From atoms to radioactivity -- understand the tiny world that powers the Sun, nuclear reactors, and even the smoke detector in your house.
5.1 The Nuclear Model of the Atom▼
Everything around you -- your phone, your chai, even you -- is made of atoms. In this section, we will look inside the atom and discover what it is made of, how we know, and what holds it all together. Think of this as zooming in with an incredibly powerful microscope!
An atom is the smallest particle of an element that still has the properties of that element. Every atom has two main parts:
A tiny, dense, positive nucleus at the centre
Negative electrons orbiting (moving around) the nucleus
The nucleus is incredibly small compared to the whole atom. Imagine a cricket stadium -- like the M. Chinnaswamy Stadium in Bengaluru. If the atom were the size of that stadium, the nucleus would be a small cricket ball sitting right at the centre of the pitch. The electrons would be like tiny flies buzzing around way up in the stands. Most of the atom is just empty space!
Here are some important facts about atom structure:
The nucleus is about 10,000 times smaller than the whole atom.
Despite being tiny, the nucleus contains almost all the mass of the atom (more than 99.9%).
Electrons are held in orbit by the electrostatic attraction between the positive nucleus and the negative electrons.
In a neutral atom, the number of electrons equals the number of protons, so the positive and negative charges balance out exactly.
⚠ Exam Tip
The nucleus is positive because it contains protons (which are positive). The electrons are negative. Opposite charges attract, which is why the electrons stay in orbit around the nucleus instead of flying away. Think of it like a planet orbiting the Sun -- but here it is electrical force, not gravity, that does the job.
Size and Scale of the Atom
To truly appreciate how small the nucleus is compared to the atom, consider these comparisons:
An atom is about 10-10 metres across (0.0000000001 m). That is one ten-billionth of a metre!
The nucleus is about 10-15 metres across -- about 100,000 times smaller than the atom itself.
If the atom were the size of the M. Chinnaswamy cricket stadium in Bengaluru (about 150 metres across), the nucleus would be about 1.5 millimetres -- smaller than a grain of rice!
If you removed all the empty space from the atoms in every human on Earth, all 8 billion people would fit into a space the size of a sugar cube. That is how much empty space atoms contain!
Despite being so tiny, the nucleus contains more than 99.9% of the atom's total mass. All those heavy protons and neutrons are packed into an incredibly small space, making the nucleus extremely dense. If you could pack matter as densely as a nucleus everywhere, a teaspoon of that material would weigh about 6 billion tonnes -- roughly the same as Mount Everest!
The Electric Force in Atoms
What keeps the atom together? The electrostatic force (or Coulomb force) between the positive nucleus and the negative electrons. This is the same force that makes a balloon stick to a wall after you rub it on your hair -- opposite charges attract each other.
This force also explains why:
Electrons stay in orbit around the nucleus (they are attracted to the positive nucleus)
The nucleus is hard to break apart (protons are held together by an even stronger force called the strong nuclear force)
Alpha particles are deflected in the scattering experiment (the positive alpha particle is repelled by the positive nucleus)
Fusion is difficult (both nuclei are positive and repel each other -- you need extreme temperatures to overcome this repulsion)
Structure of an atom showing the nucleus (protons and neutrons) with electrons orbiting around it
What Are Ions?
A normal atom is electrically neutral -- it has the same number of protons (+) as electrons (-), so the charges cancel out. But sometimes atoms gain or lose electrons:
Positive ion: An atom that has lost one or more electrons. It now has more protons than electrons, so the overall charge is positive. Example: Na+ (sodium ion -- lost 1 electron).
Negative ion: An atom that has gained one or more electrons. It now has more electrons than protons, so the overall charge is negative. Example: Cl- (chloride ion -- gained 1 electron).
Let's see this with a real example. A magnesium atom has 12 protons and 12 electrons. When it forms an ion (Mg2+), it loses 2 electrons. Now it has 12 protons but only 10 electrons, so the overall charge is +2.
Type of Ion
What Happens
Result
Example
Positive ion (cation)
Atom loses electrons
More protons than electrons
Na → Na+ (lost 1 electron)
Negative ion (anion)
Atom gains electrons
More electrons than protons
O → O2- (gained 2 electrons)
⚠ Exam Tip
When an atom becomes an ion, only electrons are added or removed -- never protons or neutrons! The nucleus does not change. If you see an exam question asking "what happens when an atom becomes a positive ion?", the answer is always "it loses electrons." Never say "it gained protons" -- protons are locked inside the nucleus.
💡 Memory Trick
Positive ions are POSITIVE because they LOST something negative. Think of it this way: if someone takes away your worries (negative things), you become a happier (more positive) person! Similarly, if someone gives you more problems (negative), you become a more negative person (negative ion).
Worked ExampleA calcium atom (Ca) has 20 protons. A calcium ion has a charge of +2. How many electrons does the Ca2+ ion have?
Step 1: Neutral Atom
A neutral calcium atom has 20 protons and 20 electrons (charges balance).
Step 2: Apply the Charge
A charge of +2 means it lost 2 electrons. So electrons = 20 - 2 = 18 electrons.
Step 3: Verify
20 protons (+20) and 18 electrons (-18) gives net charge = +2. Correct!
The Ca2+ ion has 18 electrons. The nucleus still has 20 protons (unchanged).
Before this experiment (around 1909-1911), scientists thought atoms were like a pudding -- positive charge spread evenly throughout, with electrons stuck in it like raisins in a gulab jamun. This was called the "plum pudding model."
Then, Ernest Rutherford (along with Hans Geiger and Ernest Marsden) did a brilliant experiment. They fired tiny, fast-moving alpha particles (which are positively charged) at a very thin gold foil and watched what happened:
Alpha particles fired at gold foil: most pass through, some deflect, very few bounce back
What They Observed:
Most alpha particles went straight through the gold foil without any deflection.
Some alpha particles were deflected (bent off course) at various angles.
Very few alpha particles bounced straight back towards the source (about 1 in 8,000).
What This Told Us:
Observation
What It Proves
Most particles passed straight through
The atom is mostly empty space
Some particles were deflected
The nucleus is positively charged (it repels the positive alpha particles)
Very few bounced straight back
The nucleus is very small and very dense (contains most of the atom's mass)
⚠ Exam Tip
This experiment gives THREE pieces of evidence. The exam loves asking about all three. Remember: Empty space, positive charge, small and dense. Don't just say "it proved the nucleus exists" -- you need to explain WHAT about the nucleus was proven.
💡 Memory Trick -- The Three Conclusions
Remember E-P-S for the three conclusions of alpha scattering:
Empty space (most particles passed through)
Positive nucleus (some particles were deflected -- repelled by a positive charge)
Small and dense nucleus (very few bounced back -- must be concentrated mass in a tiny area)
Why Was Gold Used?
Gold was chosen for three important reasons:
Gold is very malleable (it can be hammered incredibly thin) -- the foil was only a few atoms thick.
Gold has a large nucleus (79 protons) which gives a strong positive charge for repelling alpha particles.
A thin foil was needed so that alpha particles would only encounter one or two gold nuclei, making the results easier to interpret.
Before and After Rutherford
Before the experiment: Scientists used the "plum pudding model" (proposed by J.J. Thomson in 1904). In this model, the atom was a uniform sphere of positive charge with electrons embedded throughout -- like raisins in a gulab jamun or seeds in a watermelon. If this model were correct, alpha particles should have passed through with only very slight deflections (the positive charge would be too spread out to cause a big deflection).
After the experiment: Rutherford proposed the "nuclear model" (1911) -- a tiny, dense, positive nucleus at the centre with electrons orbiting around it in mostly empty space. The fact that some alpha particles bounced straight back could ONLY be explained by a concentrated mass of positive charge -- not a spread-out one. This is the model we still use (with some modifications) today.
The plum pudding model was replaced by the nuclear model after Rutherford's alpha scattering experiment
Worked ExampleIn an alpha scattering experiment, alpha particles are fired at a thin gold foil. Explain why: (a) most particles pass straight through, (b) some are deflected at large angles, and (c) very few bounce straight back.
(a) Most Pass Straight Through
The atom is mostly empty space. The nucleus is incredibly small compared to the overall size of the atom. Most alpha particles travel through the atom without getting close to a nucleus, so they are not deflected.
(b) Some Deflected at Large Angles
Alpha particles that pass close to a nucleus experience a strong electrostatic repulsion because both the alpha particle (charge +2) and the nucleus (positive charge) are positively charged. Like charges repel, so the alpha particle's path is bent.
(c) Very Few Bounce Back
A very small number of alpha particles make a nearly head-on collision with the nucleus. The nucleus is very small but very dense (it contains most of the atom's mass). The strong electrostatic repulsion from the concentrated positive charge in such a small space is enough to send the alpha particle back the way it came.
Three conclusions: (1) atoms are mostly empty space, (2) the nucleus has a positive charge, (3) the nucleus is very small and very dense, containing most of the atom's mass.
⚠ How to Structure Alpha Scattering Answers for Full Marks
Alpha scattering questions appear in almost every IGCSE Physics paper. Here is exactly how to structure your answer for maximum marks:
If the question asks "Describe the experiment":
Alpha particles were fired at a very thin gold foil
A detector (movable) was placed around the foil to detect where the alpha particles went
The experiment was done in a vacuum (so alpha particles were not absorbed by air)
If the question asks "State the observations and explain":
Use this three-part structure -- each observation paired with its explanation:
Observation
Explanation
Conclusion
Most alpha particles pass straight through without deflection
The atom is mostly empty space -- there is nothing in the way to deflect them
Atoms are mostly empty space
Some alpha particles are deflected at large angles
They pass close to a concentrated positive charge, and the repulsive electrostatic force pushes them away
The nucleus is positively charged
Very few alpha particles bounce straight back (more than 90 degree deflection)
A nearly head-on collision with something very small and very dense -- nearly all the mass is concentrated in a tiny space
The nucleus is very small and very dense, containing most of the mass
Key phrase to include: "This experiment provided evidence that the atom has a small, dense, positively charged nucleus, surrounded by mostly empty space." Writing this one sentence can earn you marks across multiple parts of the question.
How a sodium atom loses an electron to become a positive ion (Na+)
5.1.2 The Nucleus
What's Inside the Nucleus?
The nucleus contains two types of particles, collectively called nucleons:
Protons -- positively charged
Neutrons -- no charge (neutral)
The Subatomic Particles
Particle
Location
Relative Charge
Relative Mass
Proton
Nucleus
+1
1
Neutron
Nucleus
0
1
Electron
Orbits around nucleus
-1
Negligible (about 1/1836)
💡 Memory Trick
Proton = Positive. Neutron = Neutral. Electron = nEgative. The first letter of each particle matches the first letter of its charge (well, almost -- for electron, think of the "e" in "negative")!
Some important things to remember about these particles:
Protons and neutrons are found inside the nucleus. Together, they are called nucleons.
Electrons are found in orbits (or shells) around the nucleus.
Protons and neutrons have roughly the same mass (relative mass = 1 each).
An electron is about 1/1836 times the mass of a proton -- so small that we call it "negligible" (meaning we can usually ignore it when calculating atomic mass).
The number of protons defines what element an atom is. Change the protons, and you change the element.
The number of electrons can change (making ions), and the number of neutrons can change (making isotopes) -- but as long as the number of protons stays the same, it is still the same element.
⚠ Exam Tip
The exam may ask: "Why is the mass of the atom concentrated in the nucleus?" The answer is: because protons and neutrons (which have nearly all the mass) are in the nucleus, while electrons (which have negligible mass) are outside the nucleus. Even though electrons occupy most of the atom's volume, they contribute almost nothing to its mass.
Proton Number (Z) and Nucleon Number (A)
Proton number (Z) = the number of protons in the nucleus. Also called the atomic number. This defines what element an atom is. All carbon atoms have Z = 6. All oxygen atoms have Z = 8.
Nucleon number (A) = the total number of protons + neutrons in the nucleus. Also called the mass number.
Number of neutrons = A - Z
A = nucleon number (mass number)Z = proton number (atomic number)
Nuclide Notation
Scientists write atoms in a special shorthand that tells you everything about the nucleus at a glance. For example, carbon-12 is written as:
126C
Top number (12) = nucleon number (A) = total protons + neutronsBottom number (6) = proton number (Z) = number of protonsLetter (C) = element symbolNeutrons = 12 - 6 = 6
How to read nuclide notation: the top number is A (nucleon number), the bottom number is Z (proton number)
Worked ExampleAn atom of aluminium has a nucleon number of 27 and a proton number of 13. How many protons, neutrons, and electrons does it have?
Step 1: Protons
Proton number (Z) = 13, so there are 13 protons.
Step 2: Neutrons
Neutrons = A - Z = 27 - 13 = 14 neutrons.
Step 3: Electrons
In a neutral atom, electrons = protons = 13 electrons.
Aluminium-27 has 13 protons, 14 neutrons, and 13 electrons.
Worked ExampleWrite the nuclide notation for an atom with 26 protons and 30 neutrons.
Step 1: Identify the Element
26 protons means Z = 26. Looking at the periodic table, element 26 is iron (Fe).
Step 2: Calculate A
A = protons + neutrons = 26 + 30 = 56.
Step 3: Write the Notation
Put A on top, Z on bottom, symbol to the right.
The nuclide notation is: 5626Fe
Worked ExampleGold has a proton number of 79. An atom of gold-197 has what composition? Write the nuclide notation.
Step 1: Identify the Numbers
Proton number Z = 79. The name "gold-197" tells us the nucleon number A = 197.
Gold-197 has 79 protons, 118 neutrons, and 79 electrons. Written as 19779Au. Fun fact: this is the gold used in Rutherford's alpha scattering experiment!
Isotopes
Isotopes are atoms of the same element (same number of protons) but with a different number of neutrons. This means they have the same proton number (Z) but different nucleon numbers (A).
