In 1896, a French scientist named Henri Becquerel was studying uranium salts. He placed them in a drawer with some photographic plates, expecting nothing to happen. When he developed the plates, he was astonished to find that they had been exposed — even though they had never seen sunlight. Something invisible was coming from the uranium. Something that could penetrate solid matter. Marie Curie, who later studied this phenomenon with her husband Pierre, called it radioactivity.
Radioactivity is the spontaneous emission of particles or radiation from unstable atomic nuclei. It is a natural process that has been happening since the birth of the universe. It warms the Earth's interior, powers the stars, and has shaped the evolution of our planet. It is also a powerful tool — used in medicine to diagnose and treat cancer, in industry to test materials, and in archaeology to date ancient objects. But it is also dangerous, and understanding it is essential for using it safely. In this chapter, we are going to explore the fascinating and sometimes frightening world of radioactivity. Let us begin.
I once asked a class, "Is radioactivity natural or man-made?" Most students said man-made. They were surprised to learn that radioactivity is completely natural. It has been part of the Earth since before life existed. The potassium in your body, the carbon in the air, and the rocks beneath your feet all contain radioactive atoms. You are slightly radioactive right now. That is not a reason to be afraid — it is a reason to understand.By the end of this chapter, you should be able to:
Before we can understand radioactivity, we must understand the structure of the atom. An atom consists of a small, dense nucleus surrounded by a cloud of electrons. The nucleus contains protons and neutrons.
| Particle | Charge | Mass (u) | Location |
|---|---|---|---|
| Proton | +1 | 1.007 | Nucleus |
| Neutron | 0 | 1.009 | Nucleus |
| Electron | −1 | 1/1836 | Orbiting nucleus |
Atomic number (Z): The number of protons in the nucleus. It determines the element.
Mass number (A): The total number of protons and neutrons in the nucleus.
Mass number: A = Z + N
A = mass number, Z = atomic number (protons), N = number of neutrons
Notation: AZX, where X is the element symbol
Think of the nucleus as a tiny, dense ball at the centre of the atom. It contains almost all the mass of the atom but takes up only a tiny fraction of its volume. If the atom were a football stadium, the nucleus would be a pea at the centre. The rest is empty space filled by the electron cloud.
The nucleus is a remarkable thing. It contains positively charged protons packed closely together. According to Coulomb's Law, they should repel each other violently. Why do they not fly apart? Because of the strong nuclear force — an incredibly powerful force that acts over very short distances and holds the nucleus together. Understanding this force is key to understanding radioactivity.Isotopes are atoms of the same element that have the same number of protons but different numbers of neutrons. In other words, they have the same atomic number but different mass numbers.
Examples of isotopes:
| Isotope | Protons | Neutrons | Mass Number | Stability |
|---|---|---|---|---|
| Carbon-12 | 6 | 6 | 12 | Stable |
| Carbon-13 | 6 | 7 | 13 | Stable |
| Carbon-14 | 6 | 8 | 14 | Radioactive |
| Uranium-235 | 92 | 143 | 235 | Radioactive |
| Uranium-238 | 92 | 146 | 238 | Radioactive |
Most elements have several isotopes. Some are stable; others are radioactive. The stability of a nucleus depends on the ratio of protons to neutrons.
Think of isotopes as siblings. They are from the same family (same element) but have different personalities (different stability). Some are calm and stable; others are restless and radioactive.
Carbon-14 is one of the most famous isotopes. It is radioactive and is used to date ancient objects. All living things absorb carbon-14 while they are alive. When they die, the carbon-14 begins to decay. By measuring how much is left, we can determine how long ago the organism died. This is radiocarbon dating, and it has revolutionised archaeology.Radioactivity is the spontaneous emission of particles or radiation from an unstable atomic nucleus. It occurs when the nucleus has too much energy or an unstable ratio of protons to neutrons.
