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Understanding Particles and Radiation in Physics

3

0

T

thressi kutty

06/12/2025

Physics

Particles and Radiation

87

6 Dec 2025

10 pages

Understanding Particles and Radiation in Physics

T

thressi kutty

@thressikutty_naiu

Atomic physics covers the fundamental building blocks of matter and... Show more

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3.2.1.1
Isotope → A form of an
atom with same.
but
a different number.
neutrons.
Carbon-14-a radioactive
isotope of carbon.
Can be used to a

Atomic Structure and Isotopes

Your atoms are made of three key particles: protons (positive charge), neutrons (no charge), and electrons (negative charge). The protons and neutrons hang out together in the nucleus, whilst electrons orbit around in energy levels.

Isotopes are atoms of the same element with different numbers of neutrons. Carbon-14 is a famous radioactive isotope used for carbon dating - it helps archaeologists figure out how old ancient objects are by measuring how much carbon-14 has decayed over time.

Specific charge is simply the ratio of an object's charge to its mass measuredinC/kgmeasured in C/kg. You'll need to calculate this for different particles using the formula: specific charge = charge ÷ mass. Remember that protons and electrons have equal but opposite charges, whilst neutrons are electrically neutral.

Key Point: The notation ᴬzX tells you everything - A is the mass number protons+neutronsprotons + neutrons, Z is the atomic number (just protons), and X is the element symbol.

3.2.1.1
Isotope → A form of an
atom with same.
but
a different number.
neutrons.
Carbon-14-a radioactive
isotope of carbon.
Can be used to a

Radioactive Decay and Nuclear Forces

Unstable nuclei undergo radioactive decay to become more stable, and there are three main types you need to know. Alpha decay shoots out a helium nucleus 2protons+2neutrons2 protons + 2 neutrons, beta-minus decay turns a neutron into a proton whilst emitting an electron, and beta-plus decay converts a proton into a neutron whilst releasing a positron.

The strong nuclear force is what keeps the nucleus together despite all those positively charged protons trying to repel each other. It's incredibly powerful but only works over tiny distances - between about 0.5 and 3 femtometres. Any closer than 0.5 fm and it actually becomes repulsive, preventing the nucleus from collapsing.

During beta decay, scientists noticed that energy seemed to disappear, which led to the discovery of neutrinos - nearly massless particles that barely interact with anything. They're essential for conserving energy and momentum in these reactions.

Remember: In alpha decay, both the mass number drops by 4 and the atomic number drops by 2, whilst in beta decay, the mass number stays the same but the atomic number changes by ±1.

3.2.1.1
Isotope → A form of an
atom with same.
but
a different number.
neutrons.
Carbon-14-a radioactive
isotope of carbon.
Can be used to a

Photons and Antimatter

Every particle has a corresponding antiparticle with the same mass but opposite charge - like electrons and positrons. When they meet, they completely destroy each other in an annihilation reaction, converting all their mass into energy as two photons that fly off in opposite directions.

Pair production is the reverse process where a high-energy photon interacts with a nucleus and creates a particle-antiparticle pair. For this to happen, the photon needs at least twice the rest energy of the particles being created minimumenergy=2Erestminimum energy = 2E_rest.

Photons are packets of electromagnetic energy with energy E = hf (where h is Planck's constant and f is frequency). You can also use E = hc/λ when you know the wavelength instead. These massless particles carry the electromagnetic force and always travel at the speed of light.

Energy Conservation: In pair production, any excess energy above the minimum becomes kinetic energy of the created particles: hf = 2E_rest + KE.

3.2.1.1
Isotope → A form of an
atom with same.
but
a different number.
neutrons.
Carbon-14-a radioactive
isotope of carbon.
Can be used to a

Particle Interactions and Exchange Particles

The universe has four fundamental forces: strong nuclear, electromagnetic, weak nuclear, and gravity. Each force is carried by special particles called gauge bosons - think of them as messengers that transfer energy and momentum between particles.

Feynman diagrams are brilliant visual tools that show how particles interact over time (time goes upwards, position goes sideways). In beta decay, a W boson mediates the interaction that converts a neutron to a proton or vice versa. The size of the exchange particle determines the range of the force - bigger particles mean shorter ranges.

Electron capture happens when a proton grabs an inner electron and transforms into a neutron, releasing an electron neutrino. This process involves the weak nuclear force and W bosons, just like other beta decay processes.