For example, carbon has three common isotopes:
Carbon-12 (126C): 6 protons, 6 neutrons -- the most common
Carbon-13 (136C): 6 protons, 7 neutrons -- stable, found in nature
Carbon-14 (146C): 6 protons, 8 neutrons -- radioactive, used for carbon dating
All three are still carbon (they all have 6 protons), but they have different masses because of the different numbers of neutrons.
Key points about isotopes:
Isotopes have the same chemical properties (because they have the same number of electrons, and chemical reactions depend on electrons).
Isotopes have different physical properties (different masses, different densities, and some may be radioactive while others are stable).
Some isotopes are stable (like carbon-12) and some are unstable/radioactive (like carbon-14, which is used for carbon dating to find the age of ancient objects).
💡 Memory Trick
Isotopes: Same Protons, Different Neutrons. Think of isotopes as siblings in a family -- they have the same family name (same element, same proton number), but different weights (different neutron numbers). Carbon-12 and Carbon-14 are like a thin sibling and a slightly heavier sibling -- same family, different mass!
Worked ExampleAre 3517Cl and 3717Cl isotopes of each other? Explain your answer.
Step 1: Check Proton Numbers
Both have Z = 17, so both are atoms of chlorine (same element).
Step 2: Check Nucleon Numbers
35Cl has A = 35, so neutrons = 35 - 17 = 18. 37Cl has A = 37, so neutrons = 37 - 17 = 20. They have different numbers of neutrons.
Yes, they are isotopes because they have the same number of protons (17) but different numbers of neutrons (18 and 20).
Supplement
Proton Number = Relative Charge on Nucleus
Since each proton carries a charge of +1 and neutrons have no charge, the total positive charge on the nucleus equals the proton number (Z). For example, a carbon nucleus with 6 protons has a relative charge of +6.
Nucleon Number = Relative Mass of Nucleus
Since both protons and neutrons have a relative mass of 1, and electrons have negligible mass, the relative mass of the nucleus (and therefore the atom) approximately equals the nucleon number (A). For carbon-12, the relative mass is approximately 12.
This is an important simplification that makes many calculations easier. In reality, the actual mass of an atom is very slightly different from its nucleon number due to something called the "mass defect" (the missing mass that has been converted to binding energy holding the nucleus together). But for IGCSE, you can always use A as the relative mass.
Worked ExampleAn atom of iron has a proton number of 26 and a nucleon number of 56. (a) What is the relative charge on its nucleus? (b) What is the relative mass of the atom?
(a) Relative Charge on Nucleus
The relative charge on the nucleus equals the proton number. Each proton has charge +1, and neutrons have charge 0. So the relative charge = Z = +26.
(b) Relative Mass
The relative mass of the atom approximately equals the nucleon number. Protons and neutrons each have relative mass 1, electrons have negligible mass. So relative mass = A = 56.
(a) Relative charge on nucleus = +26. (b) Relative mass of atom = 56.
Supplement
Nuclear Fission and Fusion
Nuclear Fission: Splitting the Atom
Nuclear fission is the splitting of a heavy, unstable nucleus into two lighter nuclei, usually with the release of extra neutrons and a large amount of energy.
Think of it like breaking a large laddu into two smaller pieces -- but when this laddu breaks, it releases a huge burst of energy!
A common example is uranium-235 being hit by a neutron:
23592U + 10n → 14156Ba + 9236Kr + 310n + energy
A uranium-235 nucleus absorbs a neutron and splits into barium-141, krypton-92, and 3 neutronsCheck: proton numbers balance: 92 + 0 = 56 + 36 + 0 (both sides = 92)Check: nucleon numbers balance: 235 + 1 = 141 + 92 + 3 (both sides = 236)
Key points about fission:
Fission is used in nuclear power plants to generate electricity.
A neutron is fired at a heavy nucleus (like uranium-235) to trigger the fission.
The fission products are two lighter nuclei + extra neutrons + a large amount of energy.
The released neutrons can hit other uranium nuclei and cause them to split too, creating a chain reaction.
In a nuclear power plant, the chain reaction is controlled using control rods that absorb excess neutrons.
In an uncontrolled chain reaction (like a nuclear weapon), the energy is released all at once in a devastating explosion.
Where does fission happen in India? The Kudankulam Nuclear Power Plant in Tamil Nadu uses nuclear fission to generate electricity. India has 22 nuclear reactors across the country, including facilities at Tarapur (Maharashtra), Kalpakkam (Tamil Nadu), Rawatbhata (Rajasthan), and Kakrapar (Gujarat). The Bhabha Atomic Research Centre (BARC) in Mumbai, named after the great physicist Homi Bhabha (the father of India's nuclear programme), is where India does much of its nuclear research.
Nuclear fission: a heavy nucleus splits into two lighter nuclei, releasing neutrons and energy
Nuclear Fusion: Joining Nuclei Together
Nuclear fusion is the joining of two light nuclei to form a heavier nucleus, with the release of a large amount of energy.
This is what powers the Sun (and every star you see at night)! Two hydrogen nuclei fuse together to eventually form helium, releasing enormous energy. This is why the Sun has been shining for 4.6 billion years and will continue for billions more. India's ISRO Aditya-L1 mission is studying the Sun -- and all that energy comes from fusion!
Key points about fusion:
Fusion requires extremely high temperatures (millions of degrees) because the nuclei are all positively charged and repel each other. Only at extreme temperatures do they move fast enough to overcome this repulsion.
Fusion releases even more energy per nucleon than fission.
Fusion produces less radioactive waste than fission, making it a cleaner energy source.
Scientists have not yet achieved controlled fusion for electricity generation on Earth, though experiments are ongoing (India is part of the ITER project in France).
Fusion is the energy source of all stars, including our Sun.
A simple example:
21H + 31H → 42He + 10n + energy
Deuterium (hydrogen-2) fuses with tritium (hydrogen-3) to form helium-4 and a neutronCheck: proton numbers: 1 + 1 = 2 + 0 (both sides = 2)Check: nucleon numbers: 2 + 3 = 4 + 1 (both sides = 5)
Nuclear fusion: two light nuclei combine to form a heavier nucleus plus energy
⚠ Exam Tip
Balancing nuclear equations: In every nuclear equation, the total of the top numbers (nucleon numbers) on the left must equal the total on the right. Similarly, the total of the bottom numbers (proton numbers) on the left must equal the total on the right. This is how you find unknown particles in the exam.
Worked ExampleIn a fusion reaction inside a star, a carbon-12 nucleus (126C) fuses with a proton (11H). The product is a single nucleus plus a gamma ray. Identify the product nucleus.
Step 1: Write What You Know
126C + 11H → ??X + γ
Step 2: Balance Nucleon Numbers
Left: 12 + 1 = 13. Gamma has A = 0. So the product has A = 13.
Step 3: Balance Proton Numbers
Left: 6 + 1 = 7. Gamma has Z = 0. So the product has Z = 7. Element 7 is nitrogen (N).
126C + 11H → 137N + γ (nitrogen-13 is produced)
Chain Reactions in Fission
When a uranium-235 nucleus undergoes fission, it releases 2 or 3 extra neutrons. Each of these neutrons can potentially hit another uranium-235 nucleus and cause it to split as well, releasing yet more neutrons. This is called a chain reaction.
In a nuclear power plant (like Kudankulam), the chain reaction is controlled. Control rods (made of boron or cadmium) are inserted between the fuel rods to absorb excess neutrons, keeping the reaction at a steady rate.
In a nuclear weapon, the chain reaction is uncontrolled. Each fission triggers multiple new fissions, and the number of reactions grows exponentially in a fraction of a second, releasing devastating energy all at once.
Mass-Energy Relationship (Qualitative)
In both fission and fusion, something remarkable happens: the total mass of the products is slightly less than the total mass of the original nuclei. Where did that mass go? It was converted into energy!
You do NOT need to calculate this -- just know that when mass decreases, energy is released. This is why nuclear reactions release so much more energy than chemical reactions (like burning coal or wood). The energy released from fissioning just 1 kg of uranium is equivalent to burning about 2,500 tonnes of coal!
The key points to remember about mass-energy:
The total mass of the products is slightly less than the total mass of the reactants.
The "missing" mass has been converted into energy.
This happens in BOTH fission and fusion.
You do NOT need to use any formula for this -- just state the qualitative relationship.
⚠ Exam Tip
For IGCSE, you only need to describe fission and fusion qualitatively. You do NOT need to use E = mc² or do any mass-energy calculations. Just say: "the total mass of the products is less than the total mass of the reactants, and the lost mass has been converted into energy."
Worked ExampleIn a fission reaction, uranium-235 absorbs a neutron and splits into xenon-140 and strontium-94. How many neutrons are released? Write the full equation.
Step 1: Write What You Know
23592U + 10n → 14054Xe + 9438Sr + ?10n
Step 2: Balance Nucleon Numbers (A)
Left side: 235 + 1 = 236 Right side so far: 140 + 94 = 234 Missing: 236 - 234 = 2 neutrons needed
Step 3: Check Proton Numbers (Z)
Left: 92 + 0 = 92 Right: 54 + 38 + 0 = 92 (neutrons have Z = 0, so this checks out)
23592U + 10n → 14054Xe + 9438Sr + 210n + energy (2 neutrons are released)
Worked ExampleTwo deuterium nuclei (21H) fuse together. One product is 32He. What is the other product? Write the complete equation.
Step 1: Write What You Know
21H + 21H → 32He + ?
Step 2: Balance Nucleon Numbers (A)
Left: 2 + 2 = 4 Right so far: 3 Missing particle has A = 4 - 3 = 1
Step 3: Balance Proton Numbers (Z)
Left: 1 + 1 = 2 Right so far: 2 Missing particle has Z = 2 - 2 = 0
Step 4: Identify the Particle
A = 1, Z = 0 -- this is a neutron (10n)
21H + 21H → 32He + 10n + energy
💡 Memory Trick -- Fission vs Fusion
Fission sounds like "fish-on" -- imagine a big fish being cut into two smaller fish (splitting!).
Fusion sounds like "fuse-on" -- imagine fusing or welding two small pieces of metal together into one (joining!).
Or simply: Fission = Fission = splitting First (the big one breaks). Fusion = Fusion = fusing together (small ones join).
Fission vs Fusion: Key Differences
Feature
Fission
Fusion
What happens?
Heavy nucleus splits into lighter nuclei
Light nuclei join to form a heavier nucleus
Starting nuclei
Heavy (e.g., uranium-235, plutonium-239)
Light (e.g., hydrogen isotopes)
Energy released?
Yes, a large amount
Yes, even more per nucleon
Where it happens
Nuclear power plants (e.g., Kudankulam)
Stars (including our Sun)
Used by humans?
Yes (power plants, Pokhran tests)
Not yet for power (still being researched)
Worked ExampleHydrogen has three isotopes: hydrogen-1 (11H), deuterium (21H), and tritium (31H). How many neutrons does each isotope have? Which one might be radioactive?
All three have Z = 1 (one proton each), so all three are hydrogen. They have different numbers of neutrons (0, 1, and 2), so they are isotopes of hydrogen.
Step 3: Which Is Radioactive?
Tritium (H-3) is radioactive because it has too many neutrons relative to its protons (2 neutrons but only 1 proton makes the nucleus unstable). It undergoes beta decay with a half-life of about 12.3 years. Hydrogen-1 and deuterium are both stable.
H-1 has 0 neutrons, H-2 has 1 neutron, H-3 has 2 neutrons. Tritium (H-3) is radioactive because the neutron-to-proton ratio is too high.
The three isotopes of hydrogen: same number of protons, different numbers of neutrons
Don't Confuse Isotopes and Ions!
Students often mix up isotopes and ions. Here is the clear difference:
Feature
Isotopes
Ions
What changes?
Number of neutrons
Number of electrons
What stays the same?
Number of protons (same element)
Number of protons (same element)
Effect on mass?
Mass changes (different A)
Mass barely changes (electrons have negligible mass)
Effect on charge?
No change in charge (still neutral)
Charge changes (positive or negative)
Example
C-12 and C-14 (different neutrons)
Na and Na+ (different electrons)
⚠ Common Exam Question Types -- Section 5.1
Type 1: "Calculate the number of neutrons/protons/electrons in an atom given its nuclide notation." Use: neutrons = A - Z, electrons = protons (for neutral atom).
Type 2: "Explain how the alpha scattering experiment provides evidence for the nuclear model." Give all three conclusions with the observations that support them.
Type 3: "Write the equation for a fission/fusion reaction and identify the missing particle." Balance A on both sides, balance Z on both sides.
Type 4: "Explain the difference between fission and fusion." Fission = splitting heavy, fusion = joining light. Both release energy because mass decreases.
Type 5: "Explain what isotopes are and give an example." Same proton number, different nucleon number (different neutrons). Same element, different mass.
Key Concepts -- Section 5.1 Summary
Atoms have a positive nucleus (protons + neutrons) with negative electrons orbiting around it.
Ions are atoms that have gained or lost electrons. Positive ions lost electrons; negative ions gained electrons.
The alpha scattering experiment proved: atoms are mostly empty space, the nucleus is small and dense, and the nucleus is positively charged.
Proton number (Z) defines the element. Nucleon number (A) = protons + neutrons.
Neutrons = A - Z
Isotopes are atoms with the same Z but different A (same protons, different neutrons).
Fission: heavy nucleus splits into lighter nuclei + neutrons + energy.
Fusion: light nuclei join to form heavier nucleus + energy.
In both fission and fusion, mass decreases and energy is released.