Key points about radioactivity:
Think of an unstable nucleus as a tower of blocks that is just barely balanced. At any moment, it might collapse. You cannot predict exactly when, but you can describe the probability. That is radioactivity — random, spontaneous, and transformative.
| Property | Description |
|---|---|
| Random | Cannot predict when a specific nucleus will decay |
| Spontaneous | Does not need external energy |
| Unaffected by external conditions | Temperature, pressure, and chemistry do not affect it |
| Transformative | Changes one element into another |
| Energy-releasing | Releases radiation |
There are three main types of radiation emitted by radioactive nuclei: alpha (α), beta (β), and gamma (γ).
| Type | Nature | Charge | Mass | Symbol |
|---|---|---|---|---|
| Alpha (α) | Helium nucleus (2 protons + 2 neutrons) | +2 | 4 u | 42He |
| Beta (β) | Fast-moving electron | −1 | 1/1836 u | 0−1e |
| Gamma (γ) | High-energy electromagnetic wave | 0 | 0 | γ |
Alpha decay: The nucleus emits an alpha particle, reducing its mass number by 4 and its atomic number by 2.
Alpha decay: AZX → A−4Z−2Y + 42He
Beta decay: The nucleus emits a beta particle (electron), increasing its atomic number by 1. A neutron is converted into a proton and an electron.
Beta decay: AZX → AZ+1Y + 0−1e + antineutrino
Gamma decay: The nucleus releases excess energy as gamma radiation without changing its mass number or atomic number.
Gamma decay: AZX* → AZX + γ
(The asterisk indicates an excited state.)
| Property | Alpha (α) | Beta (β) | Gamma (γ) |
|---|---|---|---|
| Nature | Helium nucleus | Electron | Electromagnetic wave |
| Charge | +2 | −1 | 0 |
| Mass | 4 u | 1/1836 u | 0 |
| Speed | ~5% of c | Up to 99% of c | c (speed of light) |
| Penetrating power | Low (stopped by paper) | Moderate (stopped by aluminium) | High (stopped by lead) |
| Ionising power | High | Moderate | Low |
| Deflected by electric/magnetic fields? | Yes | Yes | No |
| Range in air | ~5 cm | ~1 m | Very far |
Key relationships:
Think of it this way: alpha particles are big and slow. They collide with many atoms and lose their energy quickly, so they are highly ionising but do not penetrate far. Gamma rays are small and fast. They pass through most materials without interacting, so they are highly penetrating but weakly ionising.
The inverse relationship between ionising power and penetrating power is one of the most important ideas in radioactivity. Alpha radiation is dangerous if inhaled or ingested because it deposits all its energy in a small area of tissue. Gamma radiation is dangerous because it can pass through the body and damage cells deep inside. Each type of radiation has its own dangers and its own uses.When a nucleus decays, the total mass number and total atomic number must be conserved. We can write equations to represent these changes.
Example 1: Alpha decay of uranium-238
23892U → 23490Th + 42He
Check: Mass number 238 = 234 + 4. Atomic number 92 = 90 + 2.
Example 2: Beta decay of carbon-14
146C → 147N + 0−1e
Check: Mass number 14 = 14 + 0. Atomic number 6 = 7 − 1.
Example 3: Gamma decay of an excited nucleus
6027Co* → 6027Co + γ
Check: Mass number and atomic number unchanged.
| Decay Type | Change in Mass Number | Change in Atomic Number |
|---|---|---|
| Alpha | −4 | −2 |
| Beta | 0 | +1 |
| Gamma | 0 | 0 |
The half-life of a radioactive substance is the time taken for half of the radioactive nuclei in a sample to decay. It is a measure of how quickly a substance decays.
Half-life: N = N₀ × (1/2)n
N = remaining nuclei, N₀ = initial nuclei, n = number of half-lives
Number of half-lives: n = t / T1/2
t = total time, T1/2 = half-life
Examples of half-lives:
| Isotope | Half-Life | Use |
|---|---|---|
| Uranium-238 | 4.5 billion years | Dating rocks |
| Carbon-14 | 5 730 years | Dating organic material |
| Radon-222 | 3.8 days | Medical treatment |
| Iodine-131 | 8 days | Thyroid treatment |
| Technetium-99m | 6 hours | Medical imaging |
| Francium-223 | 22 minutes | Research |
Decay curve: The number of remaining nuclei decreases exponentially with time. The graph is a curve that approaches zero but never quite reaches it.
| Number of Half-Lives | Fraction Remaining | Percentage Remaining |
|---|---|---|
| 0 | 1 | 100% |
| 1 | 1/2 | 50% |
| 2 | 1/4 | 25% |
| 3 | 1/8 | 12.5% |
| 4 | 1/16 | 6.25% |
| 5 | 1/32 | 3.125% |
Radiation is invisible, but it can be detected using various instruments.
