IB Physics SL Topic 5 — The Atomic & Nuclear World Paper 1 & 2 same Z, different A ~7 min read

Isotopes & Decay

Every carbon atom in the universe has exactly 6 protons — that’s what makes it carbon. But it can carry a different number of neutrons, giving heavier or lighter versions of the same element. Some of those versions are perfectly happy; others are lopsided and unstable, and they fix themselves by firing out radiation at moments nobody can predict. This page is where atomic structure meets radioactivity.

📘 What you need to know

What Is an Isotope?

Picture the nucleus as a bag of protons and neutrons. The number of protons is the atom’s identity badge: 1 proton is always hydrogen, 6 is always carbon, 92 is always uranium. Change the protons and you’ve changed the element entirely. But the number of neutrons is more flexible — you can add or remove a few without changing which element it is. Those different-neutron versions are called isotopes.

The classic example is hydrogen. Ordinary hydrogen has 1 proton and no neutrons. Add one neutron and you get deuterium; add two and you get tritium. All three are hydrogen (still just 1 proton), but they get steadily heavier.

PROTIUM 1H 1p, 0n DEUTERIUM 2H 1p, 1n TRITIUM 3H 1p, 2nproton neutron
All three are hydrogen because each has one proton (fixed Z). They differ only in neutron count, so the nucleon number A climbs from 1 to 3.

We write a nucleus using the notation AZX, where A is the nucleon (mass) number on top and Z is the proton number below. For isotopes of the same element, the bottom number (Z) stays put while the top number (A) changes.

same element
→ same Z, different A →
isotopes

Isotopic Data & Relative Atomic Mass

Most elements turn up in nature as a mixture of isotopes, in fixed proportions. The percentage of each is called isotopic data (or relative abundance), and it’s measured with a mass spectrometer. The relative atomic mass you see on the periodic table isn’t the mass of any single atom — it’s the weighted average across all the naturally occurring isotopes, taking their abundances into account.

To find it, multiply each isotope’s mass by its fractional abundance and add the results together:

Relative atomic mass Ar = Σ (isotope mass × fractional abundance)

🧭 Finding the relative atomic mass

  1. List each isotope with its mass number and its % abundance
  2. Turn percentages into fractions — divide each by 100 (they should add to 1)
  3. Multiply each isotope’s mass by its fraction
  4. Add all the products together — that’s the relative atomic mass
  5. Sanity-check: the answer must sit between the lightest and heaviest isotope, closer to the most abundant one

When a Nucleus Becomes Unstable

Not every isotope is content. If a nucleus has an imbalance of protons and neutrons — too many of one, or simply too many nucleons overall — it becomes unstable. An unstable nucleus can’t stay as it is, so it decays: it spontaneously reshuffles itself into a more stable arrangement, flinging out radiation in the process. This is radioactive decay, defined as the spontaneous disintegration of a nucleus to form a more stable one, emitting an alpha, beta, or gamma particle.

How long this takes varies enormously — some unstable nuclei decay within nanoseconds, others hang around for tens of thousands of years before they go.

unstable nucleus
→ emits radiation →
more stable nucleus

Spontaneous and Random

Radioactive decay has two defining features, and examiners love to test that you know both precisely.

Spontaneous means the decay can’t be influenced by outside conditions. Heating the sample, squeezing it, freezing it, or reacting it chemically makes no difference at all — the nucleus decays entirely on its own schedule. This is very different from ordinary chemical reactions, which speed up when you heat them.

Random means you can’t predict exactly when any particular nucleus will decay. Every unstable nucleus has the same fixed probability of decaying in the next second, but which one actually goes, and when, is down to chance. The upside: with a huge number of nuclei, the average behaviour of the whole group becomes very predictable, even though each individual is unpredictable.

count rate time jagged = random decays smooth average trend
A Geiger–Müller tube’s count rate jumps about unpredictably from moment to moment (teal) even though the overall trend (dashed grey) falls smoothly. The jaggedness is direct evidence that decay is random.
Quick recap: isotopes share the same proton number Z but differ in nucleon number A; isotopic abundances give the periodic table’s relative atomic mass; and unstable nuclei decay spontaneously (no outside influence) and randomly (unpredictable timing) to become more stable.
WE 1

A sample of an element contains just two isotopes: one of mass number 63 (abundance 69.0%) and one of mass number 65 (abundance 31.0%). Calculate the relative atomic mass of the sample to 2 decimal places.

Set up the weighted average turn each % into a fraction: 0.690 and 0.310 (they add to 1) Ar = (63 × 0.690) + (65 × 0.310) Ar = 43.47 + 20.15 = 63.62 Ar = 63.62 The answer sits between 63 and 65, nearer 63 because that isotope is more abundant — a good sanity check.
WE 2

Two nuclei have the following details: nucleus 1 has nucleon number 40 and 22 neutrons; nucleus 2 has nucleon number 38 and 20 neutrons. State, with reasoning, whether they are isotopes of the same element.

Find the proton number of each (protons = nucleons − neutrons) nucleus 1: Z = 40 − 22 = 18 nucleus 2: Z = 38 − 20 = 18 Compare both have Z = 18, so both are the same element their nucleon numbers differ (40 vs 38), so their neutron counts differ Yes — they are isotopes of the same element The test is always the proton number: same Z means same element; different A means different isotope.

💡 Top tips

⚠ Common mistakes

Up next: Alpha, Beta & Gamma Decay. Now that you know why nuclei become unstable, we’ll look at the three things they actually throw out — what each particle is, how it changes the nucleus, and how far each one can travel.

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