Final Revision Checklist -- Section 5.1
Before the exam, make sure you can confidently do ALL of these. Tick them off as you revise:
Describe the structure of an atom: positive nucleus with protons and neutrons, negative electrons orbiting outside
State the charge and relative mass of protons (+1, mass 1), neutrons (0, mass 1), and electrons (-1, negligible mass)
Explain how positive ions form (atom loses electrons, more protons than electrons, net positive charge)
Explain how negative ions form (atom gains electrons, more electrons than protons, net negative charge)
Calculate the number of electrons in an ion given its charge and proton number
Describe the alpha scattering experiment: alpha particles fired at thin gold foil
State the three key observations: most pass through, some deflect, very few bounce back
State the three conclusions: mostly empty space, small dense positive nucleus, nucleus contains most of the mass
Explain why this disproved the plum pudding model (diffuse positive charge could not cause large deflections)
Define proton number (Z) as the number of protons in the nucleus
Define nucleon number (A) as the total number of protons + neutrons
Calculate neutrons using the formula: neutrons = A - Z
Read and write nuclide notation (A top-left, Z bottom-left of element symbol)
Define isotopes: atoms of the same element with the same proton number but different nucleon numbers
Distinguish isotopes from ions: isotopes differ in neutrons; ions differ in electrons
Describe nuclear fission: heavy nucleus absorbs neutron and splits into two lighter nuclei plus extra neutrons plus energy
Draw or describe a chain reaction: neutrons from one fission cause further fissions
Describe nuclear fusion: two light nuclei combine to form a heavier nucleus plus energy
State that fusion requires extremely high temperatures (like inside stars)
Write and balance simple fission and fusion equations (conserving A and Z)
State qualitatively that in both fission and fusion, mass decreases and energy is released
Give practical examples: fission in nuclear power plants (Kudankulam), fusion in the Sun and stars
🌎Apply It: Real-World Physics
Can you spot nuclear physics in these real-world situations? Click each scenario to reveal the answer.
1
The Kudankulam Nuclear Power Plant in Tamil Nadu generates about 2000 MW of electricity. It uses uranium fuel rods. Inside the reactor, uranium-235 nuclei absorb neutrons and split apart, releasing energy that heats water into steam, which then turns turbines.
Is this fission or fusion? Why does splitting uranium release energy? If the uranium fuel contains 23592U, how many neutrons does each uranium nucleus have?
▼
Identify the Physics
This is nuclear fission -- splitting a heavy nucleus (uranium-235) into lighter nuclei. The word "split" is the key clue.
Work It Out
Energy is released because the total mass of the products (the two smaller nuclei + neutrons) is slightly less than the mass of the original uranium nucleus + the absorbed neutron. This "missing" mass has been converted into energy. For neutrons: A - Z = 235 - 92 = 143 neutrons in each uranium-235 nucleus.
Connect to the Syllabus
This connects to: nuclear fission (splitting a heavy nucleus), the mass-energy relationship (mass decreases, energy is released), and nuclide notation (calculating neutrons from A and Z). In the exam, you might be asked to write a fission equation and explain where the energy comes from.
Aha! Moment
India's nuclear programme was started by Homi Bhabha in the 1940s. The BARC campus in Mumbai is named after him. Every time you switch on a light in southern India, some of that electricity might come from nuclear fission at Kudankulam! One kilogram of uranium-235 releases as much energy as burning about 2,500 tonnes of coal -- that is the incredible power of nuclear fission!
2
ISRO's Aditya-L1 spacecraft, launched in September 2023, is India's first space mission to study the Sun. The Sun produces energy by combining hydrogen nuclei into helium at its core, where the temperature is about 15 million degrees Celsius.
What nuclear process powers the Sun? Why does it need such extreme temperatures? Write a simple fusion equation for hydrogen combining into helium.
▼
Identify the Physics
The Sun is powered by nuclear fusion -- light hydrogen nuclei join together to form heavier helium nuclei, releasing enormous energy in the process.
Work It Out
Extreme temperatures are needed because hydrogen nuclei are positively charged (they are protons). Positive charges repel each other. Only at extremely high temperatures do the nuclei move fast enough to overcome this repulsion and get close enough to fuse. A simple equation: 21H + 31H → 42He + 10n + energy.
Connect to the Syllabus
This connects to: nuclear fusion (light nuclei joining to form heavier nuclei), the mass-energy relationship (mass decreases, energy released), and writing fusion equations. The extreme temperatures needed for fusion are key -- this explains why we have fission power plants but not yet fusion power plants.
Aha! Moment
Scientists around the world are trying to recreate fusion on Earth to make clean, almost limitless energy. India is a member of the ITER project in France, which is building the world's largest fusion reactor. If they succeed, it could solve the world's energy problems forever -- because the fuel (hydrogen from water) is nearly unlimited! ISRO's Aditya-L1 spacecraft is studying the Sun's corona and solar wind to understand fusion processes better.
3
Rutherford's experiment used gold foil because gold can be hammered extremely thin -- just a few atoms thick. He chose alpha particles because they are heavy and positively charged. When most alpha particles sailed straight through the foil, Rutherford said he was as surprised as if "you fired a 15-inch artillery shell at tissue paper and it came back and hit you."
Why was Rutherford so shocked that some alpha particles bounced back? What did this tell him about the atom's structure?
▼
Identify the Physics
This is the alpha particle scattering experiment (Geiger-Marsden experiment, directed by Rutherford). It disproved the plum pudding model and established the nuclear model of the atom.
Work It Out
If the atom were a uniform spread of charge (plum pudding model), no alpha particle should ever bounce straight back -- there would be nothing dense or concentrated enough to deflect a heavy, fast-moving alpha particle by 180 degrees. The fact that some bounced back meant there must be something incredibly small, dense, and positively charged inside the atom -- the nucleus. The nucleus contains almost all the atom's mass concentrated in a tiny volume. Since most particles went straight through, most of the atom must be empty space.
Connect to the Syllabus
This is the alpha particle scattering experiment -- one of the most important experiments in physics history. You need to know: (1) what was observed (most pass through, some deflect, very few bounce back), (2) what each observation proves (empty space, positive nucleus, small dense nucleus), and (3) how this changed the model of the atom from the plum pudding model to the nuclear model.
Aha! Moment
Imagine rolling marbles across a football field that has one small, heavy rock hidden somewhere on it. Most marbles would roll straight across (empty space). A few might change direction slightly when they pass near the rock. And very rarely, one might hit the rock head-on and bounce right back at you. That is exactly what happens with alpha particles and the nucleus! The key insight is that the vast majority of the atom is nothingness -- if you removed all the empty space from every atom in your body, you would be smaller than a grain of sand.
4
In a chemistry lab at Bangalore International School, Tara is studying sodium chloride (table salt, which her mom uses to make sambar). She learns that when sodium (Na) reacts with chlorine (Cl), sodium loses an electron to become Na+ and chlorine gains an electron to become Cl-.
Sodium has 11 protons. How many electrons does a Na+ ion have? Has the nucleus of the sodium atom changed?
▼
Identify the Physics
This is about ion formation -- atoms gaining or losing electrons to form charged particles.
Work It Out
A neutral sodium atom has 11 protons and 11 electrons (charges balance). When it loses one electron to become Na+, it now has 11 protons but only 10 electrons. There are more positive charges than negative, so the overall charge is +1. The nucleus has NOT changed -- it still has 11 protons and the same number of neutrons. Only the electrons changed.
Connect to the Syllabus
This scenario tests your understanding of ions: (1) ions are formed by gaining or losing electrons only, (2) the nucleus never changes during ion formation, (3) positive ions have lost electrons (fewer electrons than protons), and (4) you can calculate the number of electrons in an ion by starting with the number of protons and adjusting for the charge.
Aha! Moment
This is why ionising radiation is dangerous -- it can knock electrons off atoms in your body, turning them into ions. When atoms in your DNA become ions, the chemical bonds break, and that can cause mutations or cell death. The nucleus never changes during ionisation -- it is only about electrons being removed or added! The salt (NaCl) in your sambar is made of Na+ and Cl- ions -- every time you eat, you are consuming billions of ions!
5
India's Pokhran-II nuclear tests in 1998 (Operation Shakti) demonstrated both fission and thermonuclear (fusion) capabilities. The thermonuclear device was designed to use a fission explosion to create the extreme temperatures needed to trigger fusion of hydrogen isotopes.
Why can't fusion happen at room temperature? Why was a fission bomb needed to trigger the fusion reaction? What is the fundamental physics principle that makes fusion so difficult?
▼
Identify the Physics
This involves both nuclear fission (the trigger) and nuclear fusion (the main reaction), and the concept that nuclei are all positively charged.
Work It Out
All atomic nuclei are positively charged (they contain protons). Like charges repel each other. For two nuclei to fuse, they must be pushed close enough together for the strong nuclear force to take over and bind them. This requires overcoming the enormous electrostatic repulsion between the two positive charges. The only way to do this is to give the nuclei so much kinetic energy that they can smash past the repulsion -- and that means temperatures of millions of degrees. A fission explosion provides exactly these extreme temperatures and pressures, acting as the "match" that lights the fusion "fuel."
Connect to the Syllabus
This scenario connects to both fission and fusion. Key points: (1) fusion requires extreme temperatures because nuclei are positively charged and repel each other, (2) fission is used as a "trigger" for fusion because it can generate those extreme temperatures, (3) both processes release energy because mass decreases. The concept of electrostatic repulsion between positive charges is fundamental to understanding why fusion is so difficult to achieve.
Aha! Moment
Fission is like lighting a matchstick (relatively easy). Fusion is like setting fire to a wet log -- you need the match (fission) to create enough heat first. This is why we have fission power plants today but no fusion power plants yet. We can control fission, but controlling fusion is far harder because we need to contain matter at millions of degrees! India conducted its first nuclear test (Pokhran-I, codenamed "Smiling Buddha") in 1974 under Prime Minister Indira Gandhi, making India the sixth country to test nuclear weapons.
Practice Questions: Section 5.1
Test your understanding of atomic structure, the nucleus, and nuclear reactions.
Score0 / 20
QUESTION 1
What is the charge of the nucleus of an atom?
A. Negative
B. Positive
C. Neutral
D. It varies from atom to atom
The nucleus contains protons (positive) and neutrons (neutral). Since protons are positive and neutrons have no charge, the overall charge of the nucleus is always positive.
QUESTION 2
An atom has 8 protons and 8 neutrons. What is its nucleon number?
A. 8
B. 16
C. 24
D. 0
The nucleon number (A) = protons + neutrons = 8 + 8 = 16. This is oxygen-16.
QUESTION 3
When an atom loses two electrons, it becomes:
A. A negative ion with charge -2
B. A positive ion with charge +2
C. A different element
D. A neutron
Losing electrons means losing negative charge. Two fewer electrons means the atom has 2 more protons than electrons, giving a charge of +2. It is a positive ion. It does NOT become a different element because the number of protons hasn't changed.
QUESTION 4
In Rutherford's alpha scattering experiment, most alpha particles passed straight through the gold foil. This shows that:
A. Gold atoms have no nucleus
B. Alpha particles have no charge
C. Atoms are mostly empty space
D. The nucleus is negatively charged
If most alpha particles pass straight through without hitting anything, it means there is very little solid matter for them to bump into. The atom must be mostly empty space with a very tiny nucleus.
QUESTION 5
The relative mass of an electron compared to a proton is approximately:
A. Equal (both are 1)
B. Half (0.5)
C. Negligible (about 1/1836)
D. Zero
An electron has a mass of about 1/1836 of a proton, which is negligibly small. This is why the mass of the atom is essentially the mass of the nucleus (protons + neutrons). The electron's mass is NOT zero -- it does have some mass, just very, very little.
QUESTION 6
An atom of phosphorus is represented as 3115P. How many neutrons does it have?
A. 31
B. 15
C. 16
D. 46
Neutrons = nucleon number - proton number = A - Z = 31 - 15 = 16 neutrons.
QUESTION 7
Which pair of atoms are isotopes of each other?
A.126C and 147N
B.168O and 188O
C.2311Na and 2312Mg
D.4018Ar and 4020Ca
Isotopes are atoms of the SAME element (same proton number Z) with different nucleon numbers (different number of neutrons). Only option B has the same Z (both have Z = 8, so both are oxygen) but different A (16 and 18). Options C and D have different Z values, so they are different elements, not isotopes.
QUESTION 8
In the alpha scattering experiment, a very small number of alpha particles bounced straight back. This shows that the nucleus is:
A. Large and spread out
B. Negatively charged
C. Very small, dense, and positively charged
D. Made of electrons
For an alpha particle (heavy, fast, positive) to bounce straight back, it must hit something very dense (with enough mass to repel it) and very small (since this happens rarely). The repulsion also confirms the nucleus is positively charged -- like charges repel.
QUESTION 9
Nuclear fission is the process of:
A. Joining two light nuclei together
B. Splitting a heavy nucleus into two lighter nuclei
C. Removing electrons from an atom
D. Adding neutrons to a stable nucleus
Fission means "splitting." In nuclear fission, a heavy, unstable nucleus (like uranium-235) splits into two lighter nuclei, releasing neutrons and a large amount of energy. This is used in nuclear power plants like Kudankulam.
QUESTION 10
In a fission reaction, the total mass of the products compared to the original nucleus is:
A. Greater (mass is created)
B. Slightly less (mass is converted to energy)
C. Exactly the same (mass is conserved)
D. Zero (all mass becomes energy)
In both fission and fusion, the total mass of the products is slightly LESS than the starting mass. This small decrease in mass is converted into a large amount of energy. Not ALL mass is converted -- just a small fraction.
QUESTION 11
Nuclear fusion powers the Sun. In the Sun, the main fusion process involves:
A. Hydrogen nuclei joining to form helium
B. Uranium nuclei splitting apart
C. Helium nuclei splitting into hydrogen
D. Carbon nuclei joining to form oxygen
The Sun fuses hydrogen (the lightest element) into helium. This is fusion because light nuclei are joining together. The Sun is NOT powered by fission (splitting).
QUESTION 12
A chlorine atom has 17 protons. A chloride ion (Cl-) has:
A. 16 protons and 17 electrons
B. 17 protons and 17 electrons
C. 17 protons and 18 electrons
D. 18 protons and 17 electrons
When an atom becomes a negative ion, it GAINS electrons. The number of protons never changes. Cl- has gained 1 electron, so it has 17 protons (unchanged) and 18 electrons (one more than before), giving a net charge of -1.