| Detector | How It Works |
|---|---|
| Geiger-Müller (GM) tube | Radiation ionises gas in the tube, causing a pulse of current |
| Cloud chamber | Radiation leaves a trail of ions in supersaturated vapour, forming a visible track |
| Spark chamber | Radiation causes sparks between electrodes, showing paths |
| Photographic film | Radiation darkens the film |
| Scintillation counter | Radiation causes certain materials to emit light |
| Dosimeter | Measures cumulative radiation dose |
Geiger-Müller tube: This is the most common detector. It consists of a tube filled with a gas at low pressure. When radiation enters the tube, it ionises the gas, creating a pulse of current that is counted by an electronic circuit. The rate of pulses indicates the intensity of the radiation.
Think of a GM tube as a microphone for radiation. It does not tell you what type of radiation it is (unless you use filters), but it tells you how much radiation is present. It is the workhorse of radiation detection.
The cloud chamber is one of the most beautiful detectors. It allows you to actually see the tracks of alpha and beta particles as they pass through. Alpha particles leave thick, straight tracks. Beta particles leave thin, wavy tracks. It is like watching subatomic particles dance. Every physics laboratory should have one.Radiation can damage living cells by ionising atoms and molecules in the body. This can lead to cell death, mutations, and cancer.
Biological effects of radiation:
Units of radiation:
| Unit | Measures | Definition |
|---|---|---|
| Becquerel (Bq) | Activity | 1 decay per second |
| Gray (Gy) | Absorbed dose | 1 joule per kilogram |
| Sievert (Sv) | Equivalent dose | Absorbed dose × quality factor |
Safety precautions:
| Precaution | Purpose |
|---|---|
| Time | Reduce total exposure |
| Distance | Reduce intensity (inverse square law) |
| Shielding | Absorb radiation |
| Dosimeter | Monitor exposure |
Nuclear fission is the splitting of a heavy nucleus into two lighter nuclei, releasing a large amount of energy. It is the process that powers nuclear reactors and nuclear weapons.
How fission works:
Fission of uranium-235:
23592U + 10n → 14156Ba + 9236Kr + 310n + energy
Chain reaction: The neutrons released in fission can trigger further fission events, leading to a self-sustaining chain reaction. This is the basis of nuclear reactors and nuclear weapons.
Controlled vs uncontrolled chain reactions:
| Feature | Controlled Fission | Uncontrolled Fission |
|---|---|---|
| Rate | Regulated | Exponential |
| Use | Nuclear power | Nuclear weapons |
| Control | Control rods | No control |
Nuclear fusion is the joining of two light nuclei to form a heavier nucleus, releasing a large amount of energy. It is the process that powers the Sun and other stars.
Fusion of hydrogen isotopes:
21H + 31H → 42He + 10n + energy
Conditions for fusion:
These conditions are needed to overcome the electrostatic repulsion between positively charged nuclei and bring them close enough for the strong nuclear force to take over.
| Feature | Fission | Fusion |
|---|---|---|
| Process | Splitting heavy nuclei | Joining light nuclei |
| Fuel | Uranium, plutonium | Hydrogen isotopes |
| Energy released | Large | Even larger per unit mass |
| Radioactive waste | Significant | Minimal |
| Conditions | Moderate | Extreme |
| Status | Commercial | Experimental |
Think of fission as breaking a large log into smaller pieces. Think of fusion as gluing small pieces together to make a larger log. Both release energy, but fusion releases more per unit mass.
