facility gets more fusion energy out of a fuel pellet than its lasers put in.

Test yourself

The Nuclear and Particle Physics Check

Talk about it

  1. Smoke detectors contain a tiny amount of an alpha emitter. Why is that safe to have on the ceiling but not to swallow?
  2. Carbon dating works for things up to about 50 000 years old. Why wouldn't it work for a dinosaur bone?
  3. Fusion fuel is easy to find in seawater, yet fusion power plants don't exist yet. What makes fusion so hard?
  4. Why do you think it took a 27 km machine to find the Higgs boson?

Sources

  1. OpenStax, College Physics 2e, Chapter 31 "Radioactivity and Nuclear Physics," Chapter 32 "Applications of Nuclear Physics" and Chapter 33 "Particle Physics".
  2. CERN, "The Standard Model" and "The Large Hadron Collider".
  3. Lawrence Livermore National Laboratory, "Achieving Fusion Ignition".
  4. Wikipedia, "Nuclear binding energy," "Half-life," "Nuclear fission" and "Chicago Pile-1."

Credits: all diagrams on this page, including the nuclei, the binding energy curve, the Standard Model chart and the share image, are original SVG made for Jugami.