QUESTION 13
What particle was fired at gold foil in Rutherford's scattering experiment?
A. Electrons
B. Neutrons
C. Alpha particles
D. Gamma rays
Rutherford used alpha particles (helium nuclei, charge +2) because they are heavy and positively charged, making them ideal for probing the structure of atoms. Their positive charge meant they would be repelled by any positive charge inside the atom.
QUESTION 14
Two atoms have the same proton number but different nucleon numbers. They are called:
A. Ions
B. Isotopes
C. Isomers
D. Molecules
Isotopes have the same proton number (same element) but different nucleon numbers, which means they have different numbers of neutrons. Ions have gained or lost electrons. Isomers are a chemistry concept about molecular arrangement.
QUESTION 15
In the nuclide notation 5626Fe, the number 56 represents:
A. The number of protons only
B. The number of neutrons only
C. The total number of protons and neutrons
D. The number of electrons
In nuclide notation, the top number is the nucleon number (A) which equals the total number of protons + neutrons. For iron-56: A = 56, Z = 26, so neutrons = 56 - 26 = 30.
QUESTION 16
Which of the following is NOT a conclusion from the alpha scattering experiment?
A. The atom is mostly empty space
B. The nucleus is positively charged
C. Electrons orbit in fixed energy levels
D. The nucleus contains most of the atom's mass
The alpha scattering experiment showed three things: (1) mostly empty space, (2) positive nucleus, (3) small, dense nucleus with most of the mass. It did NOT tell us about electron energy levels -- that came from later experiments (Bohr model, spectroscopy).
QUESTION 17
In nuclear fission of U-235, the released neutrons can cause further fission reactions. This is called a:
A. Chain reaction
B. Fusion reaction
C. Chemical reaction
D. Neutralisation reaction
When fission of one uranium nucleus releases 2-3 neutrons, each of those neutrons can hit another uranium nucleus and cause it to split too, releasing more neutrons. This is a chain reaction. In a power plant, the reaction is controlled. In a nuclear weapon, it is uncontrolled.
QUESTION 18
An atom of potassium has 19 protons and 20 neutrons. What is its nuclide notation?
A.1920K
B.2019K
C.3919K
D.1939K
In nuclide notation, the top number is the nucleon number A = protons + neutrons = 19 + 20 = 39. The bottom number is the proton number Z = 19. So it is written as 3919K.
QUESTION 19
Which subatomic particle has no electrical charge?
A. Proton
B. Neutron
C. Electron
D. Alpha particle
The neutron has zero charge (it is neutral -- the name "neutron" comes from "neutral"). Protons have charge +1, electrons have charge -1, and alpha particles (2 protons + 2 neutrons) have charge +2.
QUESTION 20
In the fusion reaction 21H + 31H → 42He + X, what is particle X?
A. A proton
B. A neutron
C. An electron
D. An alpha particle
Balance the nucleon numbers: Left side: 2 + 3 = 5. Right side: 4 + A = 5, so A = 1. Balance the proton numbers: Left: 1 + 1 = 2. Right: 2 + Z = 2, so Z = 0. A particle with A = 1 and Z = 0 is a neutron (10n).
5.2 Radioactivity▼
Some atoms are unstable -- their nuclei have too many neutrons, too few neutrons, or are simply too heavy. These unstable nuclei try to become stable by spitting out particles or energy. This process is called radioactive decay, and the particles or energy released are called radiation. In this section, you will learn about the three types of radiation, how we measure them, how nuclei change when they decay, and how to stay safe around radioactive materials.
You are being hit by radiation right now. Don't worry -- it is a very small, natural amount called background radiation. It is always present around us, everywhere on Earth. Background radiation comes from both natural and man-made sources:
Sources of Background Radiation
Source
Type
Details
Radon gas
Natural
Seeps out of rocks and soil. The biggest source of background radiation. Kerala's monazite sand beaches have higher natural radiation due to thorium-rich minerals.
Rocks and buildings
Natural
Many rocks (especially granite) contain small amounts of radioactive elements. Buildings made from these rocks emit low-level radiation.
Food and drink
Natural
Bananas contain potassium-40 (radioactive!). So do many other foods. Don't worry -- the amount is tiny.
Cosmic rays
Natural
High-energy radiation from space. The atmosphere blocks most of it. People living at high altitude (like in Ladakh or Leh) receive slightly more cosmic radiation.
Medical procedures
Man-made
X-rays and CT scans at hospitals expose you to small doses of radiation.
Nuclear testing fallout
Man-made
Past nuclear tests (like Pokhran) left trace radioactive material in the environment.
The amount of background radiation you receive depends on where you live and what you do:
People living in areas with granite rocks (like parts of Karnataka and Kerala) receive more radiation from the ground.
People living at high altitudes (like in Ladakh or Shimla) receive more cosmic radiation because there is less atmosphere above them to act as a shield.
People who fly frequently receive more cosmic radiation (aircraft fly at 10,000+ metres altitude).
People who have many medical X-rays or CT scans receive more man-made radiation.
But here is the important thing: background radiation is normal and unavoidable. The levels are generally too low to cause any health problems. It has been present throughout all of human history, and our bodies have evolved to handle it.
⚠ Exam Tip
The exam often asks you to name sources of background radiation. Make sure you can name at least four: radon gas, rocks/soil, cosmic rays, food and drink. The biggest single source is always radon gas. Remember that background radiation comes from both natural and man-made sources, but natural sources account for the vast majority (about 85%).
💡 Memory Trick
Remember background radiation sources using R-R-C-F-M: Radon gas, Rocks and buildings, Cosmic rays, Food and drink, Medical sources. Think: "Really Really Cool Fried Momos" (a Bangalore favourite!).
Measuring Radiation: The Geiger-Muller Tube
We detect ionising radiation using a Geiger-Muller (GM) tube connected to a counter (or ratemeter). Here is how it works:
Radiation enters the GM tube through a thin window.
The radiation ionises the gas inside the tube (knocks electrons off gas atoms).
The free electrons and ions create a brief pulse of current.
The counter detects this pulse and records it as one "count."
Each count represents one particle or ray of radiation detected.
Count rate is measured in counts per second (counts/s) or counts per minute (counts/min).
Even with no radioactive source nearby, the GM tube will still register counts from background radiation.
The GM tube makes a clicking sound with each count -- the faster the clicking, the higher the radiation level.
Important: A GM tube does not tell you what type of radiation it is detecting. It simply counts all ionising radiation that enters the tube. To identify the type, you need to do absorption tests (place different materials between the source and the detector).
A Geiger-Muller tube connected to a counter detects ionising radiation by counting ionisation events
Supplement
Corrected Count Rate
When you use a GM tube to measure a radioactive source, the reading includes both the source's radiation AND the background radiation. To find the count rate from just the source, you need to subtract the background:
You must always measure the background count rate first (with no source present) before measuring the source.
Worked ExampleA GM tube measures a background count rate of 30 counts/min. When a radioactive source is placed nearby, the total count rate is 450 counts/min. What is the corrected count rate from the source?
The corrected count rate from the source alone is 420 counts/min.
Worked ExampleIn a school lab in Bangalore, students measure a background count rate of 24 counts/min. With a source, they record 84 counts/min. What count rate is due to the source alone?
Step 1: Write the Formula
Corrected count rate = Measured - Background
Step 2: Substitute
Corrected count rate = 84 - 24 = 60 counts/min
The source alone gives a count rate of 60 counts/min.
Worked ExampleA student measures the background count rate three times and gets: 28, 32, and 30 counts/min. She then measures a radioactive source and gets 230 counts/min. What is the corrected count rate?
Step 1: Average the Background
Average background = (28 + 32 + 30) / 3 = 90 / 3 = 30 counts/min. Taking multiple readings and averaging reduces the effect of random fluctuations.
Step 2: Subtract
Corrected count rate = 230 - 30 = 200 counts/min
The corrected count rate from the source is 200 counts/min.
⚠ Exam Tip
Why do we subtract background? Because the GM tube detects ALL radiation -- both from the source AND from the natural background. To find out how much radiation comes from the source alone, we must subtract the background. If you forget to do this, your answers will be too high, and your half-life calculations will be wrong.
5.2.2 The Three Types of Nuclear Emission
What Does "Ionising" Mean?
Before we look at the three types of radiation, we need to understand what "ionising" means. Ionising radiation is radiation that has enough energy to knock electrons off atoms, turning them into ions. This is what makes radioactive radiation dangerous to living things.
When radiation passes through a material, it can collide with atoms and knock their electrons loose. The atom becomes a positive ion (it lost an electron), and the freed electron becomes a negative ion. This process is called ionisation.
All three types of nuclear radiation (alpha, beta, and gamma) are ionising, but they differ in how strongly they ionise matter.
Spontaneous and Random
Radioactive decay is:
Spontaneous -- it happens by itself, without any outside trigger. You cannot make a nucleus decay by heating it, cooling it, or doing anything to it. It just happens.
Random -- you cannot predict which particular nucleus will decay next, or exactly when it will decay. It is like popcorn in a pan -- each kernel pops at a random moment, and you cannot predict which one will pop next!
The Three Types of Radiation
Property
Alpha (α)
Beta (β)
Gamma (γ)
What is it?
A helium nucleus (2 protons + 2 neutrons)
A fast-moving electron from the nucleus
An electromagnetic wave (like light, but much higher energy)
Symbol
42He or α
0-1e or β
γ
Charge
+2
-1
0 (no charge)
Mass
4 (heaviest)
Negligible (~0)
0 (no mass)
Ionising power
Strong (most ionising)
Moderate
Weak (least ionising)
Penetrating power
Low -- stopped by paper or a few cm of air
Medium -- stopped by a few mm of aluminium
High -- reduced by thick lead or concrete
Speed
Slow (about 5% of light speed)
Fast (up to 99% of light speed)
Speed of light
💡 Memory Trick -- Analogies!
Alpha particles are like big, slow trucks on a narrow road. They bump into everything (highly ionising) but get stuck quickly (stopped by paper).
Beta particles are like motorbikes weaving through traffic. They are lighter and faster, go further (through paper but stopped by aluminium), but don't cause as much disruption.
Gamma rays are like radio waves from a cell tower. They have no substance at all, travel far (through paper and aluminium), and are very hard to stop (only thick lead or concrete).
Penetration comparison: alpha stopped by paper, beta by aluminium, gamma reduced by thick lead
⚠ Exam Tip
Ionising power and penetrating power are OPPOSITES. Alpha is the MOST ionising but LEAST penetrating. Gamma is the LEAST ionising but MOST penetrating. Why? Because alpha particles are big and charged, they interact with every atom they pass, quickly losing all their energy. Gamma rays are small and uncharged, so they slip past most atoms and keep going.
Where Does Each Type Come From?
It is important to understand where each type of radiation originates:
Alpha particles come from the nucleus. They are emitted when a heavy, unstable nucleus needs to lose mass. The nucleus ejects a package of 2 protons and 2 neutrons (a helium nucleus). This is common in very heavy elements like uranium, radium, and plutonium.
Beta particles also come from the nucleus -- NOT from the electron shells. Inside the nucleus, a neutron transforms into a proton and an electron. The newly created electron is ejected at high speed. This happens in nuclei that have too many neutrons compared to protons.
Gamma rays come from the nucleus. After emitting an alpha or beta particle, the nucleus may still have excess energy. It releases this energy as a gamma ray (a high-frequency electromagnetic wave). Gamma emission often accompanies alpha or beta decay.
Notice: all three types originate from the nucleus, not from the electron shells. This is why they are called nuclear radiation.
⚠ Exam Tip
A very common exam mistake: students say beta particles are "electrons from the atom's shells." This is WRONG. The beta particle is an electron created inside the nucleus when a neutron changes into a proton. It is a completely new particle, not an existing orbital electron.
How to Identify the Type of Radiation (Absorption Test)
In the lab, you can identify what type of radiation a source emits by placing different materials between the source and the GM tube:
Measure the count rate with nothing between the source and detector.
Place paper between them. If the count rate drops to background, the source emits alpha.
If the count is still above background, place aluminium (a few mm). If the count drops to background now, the source emits beta.
If the count is still above background after aluminium, the source emits gamma. You would need thick lead or concrete to significantly reduce it.
Remember: some sources emit more than one type of radiation. If the count drops with paper but does not reach background, and drops further with aluminium, the source may emit both alpha and beta (or alpha and gamma).
Worked ExampleA student tests a radioactive source. The background count rate is 25 counts/min. She measures the following count rates with different absorbers between the source and GM tube:
No absorber: 525 counts/min Paper: 525 counts/min 3 mm aluminium: 285 counts/min 5 cm lead: 25 counts/min
Paper did NOT reduce the count rate (still 500). This means there is no alpha radiation (alpha would be stopped by paper).
Aluminium reduced the count from 500 to 260 -- a drop of 240 counts/min. This means some radiation was stopped by aluminium, so beta radiation is present.
Lead reduced the count from 260 to 0. The remaining 260 counts/min were stopped by lead, so gamma radiation is also present.
The source emits beta and gamma radiation (no alpha). About 240 counts/min were due to beta, and about 260 counts/min were due to gamma.
⚠ Exam Tip
When describing the absorption test in an exam, always mention that you must first measure the background count rate (with no source present) and subtract it. Also, always describe what happens step by step with each material, not just the final result.
Comparison of the three types of nuclear radiation: alpha, beta, and gamma
Summary: Comparing Alpha, Beta, and Gamma
Here is an easy way to compare the three types of radiation. Think of it as a spectrum from "heavy and slow" to "weightless and fast":
Alpha: Heaviest, slowest, most ionising, least penetrating. Like a bowling ball rolling across the room -- it knocks everything over but stops quickly.
Beta: Light, fast, moderately ionising, moderately penetrating. Like a tennis ball thrown hard -- goes further than the bowling ball but does less damage per hit.
Gamma: No mass, speed of light, weakly ionising, highly penetrating. Like a laser beam -- passes through most things, rarely interacts, but can still cause damage if it does.