The weak nuclear force affects all types of particles and is responsible for radioactive decay processes. Unlike the strong force, it can change one type of particle into another completely.

Force Carriers: Virtual photons carry electromagnetic force, W and Z bosons carry weak force, gluons carry strong force, and gravitons (theoretical) carry gravity.

3.2.1.1
Isotope → A form of an
atom with same.
but
a different number.
neutrons.
Carbon-14-a radioactive
isotope of carbon.
Can be used to a

Classification of Matter

All matter divides into two main categories: hadrons (made of quarks) and leptons (fundamental particles). Hadrons feel the strong nuclear force because they contain quarks, whilst leptons don't experience this force at all.

Hadrons split into two groups: baryons (made of three quarks, like protons and neutrons) and mesons madeofaquarkantiquarkpair,likepionsandkaonsmade of a quark-antiquark pair, like pions and kaons. These particles can interact through the strong force and are generally more massive than leptons.

Leptons include familiar particles like electrons and neutrinos, plus their more exotic cousins like muons. These are truly fundamental - they can't be broken down into smaller components and only interact through electromagnetic, weak, and gravitational forces.

Each particle type has its own antiparticle with identical mass but opposite charge and other quantum numbers. When matter meets antimatter, they annihilate completely, releasing pure energy.

Memory Tip: Think "LEPtons are LIGHTweight and LEft alone by the strong force" - they don't experience strong nuclear interactions.

3.2.1.1
Isotope → A form of an
atom with same.
but
a different number.
neutrons.
Carbon-14-a radioactive
isotope of carbon.
Can be used to a

Conservation Laws and Quarks

Conservation laws are the universe's accounting rules - certain quantities must balance before and after any interaction. Energy, momentum, charge, and baryon number are always conserved, whilst strangeness is only conserved in strong interactions.

Strange particles contain strange quarks and have non-zero strangeness values. They're created in pairs through strong interactions (to conserve strangeness) but decay individually through weak interactions wherestrangenesscanchangeby0,+1,or1where strangeness can change by 0, +1, or -1.

Quarks are the building blocks of hadrons and come in six flavours, but you mainly need to know up, down, and strange quarks for A-level. They combine in groups of three (baryons) or quark-antiquark pairs (mesons) - you never find isolated quarks in nature.

Different lepton numbers exist for each lepton family: electron number LeL_e and muon number LμL_μ. These are conserved in all interactions, helping you predict what particles can be produced in various processes.

Strangeness Rule: Strange particles are always produced in pairs (to conserve strangeness) but can decay alone because weak interactions allow strangeness to change.

3.2.1.1
Isotope → A form of an
atom with same.
but
a different number.
neutrons.
Carbon-14-a radioactive
isotope of carbon.
Can be used to a

Wave-Particle Duality

Everything in the universe exhibits wave-particle duality - particles can behave like waves and waves can behave like particles. This isn't just theoretical; it's a fundamental property of matter and energy that you can observe in experiments.

The de Broglie wavelength λ=h/mvλ = h/mv tells you the wavelength associated with any moving particle. Electrons, protons, even entire atoms have wavelengths, though they're incredibly tiny for large objects. This explains why you don't notice the wave properties of everyday objects.

Light demonstrates this duality perfectly: the photoelectric effect shows light's particle nature (photons), whilst diffraction experiments reveal its wave properties. Both aspects are real and fundamental to how electromagnetic radiation behaves.

Scale Matters: Wave properties become noticeable when the de Broglie wavelength is similar to the size of obstacles or gaps the particle encounters.

3.2.1.1
Isotope → A form of an
atom with same.
but
a different number.
neutrons.
Carbon-14-a radioactive
isotope of carbon.
Can be used to a

The Photoelectric Effect

When light hits a metal surface, it can knock electrons out - but only if the light's frequency is high enough. This threshold frequency depends on the metal's work function (φ) - the minimum energy needed to free an electron from the metal's surface.

The photoelectric equation E = hf = φ + E_k(max) explains everything. Each photon gives all its energy (hf) to one electron: some energy overcomes the work function, and any leftover becomes the electron's kinetic energy.

Stopping potential VsV_s is the voltage needed to stop the fastest photoelectrons, related to their maximum kinetic energy by E_k(max) = eV_s. This lets you measure the electrons' energy experimentally and verify Einstein's photon model.