Fusion is the holy grail of energy. It promises abundant, clean energy with minimal radioactive waste. But achieving it on Earth is incredibly difficult. We need to create conditions similar to the core of the Sun. Scientists have been working on this for decades, and progress is being made. It may be the energy source of the future.| Field | Application | How It Works |
|---|---|---|
| Medicine | Cancer treatment (radiotherapy) | Gamma rays destroy cancer cells |
| Medicine | Medical imaging | Radioactive tracers emit gamma rays detected by cameras |
| Medicine | Sterilisation | Gamma rays kill bacteria on equipment |
| Industry | Thickness measurement | Radiation absorption depends on material thickness |
| Industry | Leak detection | Radioactive tracers detect leaks in pipes |
| Archaeology | Carbon dating | Measures carbon-14 decay to date organic materials |
| Geology | Rock dating | Measures uranium decay to date rocks |
| Agriculture | Food preservation | Gamma rays kill bacteria and pests |
| Smoke detectors | Detect smoke | Americium-241 ionises air; smoke interrupts current |
Mass number: A = Z + N
Alpha decay: AZX → A−4Z−2Y + 42He
Beta decay: AZX → AZ+1Y + 0−1e + antineutrino
Gamma decay: AZX* → AZX + γ
Half-life: N = N₀ × (1/2)n
Number of half-lives: n = t / T1/2
1 eV = 1.6 × 10⁻¹⁹ J
1 u = 1.66 × 10⁻²⁷ kg
Question: Radium-226 undergoes alpha decay. Write the balanced nuclear equation.
Answer:
Alpha decay: mass number decreases by 4, atomic number decreases by 2.
22688Ra → 22286Rn + 42He
Answer: Radium-226 decays into radon-222 and an alpha particle.
Units check: mass numbers balance (226 = 222 + 4) and atomic numbers balance (88 = 86 + 2). Always check both.Question: A nucleus of lead-214 undergoes beta decay. Write the balanced nuclear equation.
Answer:
Beta decay: mass number unchanged, atomic number increases by 1.
21482Pb → 21483Bi + 0−1e
Answer: Lead-214 decays into bismuth-214 and a beta particle.
Units check: mass numbers balance (214 = 214 + 0) and atomic numbers balance (82 = 83 − 1). The beta particle has atomic number −1 because it is an electron.Question: A radioactive sample has a half-life of 8 days. What fraction of the original sample remains after 32 days?
Answer:
Number of half-lives: n = t / T1/2 = 32 / 8 = 4
Fraction remaining: (1/2)4 = 1/16
Answer: 1/16 of the original sample remains.
Units check: the answer is a fraction. After 4 half-lives, 1/16 remains. This is the same as 6.25%. Half-life calculations are straightforward once you know the number of half-lives.Question: A sample of wood from an ancient tool has 25% of its original carbon-14 content. The half-life of carbon-14 is 5 730 years. Calculate the age of the tool.
Answer:
25% = 1/4 = (1/2)2, so n = 2 half-lives.
Age = n × T1/2 = 2 × 5 730 = 11 460 years
Answer: The tool is approximately 11 460 years old.
Units check: the answer is in years. This is a classic carbon dating problem. By measuring the remaining carbon-14, we can determine how many half-lives have passed, and hence the age of the sample.Question: Uranium-238 decays by alpha emission to thorium-234. Thorium-234 then decays by beta emission. Write the equation for the second decay.
Answer:
Thorium-234 (Z = 90) undergoes beta decay, so atomic number increases by 1 to 91 (protactinium), mass number stays 234.
23490Th → 23491Pa + 0−1e
Answer: Thorium-234 decays into protactinium-234 and a beta particle.
Units check: mass numbers balance (234 = 234 + 0) and atomic numbers balance (90 = 91 − 1). This is part of the uranium decay series, which eventually ends in stable lead-206.Graphs are essential for understanding radioactive decay.
Decay curve: If you plot the number of remaining nuclei on the vertical axis and time on the horizontal axis, you get an exponential decay curve.
Logarithmic graph: If you plot the natural logarithm of the count on the vertical axis and time on the horizontal axis, you get a straight line with a negative gradient. The gradient is related to the decay constant (λ).
Activity vs time: The activity (number of decays per second) also decreases exponentially with the same half-life.
These graphs help us visualise the random but predictable nature of radioactive decay. They turn statistical processes into pictures.
Think of a graph as a map of a relationship. The shape tells you how one quantity changes with another.
Note: Direct experiments with radioactive sources require strict safety precautions and are often performed as simulations or with very low-activity sources.
Apparatus: A Geiger-Müller tube, a radioactive source (e.g., protactinium-234 or a simulated source), a scaler/timer, and a computer for data logging.
Method:
Calculation: If the initial count rate is 800 counts/min and it drops to 400 counts/min after 5 minutes, the half-life is 5 minutes.
Precautions:
Likely source of error: Background radiation can affect the count rate. Always measure and subtract the background count.