Supplement
Deflection in Electric and Magnetic Fields
When radiation passes through electric or magnetic fields, the charged particles are deflected (bent), but gamma rays are not:
Alpha particles (+2 charge, heavy): Deflected slightly towards the negative plate in an electric field. In a magnetic field, they curve gently.
Beta particles (-1 charge, very light): Deflected strongly towards the positive plate in an electric field (opposite direction to alpha!). In a magnetic field, they curve sharply and in the opposite direction.
Gamma rays (no charge, no mass): Not deflected at all. They pass straight through both electric and magnetic fields.
Deflection in an electric field: alpha bends towards negative, beta bends towards positive, gamma goes straight
Why Alpha and Beta Deflect Differently
Beta deflects more than alpha for two reasons:
Beta particles have much less mass, so the same force produces a bigger acceleration (F = ma, so smaller m means bigger a).
Beta particles move faster, but their much smaller mass dominates.
Alpha deflects towards the negative plate because it is positive (attracted to negative). Beta deflects towards the positive plate because it is negative (attracted to positive).
⚠ Exam Tip
Remember the deflection directions: Alpha goes to negative (positive is attracted to negative). Beta goes to positive (negative is attracted to positive). Gamma goes straight (no charge, so no deflection). In a magnetic field, the directions are different (use Fleming's left-hand rule), but the key point is the same: alpha and beta deflect in opposite directions, beta deflects more due to lower mass, and gamma is not deflected.
Relative Ionising Effects
Why is alpha the most ionising? Two reasons:
Alpha has a larger charge (+2) compared to beta (-1), so it has a stronger interaction with the electrons in atoms it passes.
Alpha moves slower, so it spends more time near each atom, giving it more chance to knock electrons off.
Gamma rays have no charge and no mass, so they interact very weakly with matter and are the least ionising.
Deflection in Magnetic Fields
The behaviour of radiation in a magnetic field follows similar principles but with some key differences:
Alpha particles curve in one direction (determined by Fleming's left-hand rule). The curve is gentle because alpha particles are heavy.
Beta particles curve in the opposite direction to alpha (because they have opposite charge) and the curve is much tighter because beta particles are much lighter.
Gamma rays are not deflected at all -- they pass straight through the magnetic field without any change in direction.
The key points for the exam:
Alpha and beta curve in opposite directions (because they have opposite charges).
Beta curves more sharply than alpha (because it is much lighter -- same force produces more acceleration on a lighter particle).
Gamma is unaffected by both electric and magnetic fields.
⚠ Exam Tip
If an exam question shows radiation passing through a magnetic field and asks you to identify each type: the one that goes straight is gamma. Of the two that curve, the one that curves more is beta (lighter), and the one that curves less is alpha (heavier). They curve in opposite directions because of their opposite charges.
5.2.3 Radioactive Decay
What Is Radioactive Decay?
Radioactive decay is the process by which an unstable nucleus changes by emitting radiation (alpha, beta, or gamma). The key points are:
It is spontaneous -- it happens by itself without any external cause. You cannot make it happen faster by heating, cooling, crushing, or doing anything to the sample. It is a nuclear process, completely independent of physical or chemical conditions.
It is random -- you cannot predict which particular nucleus will decay next, or exactly when any individual nucleus will decay. However, for a large number of nuclei, you CAN predict roughly how many will decay in a given time (that is the concept of half-life).
When an atom emits alpha or beta radiation, the element changes -- it becomes a different element. This is because the number of protons changes! This is sometimes called transmutation (changing one element into another).
When an atom emits gamma radiation, the element does NOT change -- the nucleus simply loses excess energy.
Think of radioactive decay like a bowl of popcorn kernels in a hot pan. Each kernel pops (decays) at a random, unpredictable moment. You cannot predict which specific kernel will pop next. But if you have 1000 kernels, you can predict that after a certain time, roughly half will have popped. That is exactly how radioactive decay works!
⚠ Exam Tip
The words "spontaneous" and "random" have very specific meanings in physics:
Spontaneous = not triggered by anything external, happens by itself. NOT the same as "sudden" or "fast."
Random = cannot be predicted for an individual nucleus. NOT the same as "rare" or "uncommon."
Use these exact words in the exam. Do NOT say "it happens randomly and spontaneously" without explaining what each word means if asked to define them.
Supplement
Why Are Some Isotopes Radioactive?
An isotope is radioactive (unstable) when its nucleus has:
Too many neutrons compared to protons (the nucleus is neutron-rich and may emit beta radiation to convert a neutron into a proton)
Too few neutrons for stability
Too many nucleons overall (the nucleus is simply too heavy and may emit alpha radiation to shed mass)
⚠ Exam Tip
The exam might ask: "Why is carbon-14 radioactive but carbon-12 is not?" The answer is: Carbon-14 has 8 neutrons (too many for stability with 6 protons), making its nucleus unstable. Carbon-12 has 6 neutrons, which is the right balance for 6 protons, so it is stable. The key idea is that the neutron-to-proton ratio determines stability.
Alpha Decay
When a nucleus emits an alpha particle (42He):
The proton number (Z) decreases by 2
The nucleon number (A) decreases by 4
The element changes -- it becomes a different element (2 places lower in the periodic table)
AZX → A-4Z-2Y + 42He
X = parent nucleus (original element)Y = daughter nucleus (new element)He = alpha particle emitted
Worked ExampleRadium-226 (22688Ra) undergoes alpha decay. Write the decay equation and identify the daughter nucleus.
Step 1: Write the Alpha Decay Pattern
22688Ra → ??Y + 42He
Step 2: Calculate New Nucleon Number
A of daughter = 226 - 4 = 222
Step 3: Calculate New Proton Number
Z of daughter = 88 - 2 = 86. Element 86 is radon (Rn).
22688Ra → 22286Rn + 42He
Worked ExampleUranium-238 (23892U) undergoes alpha decay. What is the daughter nucleus?
Step 1: Apply the Rule
Alpha decay: A decreases by 4, Z decreases by 2.
Step 2: Calculate
New A = 238 - 4 = 234. New Z = 92 - 2 = 90. Element 90 is thorium (Th).
23892U → 23490Th + 42He
Beta Decay
When a nucleus emits a beta particle (0-1e), a neutron inside the nucleus changes into a proton and an electron. The electron is ejected at high speed as the beta particle.
The proton number (Z) increases by 1 (one more proton)
The nucleon number (A) stays the same (a neutron became a proton -- still the same total number of nucleons)
The element changes -- it becomes the next element up in the periodic table
AZX → AZ+1Y + 0-1e
The neutron-to-proton conversion: 10n → 11p + 0-1e
Worked ExampleCarbon-14 (146C) undergoes beta decay. Write the decay equation.
Step 1: Apply Beta Decay Rules
Beta decay: Z increases by 1, A stays the same.
Step 2: Calculate
New A = 14 (unchanged). New Z = 6 + 1 = 7. Element 7 is nitrogen (N).
146C → 147N + 0-1e
Worked ExampleStrontium-90 (9038Sr) undergoes beta decay. What does it become?
Step 1: Apply the Rules
Beta decay: A stays the same, Z increases by 1.
Step 2: Calculate
New A = 90. New Z = 38 + 1 = 39. Element 39 is yttrium (Y).
9038Sr → 9039Y + 0-1e
Gamma Emission
When a nucleus emits gamma radiation:
The proton number (Z) does NOT change
The nucleon number (A) does NOT change
The element does NOT change -- the nucleus just loses excess energy
Gamma emission often happens alongside alpha or beta decay. After the nucleus emits an alpha or beta particle, it may still have excess energy, which it releases as a gamma ray.
⚠ Exam Tip
Common misconception about beta particles: Students often say "the electron comes from the electron shell." This is WRONG! The beta particle (electron) is created inside the nucleus when a neutron changes into a proton and an electron. It is NOT an orbital electron. The equation inside the nucleus is: 10n → 11p + 0-1e. The newly created electron is then ejected at high speed.
Worked ExampleA nucleus of 24195Am decays to form 23793Np. What type of decay has occurred? Write the complete equation.
Step 1: Find the Changes
Change in A: 241 - 237 = 4 (decreased by 4) Change in Z: 95 - 93 = 2 (decreased by 2)
Step 2: Identify the Decay Type
A decreased by 4 and Z decreased by 2. This matches alpha decay (an alpha particle has A = 4, Z = 2).
Step 3: Write the Equation
Check: Left: A = 241, Z = 95. Right: A = 237 + 4 = 241, Z = 93 + 2 = 95. Both sides balance.
24195Am → 23793Np + 42He (alpha decay)
Worked ExamplePhosphorus-32 (3215P) undergoes beta decay. Write the decay equation and name the element formed.
Step 1: Apply Beta Decay Rules
Beta decay: A stays the same, Z increases by 1.
Step 2: Calculate
New A = 32 (unchanged). New Z = 15 + 1 = 16. Element 16 is sulphur (S).
Step 3: Verify
Left: A = 32, Z = 15. Right: A = 32 + 0 = 32, Z = 16 + (-1) = 15. Both sides balance.
3215P → 3216S + 0-1e (the element formed is sulphur)
⚠ Exam Tip
Always check your decay equations balance! The total nucleon numbers on both sides must be equal, and the total proton numbers on both sides must be equal. This is the number one way to check your answer in the exam.
Summary of Decay Types
Decay Type
Particle Emitted
Change in Z
Change in A
Element Changes?
Alpha (α)
42He
Decreases by 2
Decreases by 4
Yes -- becomes element 2 places lower
Beta (β)
0-1e
Increases by 1
No change
Yes -- becomes element 1 place higher
Gamma (γ)
EM radiation (photon)
No change
No change
No -- same element, just loses energy
How to Balance Nuclear Decay Equations
Nuclear equations must always balance on both sides. Here is a step-by-step method:
Write down what you know on each side of the arrow.
Add up all the nucleon numbers (A) on the left side. The total on the right side must be the same.
Add up all the proton numbers (Z) on the left side. The total on the right side must be the same.
If there is an unknown particle, use the balance to work out its A and Z values.
Use the Z value to identify the element (look it up on the periodic table).
Common particles you need to know:
Particle
Symbol
A (top number)
Z (bottom number)
Proton
11p
1
1
Neutron
10n
1
0
Alpha particle
42He
4
2
Beta particle
0-1e
0
-1
Gamma ray
γ
0
0
💡 Memory Trick -- Decay Changes
Alpha: "A loses 4, Z loses 2" -- think "Alpha takes Away 4 and 2" (A for Away!).
Beta: "A stays same, Z goes up By 1" -- think "Beta Builds Z up by 1" (B for Builds!).
Gamma: "Nothing changes" -- think "Gamma just Glows" (it releases energy but nothing else changes).
Worked ExampleThorium-232 (23290Th) undergoes alpha decay to form radium. The radium then undergoes beta decay. What is the final nucleus after both decays?
After alpha then beta decay: 23290Th → 22888Ra → 22889Ac. The final nucleus is actinium-228.
5.2.4 Half-life
What Is Half-life?
Half-life is the time it takes for half the undecayed radioactive nuclei in a sample to decay. It can also be defined as the time for the activity (count rate) of a sample to fall to half its original value.
Think of it like the popcorn analogy: if you have 1000 unpopped kernels and after 2 minutes, 500 have popped, the half-life is 2 minutes. After another 2 minutes, half of the remaining 500 will have popped (250 more), leaving 250 unpopped. And so on.
Here is the pattern:
Number of Half-lives
Fraction Remaining
If starting with 1000 nuclei
Number Decayed
0
1 (all)
1000
0
1
1/2
500
500
2
1/4
250
750
3
1/8
125
875
4
1/16
62.5
937.5
5
1/32
31.25
968.75
Notice that each time, exactly half of whatever remains decays. After one half-life, 500 remain. After the second half-life, half of those 500 (which is 250) decay, leaving 250. It is not "250 decay each time" -- it is always "half of whatever is left."
Visual representation of half-life: each step, half of the remaining undecayed nuclei decay
Radioactive decay curve showing how activity halves with each half-life
⚠ Exam Tip
Two definitions of half-life -- know both! Half-life can be defined as: (1) the time taken for half the undecayed nuclei to decay, OR (2) the time taken for the activity (count rate) to fall to half its original value. Both definitions are correct and may appear in the exam. Use whichever one fits the question better.
Worked ExampleA radioactive sample has an activity of 1200 counts/min. After 30 minutes, the activity has dropped to 150 counts/min. What is the half-life?
Worked ExampleA sample of iodine-131 has a half-life of 8 days. If the initial activity is 6400 counts/min, what will the activity be after 32 days?
Step 1: How Many Half-lives?
Number of half-lives = 32 / 8 = 4 half-lives
Step 2: Halve 4 Times
6400 → 3200 → 1600 → 800 → 400
After 32 days, the activity will be 400 counts/min.
Worked ExampleFrom the decay curve below, a radioactive sample starts with an activity of 800 counts/min. After 10 minutes, the activity is 400 counts/min. After 20 minutes, it is 200 counts/min. After 30 minutes, it is 100 counts/min. (a) What is the half-life? (b) What would the activity be after 50 minutes?
(a) Half-life = 10 minutes. (b) After 50 minutes, the activity is 25 counts/min.
Worked ExampleThe following data was collected for a radioactive source. The background count rate was separately measured as 20 counts/min. Determine the half-life.
Time 0: 820 - 20 = 800 counts/min
Time 10: 420 - 20 = 400 counts/min
Time 20: 220 - 20 = 200 counts/min
Time 30: 120 - 20 = 100 counts/min
Time 40: 70 - 20 = 50 counts/min
Step 2: Find the Halving Pattern
800 → 400 (halved in 10 min) 400 → 200 (halved in 10 min) 200 → 100 (halved in 10 min) 100 → 50 (halved in 10 min)
Step 3: Determine Half-life
Each time the corrected count rate halves, exactly 10 minutes pass.