Increasing light intensity (keeping frequency constant) produces more photoelectrons per second but doesn't change their individual energies. Only increasing frequency gives each electron more kinetic energy.

Counter-intuitive: Bright red light won't eject electrons from zinc, but dim ultraviolet light will - frequency matters more than intensity for the photoelectric effect.

3.2.1.1
Isotope → A form of an
atom with same.
but
a different number.
neutrons.
Carbon-14-a radioactive
isotope of carbon.
Can be used to a

Energy Levels and Spectra

Electrons in atoms can only exist at specific discrete energy levels - they can't hang around anywhere in between. When electrons jump between these levels, they absorb or emit photons with energies exactly equal to the energy difference between levels.

Line spectra provide brilliant evidence for these energy levels. Each bright or dark line corresponds to a specific photon frequency, showing that electrons can only make certain allowed transitions. No in-between energies appear because no in-between levels exist.

Ionisation energy is the energy needed to completely remove an electron from an atom's ground state (lowest energy level). Different elements have different ionisation energies because their electron arrangements vary.

The patterns in atomic spectra are unique to each element, making spectroscopy a powerful tool for identifying substances. Astronomers use this to determine what distant stars are made of just by analysing their light.

Think of it like stairs: Electrons can only stand on the steps (energy levels), never floating between them - and they emit or absorb specific amounts of energy when changing steps.

3.2.1.1
Isotope → A form of an
atom with same.
but
a different number.
neutrons.
Carbon-14-a radioactive
isotope of carbon.
Can be used to a

Electron Collisions and Excitation

When fast-moving electrons collide with atoms, they can transfer energy to the atom's electrons, causing excitation - bumping electrons up to higher energy levels. The excited electrons quickly fall back down, releasing photons as they cascade through the energy levels.

Electron volts (eV) are handy energy units in atomic physics. One eV equals 1.6 × 10⁻¹⁹ joules - it's the kinetic energy gained by an electron accelerated through a 1V potential difference. Convert between eV and joules by multiplying or dividing by 1.6 × 10⁻¹⁹.

If the colliding electron has enough energy (greater than the ionisation energy), it can completely knock an electron out of the atom, creating an ion. This process requires more energy than just exciting electrons to higher levels.

Fluorescent tubes demonstrate these principles perfectly: high voltage accelerates electrons that collide with mercury atoms, exciting them to emit UV light. The phosphor coating then absorbs the UV and re-emits visible light through its own excitation process.

Energy Threshold: Excitation and ionisation only happen when the colliding electron has at least the exact energy needed - there's no partial credit in quantum mechanics!



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Physics

87

6 Dec 2025

10 pages

Understanding Particles and Radiation in Physics

T

thressi kutty

@thressikutty_naiu

Atomic physics covers the fundamental building blocks of matter and how they behave. You'll explore everything from the structure of atoms and radioactive decay to the dual nature of light and matter, plus some fascinating quantum effects that explain how... Show more

3.2.1.1
Isotope → A form of an
atom with same.
but
a different number.
neutrons.
Carbon-14-a radioactive
isotope of carbon.
Can be used to a

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Atomic Structure and Isotopes

Your atoms are made of three key particles: protons (positive charge), neutrons (no charge), and electrons (negative charge). The protons and neutrons hang out together in the nucleus, whilst electrons orbit around in energy levels.

Isotopes are atoms of the same element with different numbers of neutrons. Carbon-14 is a famous radioactive isotope used for carbon dating - it helps archaeologists figure out how old ancient objects are by measuring how much carbon-14 has decayed over time.

Specific charge is simply the ratio of an object's charge to its mass measuredinC/kgmeasured in C/kg. You'll need to calculate this for different particles using the formula: specific charge = charge ÷ mass. Remember that protons and electrons have equal but opposite charges, whilst neutrons are electrically neutral.

Key Point: The notation ᴬzX tells you everything - A is the mass number protons+neutronsprotons + neutrons, Z is the atomic number (just protons), and X is the element symbol.

3.2.1.1
Isotope → A form of an
atom with same.
but
a different number.
neutrons.
Carbon-14-a radioactive
isotope of carbon.
Can be used to a

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Radioactive Decay and Nuclear Forces

Unstable nuclei undergo radioactive decay to become more stable, and there are three main types you need to know. Alpha decay shoots out a helium nucleus 2protons+2neutrons2 protons + 2 neutrons, beta-minus decay turns a neutron into a proton whilst emitting an electron, and beta-plus decay converts a proton into a neutron whilst releasing a positron.