This experiment is a beautiful way to see radioactive decay in action. The count rate halves at regular intervals, just as the theory predicts. It is a direct demonstration of the probabilistic nature of the universe. Once you have done it, you will understand half-life in your bones.Radioactivity is the spontaneous emission of particles or radiation from an unstable atomic nucleus.
Alpha (α), beta (β), and gamma (γ).
Gamma > beta > alpha. Gamma is the most penetrating; alpha is the least.
Half-life is the time taken for half of the radioactive nuclei in a sample to decay.
23892U → 23490Th + 42He.
(1/2)3 = 1/8 = 12.5%.
Fission is the splitting of a heavy nucleus; fusion is the joining of light nuclei. Both release energy.
Limit exposure time; increase distance; use lead shielding; use tongs; wear a dosimeter.
(a) Define radioactivity and describe the three types of radiation. [5]
(b) Compare the penetrating power and ionising power of alpha, beta, and gamma radiation. [4]
(c) Explain why alpha radiation is more dangerous if inhaled than if it is outside the body. [3]
(a) Radioactivity is the spontaneous emission of particles or radiation from unstable nuclei. Alpha: helium nucleus. Beta: electron. Gamma: electromagnetic wave. (5 marks.)
(b) Penetrating: gamma > beta > alpha. Ionising: alpha > beta > gamma. (4 marks.)
(c) Alpha particles are highly ionising and deposit all their energy in a small area of tissue. Outside the body, they are stopped by the skin. Inside the body, they can damage sensitive cells. (3 marks.)
(a) Define half-life. [2]
(b) A radioactive isotope has a half-life of 6 hours. A sample initially has a count rate of 1 200 counts/min. Calculate the count rate after 24 hours. [4]
(c) Explain how carbon dating is used to determine the age of ancient objects. [4]
(a) Half-life is the time for half the radioactive nuclei in a sample to decay. (2 marks.)
(b) n = 24 / 6 = 4 half-lives. Count rate = 1 200 × (1/2)4 = 1 200 / 16 = 75 counts/min. (4 marks.)
(c) Living things absorb carbon-14. When they die, carbon-14 decays with a half-life of 5 730 years. By measuring the remaining carbon-14, we can determine how many half-lives have passed and hence the age. (4 marks.)
(a) Distinguish between nuclear fission and nuclear fusion. [4]
(b) Describe how a controlled chain reaction is maintained in a nuclear reactor. [4]
(c) State two uses of radioactivity in medicine. [2]
(a) Fission: splitting heavy nuclei. Fusion: joining light nuclei. Fission produces radioactive waste; fusion produces minimal waste. Fusion requires extreme conditions. (4 marks.)
(b) Control rods absorb neutrons to regulate the rate of fission. The moderator slows neutrons to make them more effective. The chain reaction is kept at a steady rate. (4 marks.)
(c) Cancer treatment (radiotherapy); medical imaging (tracers). (2 marks.)
Explain why the decay of a radioactive nucleus is a random process, yet the decay of a large sample is predictable.
The decay of a single nucleus is random — we cannot predict when it will decay. However, when there are billions of nuclei in a sample, the statistical behaviour becomes predictable. The half-life is a statistical property that emerges from the random behaviour of many individual nuclei. This is similar to how the behaviour of a single gas molecule is random, but the pressure of a gas is predictable.
Explain why nuclear fusion is considered the ideal energy source of the future, and why it is so difficult to achieve.
Fusion releases enormous energy with minimal radioactive waste and abundant fuel (hydrogen isotopes). However, it requires extremely high temperatures and pressures to overcome the electrostatic repulsion between nuclei. Creating and containing these conditions on Earth is extremely difficult and has not yet been achieved on a commercial scale.
A student says, "Radioactivity is dangerous, so we should ban all use of radioactive materials." Discuss this statement.
Radioactivity can be dangerous, but it also has many life-saving uses. It is used to treat cancer, diagnose diseases, generate low-carbon electricity, and date archaeological objects. Banning all use would deprive society of these benefits. The key is to use radioactivity safely, with proper precautions and regulations. The risks must be balanced against the benefits.
Radioactivity is the invisible energy released by unstable atoms — a force of nature that can heal or harm, power our cities or destroy them, and in understanding it, we learn to use it wisely for the benefit of all.