The half-life is 10 minutes. (Note: we had to subtract the background of 20 counts/min first!)
⚠ Exam Tip
Reading half-life from a graph: Pick any value on the y-axis (say 800). Find where it drops to half (400). Read across to the curve, then down to the time axis. The time difference is one half-life. Always check by doing it from a different starting point -- you should get the same answer. If you get different answers, your graph reading may be slightly off -- use the average.
The Dice Experiment Analogy
In class, your teacher might demonstrate half-life using dice. Here is how it works:
Start with 100 dice (these represent 100 undecayed radioactive nuclei).
Roll them all. Remove every die that shows a 6 (these have "decayed").
Count how many remain. Roll those again. Remove all the 6s.
Keep going until very few dice remain.
You cannot predict WHICH specific die will show a 6 on any roll (random!). No one forces the dice to show 6 -- it happens by itself (spontaneous!). But you can predict that roughly 1/6 of the dice will be removed each round. This is exactly how radioactive decay works -- random for individual nuclei, but predictable for large numbers.
Important Things About Half-life
Half-life is a constant for any given isotope. It does not change with temperature, pressure, chemical reactions, or any other external condition.
Different isotopes have wildly different half-lives: uranium-238 has a half-life of 4.5 billion years, while polonium-214 has a half-life of just 0.000164 seconds!
After one half-life, 50% of the original nuclei remain undecayed. After two half-lives, 25% remain. After ten half-lives, less than 0.1% remain -- effectively the sample is no longer significantly radioactive.
Half-life also applies to the activity (count rate) of a sample: the activity halves with each half-life too.
Each fraction is the previous one divided by 2. After 3 half-lives, only 1/8 (12.5%) remains. After 4 half-lives, only 1/16 (6.25%) remains. If the exam gives you a fraction and asks how many half-lives, just count how many times you can double the denominator starting from 1.
Step-by-Step Guide: Finding Half-life from Data
Here is a reliable method for half-life questions in the exam:
Step 1: If background radiation is given, subtract it from all count rate values first to get the corrected count rates.
Step 2: Write out the corrected values in order.
Step 3: Find where the value halves. Note the time taken for each halving.
Step 4: Check that the halving time is consistent (it should be the same each time). If it varies slightly, this is normal -- take the average.
Step 5: The consistent halving time is your half-life.
Alternatively, if given start and end values:
Count how many times you need to halve the starting value to reach the ending value.
Divide the total time by the number of halvings.
Worked ExampleA radioactive sample initially contains 8000 undecayed atoms. After 15 minutes, only 1000 atoms remain undecayed. Calculate the half-life.
The type of radiation and the half-life of an isotope determine what it can be used for. Here are the key applications you need to know:
Application
Radiation Type Needed
Half-life Needed
Why?
Smoke detectors
Alpha
Long (Am-241: 432 years)
Alpha ionises air between two plates, creating a small current. Smoke absorbs the alpha particles, current drops, alarm sounds. Long half-life means it works for years without replacement.
Food irradiation
Gamma
Long
Gamma penetrates packaging to kill bacteria. Must not make food radioactive (gamma does not do this). Long half-life so the source lasts.
Sterilisation of medical equipment
Gamma
Long
Same principle as food irradiation -- gamma penetrates sealed packaging to kill microbes without opening it.
Thickness measurement (e.g., paper mills, metal sheets)
Beta
Long
Beta partially penetrates thin materials. Too thick = less beta gets through. Too thin = more gets through. A detector measures the transmitted beta and adjusts the rollers. Alpha would be fully stopped; gamma would pass through unchanged.
Cancer diagnosis (tracers)
Gamma
Short (Tc-99m: 6 hours)
Gamma passes out of the body and is detected by cameras. Short half-life means the patient is not radioactive for long. Alpha and beta would be absorbed by the body and damage tissue.
Cancer treatment
Gamma
Moderate (Co-60: 5.3 years)
Gamma rays from cobalt-60 are focused on tumours to destroy cancer cells. The source lasts long enough to be practical.
⚠ Exam Tip
When explaining why a particular isotope is suitable for an application, always mention BOTH the type of radiation AND the half-life. For example: "Americium-241 is suitable for smoke detectors because it emits alpha radiation (which ionises air to create a detectable current) and has a long half-life (so it doesn't need to be replaced frequently)."
How to Answer "Why is this isotope suitable?" Questions
The exam loves these questions! Here is a template you can follow:
State the radiation type and why it is needed (e.g., "Alpha is needed because it ionises air" or "Gamma is needed because it can penetrate through...")
State the half-life and why it is suitable (e.g., "A long half-life means it does not need to be replaced often" or "A short half-life means the patient is not radioactive for long")
Explain why other types would NOT work if the question asks (e.g., "Alpha would be absorbed by the body and could not be detected externally" or "Gamma would pass through the paper unchanged, making thickness measurement impossible")
Worked ExampleA factory produces aluminium sheets. They want to use a radioactive source to monitor the thickness of the sheets continuously. Explain why a beta source with a long half-life is the best choice.
Why Beta?
Beta particles are partially absorbed by a few millimetres of aluminium. If the sheet is too thick, fewer beta particles reach the detector on the other side, and the count rate decreases. If the sheet is too thin, more beta particles reach the detector, and the count rate increases. This change in count rate can be used to automatically adjust the rollers.
Why Not Alpha?
Alpha particles would be completely stopped by even a very thin sheet of aluminium. There would be zero count rate regardless of thickness, making it useless for measuring thickness changes.
Why Not Gamma?
Gamma rays would pass through the aluminium sheet with very little absorption regardless of thickness. The count rate would barely change even if the thickness varied a lot, making it insensitive to thickness changes.
Why Long Half-life?
A long half-life means the source does not need to be replaced frequently. In a factory running 24/7, you want a source that lasts years, not one that decays in hours or days. Frequent replacement would be costly and disruptive.
Beta radiation is partially absorbed by aluminium, so changes in thickness cause measurable changes in count rate. A long half-life ensures the source remains effective for years without replacement.
5.2.5 Safety Precautions
Dangers of Ionising Radiation
Ionising radiation is dangerous because it can knock electrons off atoms in living cells. This can:
Kill cells -- high doses destroy cells, causing radiation sickness
Cause mutations -- damage to DNA can cause genetic changes
Cause cancer -- mutations in DNA can lead to uncontrolled cell growth
Safe Handling Rules
Always use tongs or remote handling tools -- never pick up radioactive sources with your hands
Store sources in lead-lined containers when not in use
Keep exposure time as short as possible
Point sources away from people
Never eat, drink, or smoke when working with radioactive materials
Supplement
The Three Safety Principles
To reduce radiation exposure, there are three key strategies:
Reduce TIME: Spend as little time as possible near the source. Less time = less radiation absorbed.
Increase DISTANCE: Move as far away from the source as possible. Radiation intensity decreases with distance.
Use SHIELDING: Place absorbing materials (lead, concrete) between you and the source. The right shielding depends on the type of radiation.
💡 Memory Trick
Remember the three safety principles as T-D-S: Time, Distance, Shielding. Think of it as "T.D.S." -- just like the TDS (Total Dissolved Solids) reading on your water purifier at home. Less is better for both radiation exposure AND TDS!
The three principles of radiation safety: reduce time, increase distance, use shielding (T-D-S)
Irradiation vs Contamination
These two words are often confused, but they mean very different things:
Feature
Irradiation
Contamination
What happens?
An object is exposed to radiation from an external source. The radiation passes through or is absorbed.
Radioactive material is deposited on or inside an object. The radioactive atoms are now part of or attached to the object.
Does the object become radioactive?
No -- once the radiation source is removed, the object is no longer receiving radiation. It does not emit radiation itself.
Yes -- the radioactive material is now on/in the object, so it continues to emit radiation until the radioactive atoms decay.
Example
Having a chest X-ray. The radiation passes through you, but you do not become radioactive afterwards.
Nuclear fallout landing on crops. The crops now have radioactive dust on them and are contaminated.
How to deal with it?
Simply move away from the source or use shielding.
Much harder -- you must physically remove the radioactive material (washing, scrubbing, or disposing of contaminated items).
⚠ Exam Tip
Irradiation does NOT make things radioactive. Just like standing in sunlight does not make you into a light source, being irradiated does not make you radioactive. Contamination IS radioactive material being left behind. This distinction is crucial in exam answers about food irradiation and medical uses of radiation.
Choosing the Right Shielding
The type of shielding you need depends on the type of radiation:
Alpha sources: A few centimetres of air or a sheet of paper is enough. However, if there is a risk of inhaling or ingesting alpha-emitting material, you need sealed containers and respiratory protection.
Beta sources: A few millimetres of aluminium will stop beta particles. Perspex (acrylic) screens are also effective and allow you to see the work area.
Gamma sources: Thick lead or concrete is needed. Lead aprons are used in hospitals during X-ray procedures. Concrete walls in nuclear power plants can be several metres thick.
Summary: Uses and Their Radiation Requirements
Let's consolidate everything we have learned about applications. For each use, think about: (a) what type of radiation is needed and why, (b) what half-life is needed and why.
Worked ExampleA doctor wants to check whether a patient's thyroid gland is working properly. She plans to give the patient a radioactive tracer to drink, then use a gamma camera to image the thyroid from outside the body. Should she use an alpha, beta, or gamma emitter? Should it have a long or short half-life? Explain your choices.
Radiation Type
She should use a gamma emitter. Gamma rays can pass out of the body and be detected by the camera outside. Alpha would be stopped inside the body (too dangerous internally, cannot be detected externally). Beta would also be mostly absorbed by body tissue before reaching the camera.
Half-life
She should use an isotope with a short half-life (hours to a few days). This is long enough for the tracer to reach the thyroid and for the scan to be completed, but short enough that the patient is not radioactive for a dangerously long time. Iodine-131 (half-life 8 days) is commonly used for thyroid scans. Tc-99m (6 hours) is used for other organs.
Why Not a Long Half-life?
A long half-life (years) would mean the patient remains radioactive for a very long time, increasing their total radiation dose. The tracer would keep emitting radiation long after the scan is finished, with no benefit but increasing the risk of damage to healthy cells.
Use a gamma emitter with a short half-life. Gamma can escape the body for detection; a short half-life minimises the patient's radiation exposure.
Which Type Is Most Dangerous?
This is a tricky question because the answer depends on whether the source is outside or inside your body:
Outside the body: Gamma is the most dangerous because it penetrates skin and reaches internal organs. Alpha is least dangerous because it is stopped by your dead outer layer of skin.
Inside the body (if you swallow or breathe in a radioactive source): Alpha is the most dangerous! All of its ionising energy is absorbed by your internal tissues, causing maximum damage. Gamma is less dangerous inside because much of it passes straight through without interacting.
⚠ Exam Tip
This "inside vs outside" distinction is a favourite exam question! If the source is outside the body, gamma is most harmful (penetrates to organs). If the source is inside the body (inhaled or swallowed), alpha is most harmful (all energy deposited in tissue, highly ionising).
Radiation Exposure in Everyday Life
We are all exposed to small amounts of radiation every day. Here are some typical annual doses (in millisieverts, mSv):
Average natural background: about 2.4 mSv per year
Kerala monazite sands: up to 70 mSv per year in some spots
A single chest X-ray: about 0.02 mSv
A CT scan: about 7 mSv
Maximum allowed for nuclear workers: 20 mSv per year
The key principle is: keep your total exposure as low as reasonably achievable (this is called the ALARA principle).
⚠ Exam Tip
In an exam question about safety, mention specific precautions, not vague ones. Don't just say "be careful." Say: "Use long tongs to keep distance from the source" or "Store in a lead-lined box." Specific answers get marks; vague answers don't. The three key words to remember are: Time, Distance, Shielding.
Safety Precautions in a School Lab
If you ever handle radioactive sources in your physics lab at school, here are the rules your teacher will follow:
Always use long-handled tongs to hold the source -- never use bare hands.
Keep the source at arm's length and point it away from your body and other people.
Keep exposure time to a minimum -- do your measurements quickly and return the source to its lead-lined container.
Never eat, drink, or put your hands near your face when working with radioactive sources.
Store all sources in lead-lined containers in a locked, labelled cupboard.
Wash your hands thoroughly after any practical work involving radioactive materials.
The teacher should have a radiation monitoring badge (dosimeter) to track their total exposure over time.
⚠ Common Exam Question Types -- Section 5.2
Type 1: "Name sources of background radiation." Give at least 4: radon gas, rocks/soil, cosmic rays, food/drink. The biggest is always radon.
Type 2: "Compare the properties of alpha, beta, and gamma radiation." Use a table: charge, mass, ionising power, penetrating power, stopped by what.
Type 3: "Write a decay equation for alpha/beta decay." Alpha: Z decreases by 2, A decreases by 4. Beta: Z increases by 1, A unchanged. Always check both sides balance.
Type 4: "Calculate the half-life from data." Subtract background first! Then find how many halvings occur in the given time. Half-life = total time / number of halvings.
Type 5: "Explain why a particular isotope is suitable for a given application." State the radiation type and why it works, the half-life and why it is suitable, and why other types would not work.
Type 6: "State three safety precautions." Be specific: use tongs (distance), minimise time, store in lead-lined containers (shielding). Do NOT say "be careful" -- that gets zero marks!
Worked ExampleA radioactive source has an activity of 2400 counts/min. The background count rate is 40 counts/min. After 6 hours, the measured count rate is 190 counts/min. What is the half-life of the source?
Step 1: Find Corrected Count Rates
Initial corrected count rate = 2400 - 40 = 2360 counts/min
Wait -- this doesn't halve neatly. Let me re-read: the measured count rate at the start was 2400, so corrected = 2400 - 40 = 2360. After 6 hours, measured = 190, so corrected = 190 - 40 = 150.
Hmm, let me check: 2360 to 150... Does 2360 halve neatly to 150?
2360 → 1180 → 590 → 295 → 147.5
After 4 halvings we get approximately 147.5, which is close to 150. So approximately 4 half-lives.
Step 2: A Better Approach
Actually, let's re-examine. Perhaps the initial activity should be taken as given (not needing background correction because it says "activity"). If the source activity is 2400 and the measured count rate after 6 hours is 190:
Corrected after 6 hours: 190 - 40 = 150 counts/min
2400 → 1200 → 600 → 300 → 150
That's exactly 4 halvings! So 4 half-lives = 6 hours.
The half-life is 1.5 hours (90 minutes). Key step: you MUST subtract the background count rate before finding half-lives!
Worked ExampleCobalt-60 has a half-life of 5.3 years and is used in cancer treatment. A hospital buys a cobalt-60 source with an activity of 4000 units. What will the activity be after 15.9 years? After how long will the activity drop below 500 units?
Part A: Activity After 15.9 Years
Number of half-lives = 15.9 / 5.3 = 3 half-lives exactly.
4000 → 2000 → 1000 → 500 units
Part B: When Activity Drops Below 500
From Part A, after exactly 3 half-lives (15.9 years), the activity is exactly 500. So the activity drops below 500 units after just over 15.9 years (or 3 half-lives). After 4 half-lives (21.2 years), it would be 250 units.
After 15.9 years, the activity is 500 units. The activity drops below 500 units just after 15.9 years (3 half-lives). This is why hospitals periodically need to replace their cobalt-60 sources!
How to Read Half-life from a Decay Curve Graph
In exams, you will often be given a graph showing activity (or count rate) on the y-axis and time on the x-axis. The curve starts high and falls, getting flatter but never quite reaching zero. Here is a step-by-step method to find the half-life from any such graph:
Check whether background has already been subtracted. If the question states "corrected count rate" or "activity" on the y-axis, it is already done. If it says "measured count rate" and gives you a background value, you must subtract the background from every reading first.
Pick ANY starting value on the y-axis. It does not have to be the initial value. For example, if the graph starts at 800 counts/min, you could start there, or you could start at 400, or 200 -- any value that appears clearly on the graph.
Calculate half of that value. If you chose 800, then half = 400.
Draw a horizontal line from your starting value across to the curve. Mark where it hits the curve. Read the time value directly below this point on the x-axis. Call this t1.
Draw a horizontal line from the half-value across to the curve. Mark where it hits the curve. Read the time value directly below this point on the x-axis. Call this t2.
The half-life is t2 - t1. This is the time taken for the activity to halve from your starting value to half of it.
Check your answer by repeating with a different starting value. If you get the same time difference, your answer is correct. If you get a slightly different value, take the average.
Common mistake: Students often only read one time value. You need TWO time values (the time when activity is X, and the time when activity is X/2). The half-life is the DIFFERENCE between them.
Another common mistake: Forgetting to subtract background radiation before reading from the graph. If the background is 20 counts/min and the graph shows measured values, subtract 20 from every reading.
Worked ExampleA decay curve graph shows corrected count rate on the y-axis. At time = 0 minutes, the activity is 1200 counts/min. At time = 4 minutes, the activity is 600 counts/min. At time = 8 minutes, the activity is 300 counts/min. At time = 12 minutes, the activity is 150 counts/min. What is the half-life?
Step 1: Check Background
The question says "corrected count rate" so background has already been subtracted. Good -- we can use the values directly.
Step 2: Pick a Starting Value and Find When It Halves
Starting value: 1200 counts/min at t = 0 min
Half of 1200 = 600 counts/min, which occurs at t = 4 min
So one half-life = 4 - 0 = 4 minutes
Step 3: Verify with Another Starting Value
Starting value: 600 counts/min at t = 4 min
Half of 600 = 300 counts/min, which occurs at t = 8 min
Half-life = 8 - 4 = 4 minutes (same -- confirmed!)
Step 4: Triple-check
Starting value: 300 counts/min at t = 8 min
Half of 300 = 150 counts/min, which occurs at t = 12 min
Half-life = 12 - 8 = 4 minutes (confirmed again!)
The half-life is 4 minutes. We verified this by checking three different pairs of values on the graph, and they all gave the same answer.
Half-lives of Some Important Isotopes
Isotope
Half-life
Use or Significance
Polonium-214
0.000164 seconds
Very short -- decays almost instantly
Technetium-99m
6 hours
Medical tracers (short enough for patient safety)
Iodine-131
8 days
Thyroid treatment and diagnosis
Cobalt-60
5.3 years
Cancer treatment (gamma source)
Strontium-90
29 years
Dangerous nuclear fallout product
Americium-241
432 years
Smoke detectors (lasts decades)
Carbon-14
5,730 years
Carbon dating of ancient objects
Uranium-238
4.5 billion years
Dating rocks and the Earth itself
Nuclear Energy in India: A Quick Overview
India has a significant nuclear energy programme. Here are some key facts:
Kudankulam Nuclear Power Plant (Tamil Nadu) -- India's largest, with two 1000 MW reactors and more under construction. Uses pressurised water reactors with enriched uranium fuel.
Tarapur Atomic Power Station (Maharashtra) -- India's first commercial nuclear power station, operational since 1969. It was built with American assistance.
BARC (Mumbai) -- India's premier nuclear research centre, named after Homi Bhabha. Develops reactor designs, isotope production, and nuclear medicine technology.
India has a unique three-stage nuclear programme designed to eventually use thorium (which India has in abundance in Kerala's monazite sands) as nuclear fuel.
Nuclear power currently provides about 3% of India's electricity, but this is planned to increase significantly.
All Indian nuclear reactors use nuclear fission. Fusion power is still being researched worldwide (India is a partner in the ITER project in France).
💡 Memory Trick -- Matching Isotopes to Applications
Think of it as matching the "personality" of the isotope to the job:
Quick jobs need short half-lives: Medical scans take hours, so Tc-99m (6 hours) is perfect -- it does its job and then mostly disappears.
Permanent jobs need long half-lives: Smoke detectors need to work for decades, so Am-241 (432 years) is ideal -- it will never run out in your lifetime.
The radiation type must match the job: Need to go through packaging? Use gamma. Need to ionise air? Use alpha. Need to partially penetrate thin materials? Use beta.
Key Concepts -- Section 5.2 Summary
Background radiation is always present from natural sources (radon, rocks, cosmic rays, food) and some man-made sources (medical, nuclear fallout).
A Geiger-Muller tube detects ionising radiation by counting ionisation events.
Radioactive decay is spontaneous (happens by itself) and random (unpredictable for individual nuclei).
Alpha (α): helium nucleus, +2 charge, mass 4, most ionising, stopped by paper.
Beta (β): fast electron from nucleus, -1 charge, negligible mass, moderately ionising, stopped by aluminium.
Gamma (γ): EM wave, no charge, no mass, least ionising, reduced by thick lead/concrete.
Alpha decay: Z decreases by 2, A decreases by 4. Beta decay: Z increases by 1, A unchanged. Gamma: no change.
Half-life = time for half the undecayed nuclei to decay (or activity to halve).
Applications: smoke detectors (alpha), food irradiation (gamma), thickness measurement (beta), medical tracers (gamma, short half-life).
Safety: reduce time, increase distance, use shielding.
Irradiation does NOT make objects radioactive. Contamination DOES (radioactive material left on/in the object).
Outside the body: gamma is most dangerous (penetrates to organs). Inside the body: alpha is most dangerous (all energy absorbed by tissue).
Final Revision Checklist -- Section 5.2
Before the exam, make sure you can confidently do ALL of these. Tick them off as you practise:
Name at least 4 sources of background radiation (the biggest one is always radon gas)
Explain how a Geiger-Muller tube detects radiation (ionisation of gas → pulse of current → count)
Calculate corrected count rates (measured minus background)
State all properties of alpha, beta, and gamma in a table (charge, mass, ionising power, penetrating power, stopped by what)
Explain the inverse relationship between ionising and penetrating power
Describe deflection in electric fields (alpha to negative, beta to positive, gamma straight)
Explain why beta deflects more than alpha (lighter mass)
Write alpha decay equations (Z - 2, A - 4)
Write beta decay equations (Z + 1, A unchanged) and explain the neutron-to-proton conversion
State that gamma causes no change in Z or A
Define half-life using both definitions
Calculate half-life from tables (with and without background subtraction)
Read half-life from decay curve graphs
Match isotopes to applications based on radiation type AND half-life
State the three safety principles: Time, Distance, Shielding (T-D-S)
List specific lab safety precautions (tongs, lead containers, minimise time, point away)
Explain the difference between irradiation and contamination
Explain which type is most dangerous outside vs inside the body
🌎Apply It: Real-World Physics
Can you spot radioactivity and nuclear physics in these real-world situations? Click each scenario to reveal the answer.
1
The beaches of Kollam and Alappuzha in Kerala are famous for their black monazite sands, which contain thorium -- a naturally radioactive element. Studies have shown that people living in these areas receive about 5-10 times more natural background radiation than the global average, yet health studies have not found significantly higher cancer rates.
What is the main source of this extra background radiation? Why might the health effects be less severe than expected?
▼
Identify the Physics
This is about background radiation from natural sources. Thorium in monazite sand is a radioactive element that decays through a chain of steps, eventually producing radon gas (which emits alpha radiation). The radiation from the sand itself includes alpha, beta, and gamma radiation.
Work It Out
The main source is thorium and its decay products in the monazite sand, plus radon gas that seeps out of the ground. Alpha radiation from thorium is stopped by skin (so external exposure is limited), but radon gas can be inhaled, delivering alpha radiation directly to lung tissue. The health effects may be less severe than expected because: (1) much of the alpha radiation is stopped by the outer layer of dead skin, (2) humans may have some biological repair mechanisms for low-level radiation damage, and (3) the radiation is spread over a lifetime rather than delivered in a single high dose.
Connect to the Syllabus
This scenario connects to several syllabus points: background radiation (radon gas is the biggest natural source), the fact that background radiation exists everywhere, and the concept that alpha radiation (from radon's decay) is the most ionising type. It also connects to the safety principle of shielding -- houses in Kerala with good ventilation have lower indoor radon levels than poorly ventilated ones.
Aha! Moment
Kerala's natural radiation levels have been studied by scientists from BARC and international agencies for decades. It is one of the world's most important sites for understanding the health effects of low-level radiation. This research helps set safety standards for nuclear workers worldwide! Despite receiving 5-10 times more radiation than average, the people of these areas live normal, healthy lives -- showing that the human body can handle low levels of radiation without significant harm.
2
The Food Safety and Standards Authority of India (FSSAI) has approved the use of gamma irradiation to preserve spices like turmeric, chilli powder, and onions. A cobalt-60 source emits gamma rays that kill bacteria and insects in the food without making the food radioactive.
Why is gamma radiation used instead of alpha or beta for food irradiation? Why does the food not become radioactive after treatment? Why is cobalt-60 (half-life 5.3 years) a good choice?
▼
Identify the Physics
This is about the application of gamma radiation in food preservation, choosing the right type of radiation and half-life for the job.
Work It Out
Why gamma? Gamma rays have the highest penetrating power, so they can pass through the food packaging and reach all parts of the food to kill bacteria and insects throughout. Alpha would be stopped by the packaging. Beta would only penetrate a few millimetres into the food.
Why doesn't food become radioactive? Gamma radiation is electromagnetic energy, not particles of matter. When gamma rays pass through food, they kill bacteria by damaging their DNA, but they do not add any radioactive atoms to the food. Irradiation does not mean contamination!
Why cobalt-60? Its half-life of 5.3 years is long enough that the source lasts for a useful period before needing replacement, but not so long that it becomes a permanent waste disposal problem. A very short half-life would mean the source loses its activity too quickly to be practical.
Connect to the Syllabus
This scenario tests three important concepts: (1) why gamma is used (high penetrating power to reach all parts of the food through packaging), (2) why alpha and beta would not work (stopped before reaching the food or not penetrating enough), and (3) why a long half-life is needed (source must last for practical use). Remember: irradiation and contamination are different -- irradiation passes energy through the food, contamination means radioactive material is added to the food.
Aha! Moment
India is one of the largest users of food irradiation in Asia! The BARC in Mumbai developed the technology for irradiating onions and spices. Next time you buy packaged spices, look for the "Radura" symbol (a green flower-like logo) -- it means the food has been irradiated for safety. It is completely safe to eat! The irradiated food does not become radioactive, just like you do not become radioactive after an X-ray at the hospital. The gamma rays kill bacteria and then the energy passes through -- nothing radioactive stays in the food.
3
Tara's building in Bangalore has smoke detectors in the corridor. Her father tells her they contain a tiny amount of americium-241 (Am-241), which emits alpha particles. The alpha particles ionise the air between two metal plates, creating a small electric current. When smoke enters, it absorbs the alpha particles, the current drops, and the alarm sounds.
Why must the source emit alpha particles (not beta or gamma)? Am-241 has a half-life of 432 years -- why is this important? Is the smoke detector dangerous to have in your home?
▼
Identify the Physics
This is about the application of alpha radiation in smoke detectors and choosing the right isotope based on radiation type and half-life.
Work It Out
Why alpha? Alpha particles are the most ionising type of radiation. They are very effective at ionising the air molecules between the plates, creating a reliable current. Also, alpha is stopped by just a few centimetres of air, so the radiation stays inside the detector and does not escape to harm anyone. Beta or gamma would be too penetrating -- they would pass through the smoke without being absorbed, so the current would not drop when smoke enters.
Why a 432-year half-life? A long half-life means the source stays active for decades without needing replacement. The smoke detector will work for the entire lifetime of the building. If the half-life were short (say, a few days), the source would decay quickly and the detector would stop working.
Is it dangerous? No! The amount of Am-241 is incredibly tiny (about 1 microgram). Alpha particles cannot penetrate your skin or even travel more than a few centimetres in air. The detector is completely safe as long as you do not break it open and inhale or swallow the source material.
Connect to the Syllabus
This is a classic exam question about choosing the right isotope for an application. You need to explain: (1) why alpha is used (most ionising, creates current in air, stopped within the detector so safe), (2) why beta and gamma would not work (not ionising enough, or would pass through smoke without being absorbed), and (3) why a long half-life is needed (no frequent replacement). This also connects to safety -- the source is safe because alpha cannot penetrate skin.
Aha! Moment
The tiny Am-241 source in a smoke detector gives off about the same radiation as eating one banana! You receive more radiation from a single X-ray at the hospital than from living with a smoke detector for your entire life. The safety risk is essentially zero, but the fire-detection benefit has saved millions of lives worldwide. When disposing of old smoke detectors, they should be returned to the manufacturer or a proper waste facility -- do not throw them in regular rubbish!
4
A group of trekkers is planning a trip to Pangong Lake in Ladakh (altitude: about 4,350 metres). Their guide tells them that at this altitude, they will receive more cosmic radiation than at sea level because there is less atmosphere above them to block it. At sea level, about 300 metres of atmosphere shields us.
Cosmic rays are a source of background radiation. Why do people at high altitudes like Ladakh receive more cosmic radiation? Is the extra exposure dangerous for a short trek?
▼
Identify the Physics
This is about cosmic rays as a source of background radiation and how the atmosphere acts as a natural shield.
Work It Out
Cosmic rays are high-energy particles (mainly protons) that come from outer space. When they hit the Earth's atmosphere, they collide with air molecules and produce showers of secondary particles. The atmosphere acts as a shield, absorbing many of these particles before they reach ground level. At sea level, you have the full thickness of the atmosphere protecting you. At 4,350 metres in Ladakh, there is less atmosphere above you, so more cosmic radiation reaches you. At this altitude, the cosmic radiation exposure is roughly 2-3 times higher than at sea level.
For a short trek (a few days or weeks), the extra dose is tiny and not dangerous at all. Even airline pilots and flight attendants who fly at 10,000+ metres regularly throughout their careers receive only slightly elevated doses. The risk from a short trek is negligible compared to everyday risks.
Connect to the Syllabus
This scenario connects to background radiation -- specifically cosmic rays as one of the natural sources. The atmosphere acts as natural shielding (one of the three safety principles: shielding). At higher altitudes, there is less shielding, so more cosmic radiation reaches you. Astronauts on the International Space Station receive even more cosmic radiation because they are above most of the atmosphere.
Aha! Moment
When you fly from Bangalore to Delhi at 10,000 metres altitude, you receive about 5 times more cosmic radiation than on the ground -- but the total dose for a 2-hour flight is still only about the same as one chest X-ray. The atmosphere is an incredible natural shield! Without it, life on Earth would not exist because cosmic radiation would be too intense. This is also why astronauts on the ISS need special shielding, and why Mars colonisation is so challenging -- Mars has a very thin atmosphere and no magnetic field to deflect charged cosmic ray particles.
5
At Tata Memorial Hospital in Mumbai, doctors use technetium-99m (Tc-99m) for medical imaging. A patient is injected with a small amount of Tc-99m, which emits gamma rays. A special camera outside the body detects these gamma rays and builds up an image of where the tracer has concentrated. Tc-99m has a half-life of 6 hours. If a patient is injected at 8:00 AM with a dose giving an activity of 800 MBq, the doctors need the scan done before the activity drops too low.
Why is gamma radiation ideal for medical imaging (not alpha or beta)? What will the activity be at 8:00 PM the same day? Why is a 6-hour half-life good for this purpose?
▼
Identify the Physics
This combines the application of gamma radiation in medical imaging with a half-life calculation.
Work It Out
Why gamma? Gamma rays have no charge and no mass, so they can pass out of the body without being absorbed. This means the camera outside the body can detect them. Alpha particles would be completely stopped inside the body (they cannot even penetrate skin), so they could never reach an external detector. Beta would also be mostly absorbed. Worse, alpha and beta radiation absorbed inside the body would cause much more biological damage because they are more ionising.
Activity at 8:00 PM: Time elapsed = 8:00 AM to 8:00 PM = 12 hours. Number of half-lives = 12 / 6 = 2 half-lives. 800 → 400 (after 1 half-life, at 2:00 PM) → 200 (after 2 half-lives, at 8:00 PM). Activity at 8:00 PM = 200 MBq.
Why 6 hours? It is short enough that the patient is not radioactive for long -- by the next day, after about 4 half-lives (24 hours), the activity has dropped to 800/16 = 50 MBq, which is very low. But 6 hours is long enough to give doctors time to prepare and complete the scan. A half-life of seconds would be useless (decays before the scan). A half-life of years would leave the patient radioactive for far too long.
Connect to the Syllabus
This scenario brings together several key concepts: choosing the right radiation type for an application (gamma for medical tracers because it can escape the body), choosing the right half-life (short for patient safety, long enough for the procedure), and half-life calculations (halving the activity repeatedly). In the exam, you might be asked to calculate the activity at various times, or explain why gamma is used instead of alpha or beta.
Aha! Moment
Tc-99m is the most widely used radioactive tracer in medicine worldwide -- about 40 million procedures per year! India produces Tc-99m at the BARC reactor in Mumbai. The "m" in Tc-99m stands for "metastable," meaning the nucleus is in an excited state and releases gamma rays as it settles down. It is a perfect medical tool: gamma for easy detection, short half-life for patient safety, and it naturally concentrates in different organs depending on the chemical it is attached to. Tata Memorial Hospital in Mumbai is one of India's leading cancer treatment centres, and nuclear medicine plays a crucial role in diagnosing and treating cancer patients.
Practice Questions: Section 5.2
Test your understanding of radioactivity, decay, half-life, and safety.
Score0 / 20
QUESTION 1
Which of the following is the biggest source of natural background radiation for most people?
A. Radon gas from rocks and soil
B. Cosmic rays from space
C. Medical X-rays
D. Nuclear power plants
Radon gas is the single largest source of background radiation for most people. It seeps out of rocks and soil and can accumulate in buildings. It accounts for about 50% of average background radiation exposure.
QUESTION 2
A Geiger-Muller tube detects a count rate of 360 counts/min from a source. The background count rate is 40 counts/min. What is the corrected count rate?
A. 400 counts/min
B. 320 counts/min
C. 360 counts/min
D. 180 counts/min
Corrected count rate = measured count rate - background = 360 - 40 = 320 counts/min. Always subtract the background to find the count rate from the source alone.
QUESTION 3
An alpha particle consists of:
A. 2 protons only
B. 2 electrons and 2 neutrons
C. 2 protons and 2 neutrons
D. 4 protons
An alpha particle is identical to a helium-4 nucleus: 2 protons and 2 neutrons. It has a charge of +2 and a mass number of 4. It is written as 42He.
QUESTION 4
Which type of radiation is stopped by a few sheets of paper?
A. Alpha
B. Beta
C. Gamma
D. All of the above
Alpha particles are the least penetrating type of radiation. They are stopped by a few sheets of paper or a few centimetres of air. Beta passes through paper but is stopped by aluminium. Gamma passes through both and needs thick lead or concrete.
QUESTION 5
Radioactive decay is described as spontaneous and random. This means:
A. It can be started by heating the source
B. All nuclei in a sample decay at the same time
C. It cannot be predicted which nucleus will decay next, and it happens without any trigger
D. It only happens when radiation hits the nucleus
"Spontaneous" means it happens on its own without any external cause -- you cannot speed it up or slow it down by changing temperature, pressure, or anything else. "Random" means you cannot predict which particular nucleus will decay next, or exactly when.
QUESTION 6
When a nucleus undergoes beta decay, what happens to the proton number and nucleon number?
A. Proton number decreases by 1, nucleon number decreases by 1
B. Proton number increases by 1, nucleon number stays the same
C. Proton number stays the same, nucleon number decreases by 1
D. Proton number increases by 2, nucleon number increases by 4
In beta decay, a neutron converts into a proton + electron. The electron (beta particle) is emitted. So: one more proton (Z increases by 1), one fewer neutron, but the total nucleons (protons + neutrons) stays the same (A unchanged).
QUESTION 7
Polonium-210 (21084Po) undergoes alpha decay. What is the daughter nucleus?
A.21085At
B.20884Po
C.20682Pb
D.20684Po
Alpha decay: A decreases by 4, Z decreases by 2. New A = 210 - 4 = 206. New Z = 84 - 2 = 82. Element 82 is lead (Pb). So the daughter is 20682Pb.
QUESTION 8
A radioactive sample has a half-life of 5 hours. If the initial activity is 3200 counts/min, what will the activity be after 20 hours?
A. 800 counts/min
B. 400 counts/min
C. 200 counts/min
D. 100 counts/min
Number of half-lives = 20 / 5 = 4. Halve 4 times: 3200 → 1600 → 800 → 400 → 200. The activity after 20 hours is 200 counts/min.
QUESTION 9
Which type of radiation causes the most ionisation per unit distance travelled?
A. Alpha
B. Beta
C. Gamma
D. They all ionise equally
Alpha particles are the most ionising because they have the largest charge (+2) and move the slowest. Their large charge means they interact strongly with atoms they pass, and their slow speed means they spend more time near each atom, giving them more opportunity to knock out electrons.
QUESTION 10
In a beta decay, the particle emitted from the nucleus is:
A. A proton
B. A neutron
C. A fast-moving electron
D. An electromagnetic wave
A beta particle is a fast-moving electron that is created inside the nucleus when a neutron changes into a proton and an electron. The electron is then ejected from the nucleus at high speed. Note: this is NOT an orbital electron -- it comes from inside the nucleus.
QUESTION 11
When radiation passes between charged plates in an electric field, gamma rays:
A. Bend towards the positive plate
B. Bend towards the negative plate
C. Pass straight through without deflection
D. Are absorbed by the plates
Gamma rays have no charge and no mass, so they are not affected by electric or magnetic fields. They pass straight through without any deflection. Alpha particles bend towards the negative plate (because alpha is positive), and beta particles bend towards the positive plate (because beta is negative).
QUESTION 12
Which isotope and radiation type is used in smoke detectors?
A. Cobalt-60, gamma
B. Americium-241, alpha
C. Technetium-99m, gamma
D. Strontium-90, beta
Smoke detectors use americium-241, which emits alpha particles. Alpha is ideal because it ionises the air to create a current, and is easily absorbed by smoke particles. Am-241 has a half-life of 432 years, so it works for the lifetime of the detector.
QUESTION 13
When a nucleus emits a gamma ray, the proton number and nucleon number:
A. Both decrease
B. Both increase
C. Both stay the same
D. Proton number increases, nucleon number decreases
Gamma emission is the release of electromagnetic energy from the nucleus. No particles are emitted, so no protons or neutrons leave the nucleus. Both A and Z remain unchanged. The element does not change -- the nucleus simply loses excess energy.
QUESTION 14
For measuring the thickness of paper in a paper mill, which type of radiation should be used?
A. Alpha (it would be completely stopped by any thickness)
B. Beta (it is partially absorbed by paper, so changes in thickness are detectable)
C. Gamma (it passes through paper with almost no absorption)
D. Any type would work equally well
Beta radiation is ideal for paper thickness measurement because it is partially absorbed by paper. If the paper is too thick, less beta gets through; too thin, and more gets through. A detector measures the transmitted radiation and adjusts the rollers. Alpha would be fully stopped by any paper. Gamma would pass through without significant change regardless of thickness.
QUESTION 15
A sample starts with 4000 undecayed nuclei. After 3 half-lives, how many undecayed nuclei remain?
A. 1000
B. 500
C. 250
D. 2000
After each half-life, the number halves. After 1: 4000/2 = 2000. After 2: 2000/2 = 1000. After 3: 1000/2 = 500. So 500 undecayed nuclei remain after 3 half-lives.
QUESTION 16
Ionising radiation can be dangerous because it can:
A. Make objects magnetic
B. Create new elements in your body
C. Damage DNA, causing mutations and cancer
D. Make your body radioactive permanently
Ionising radiation knocks electrons off atoms in living cells. When this happens to atoms in DNA molecules, the chemical bonds can break. This can cause mutations (changes in DNA) that may lead to uncontrolled cell growth -- cancer. High doses can also directly kill cells.
QUESTION 17
Which of the following is a correct safety precaution when handling radioactive sources in a school lab?
A. Wear rubber gloves to block all radiation
B. Use long tongs and keep exposure time short
C. Hold the source close to your body for a clear reading
D. Store sources on an open shelf for easy access
The correct precautions include: use long tongs (increases distance from source), minimise exposure time, store sources in lead-lined containers, and point sources away from people. Rubber gloves would stop alpha but not beta or gamma. Sources should never be held close to the body.
QUESTION 18
Technetium-99m is used as a medical tracer. Its half-life of 6 hours is ideal because:
A. It gives doctors years to complete the scan
B. It is long enough for the scan but short enough that the patient is not radioactive for long
C. It decays so fast the patient gets no radiation at all
D. The half-life does not matter for medical tracers
A 6-hour half-life is ideal: long enough to give doctors time to prepare and perform the scan (several hours), but short enough that the activity drops to very low levels within a day or two, minimising the patient's radiation exposure. A half-life of seconds would decay too fast; years would leave the patient radioactive too long.
QUESTION 19
Nitrogen-13 (137N) undergoes beta decay. What is the daughter nucleus?
A.136C
B.138O
C.95B
D.127N
Beta decay: A stays the same, Z increases by 1. New A = 13 (unchanged). New Z = 7 + 1 = 8. Element 8 is oxygen (O). So the daughter is 138O.
QUESTION 20
The three principles for reducing radiation exposure are:
A. Heat, pressure, and volume
B. Speed, mass, and charge
C. Reduce time, increase distance, use shielding
D. Wear gloves, use a mask, work outdoors
The three key safety principles are: (1) Reduce TIME near the source, (2) Increase DISTANCE from the source (radiation intensity decreases with distance), and (3) Use appropriate SHIELDING (e.g., lead for gamma, aluminium for beta). Remember: T-D-S (Time, Distance, Shielding).