The strong nuclear force is what keeps the nucleus together despite all those positively charged protons trying to repel each other. It's incredibly powerful but only works over tiny distances - between about 0.5 and 3 femtometres. Any closer than 0.5 fm and it actually becomes repulsive, preventing the nucleus from collapsing.

During beta decay, scientists noticed that energy seemed to disappear, which led to the discovery of neutrinos - nearly massless particles that barely interact with anything. They're essential for conserving energy and momentum in these reactions.

Remember: In alpha decay, both the mass number drops by 4 and the atomic number drops by 2, whilst in beta decay, the mass number stays the same but the atomic number changes by ±1.

3.2.1.1
Isotope → A form of an
atom with same.
but
a different number.
neutrons.
Carbon-14-a radioactive
isotope of carbon.
Can be used to a

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Photons and Antimatter

Every particle has a corresponding antiparticle with the same mass but opposite charge - like electrons and positrons. When they meet, they completely destroy each other in an annihilation reaction, converting all their mass into energy as two photons that fly off in opposite directions.

Pair production is the reverse process where a high-energy photon interacts with a nucleus and creates a particle-antiparticle pair. For this to happen, the photon needs at least twice the rest energy of the particles being created minimumenergy=2Erestminimum energy = 2E_rest.

Photons are packets of electromagnetic energy with energy E = hf (where h is Planck's constant and f is frequency). You can also use E = hc/λ when you know the wavelength instead. These massless particles carry the electromagnetic force and always travel at the speed of light.

Energy Conservation: In pair production, any excess energy above the minimum becomes kinetic energy of the created particles: hf = 2E_rest + KE.

3.2.1.1
Isotope → A form of an
atom with same.
but
a different number.
neutrons.
Carbon-14-a radioactive
isotope of carbon.
Can be used to a

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Particle Interactions and Exchange Particles

The universe has four fundamental forces: strong nuclear, electromagnetic, weak nuclear, and gravity. Each force is carried by special particles called gauge bosons - think of them as messengers that transfer energy and momentum between particles.

Feynman diagrams are brilliant visual tools that show how particles interact over time (time goes upwards, position goes sideways). In beta decay, a W boson mediates the interaction that converts a neutron to a proton or vice versa. The size of the exchange particle determines the range of the force - bigger particles mean shorter ranges.

Electron capture happens when a proton grabs an inner electron and transforms into a neutron, releasing an electron neutrino. This process involves the weak nuclear force and W bosons, just like other beta decay processes.

The weak nuclear force affects all types of particles and is responsible for radioactive decay processes. Unlike the strong force, it can change one type of particle into another completely.

Force Carriers: Virtual photons carry electromagnetic force, W and Z bosons carry weak force, gluons carry strong force, and gravitons (theoretical) carry gravity.

3.2.1.1
Isotope → A form of an
atom with same.
but
a different number.
neutrons.
Carbon-14-a radioactive
isotope of carbon.
Can be used to a

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Classification of Matter

All matter divides into two main categories: hadrons (made of quarks) and leptons (fundamental particles). Hadrons feel the strong nuclear force because they contain quarks, whilst leptons don't experience this force at all.

Hadrons split into two groups: baryons (made of three quarks, like protons and neutrons) and mesons madeofaquarkantiquarkpair,likepionsandkaonsmade of a quark-antiquark pair, like pions and kaons. These particles can interact through the strong force and are generally more massive than leptons.

Leptons include familiar particles like electrons and neutrinos, plus their more exotic cousins like muons. These are truly fundamental - they can't be broken down into smaller components and only interact through electromagnetic, weak, and gravitational forces.

Each particle type has its own antiparticle with identical mass but opposite charge and other quantum numbers. When matter meets antimatter, they annihilate completely, releasing pure energy.

Memory Tip: Think "LEPtons are LIGHTweight and LEft alone by the strong force" - they don't experience strong nuclear interactions.

3.2.1.1
Isotope → A form of an
atom with same.
but
a different number.
neutrons.
Carbon-14-a radioactive
isotope of carbon.
Can be used to a

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Conservation Laws and Quarks

Conservation laws are the universe's accounting rules - certain quantities must balance before and after any interaction. Energy, momentum, charge, and baryon number are always conserved, whilst strangeness is only conserved in strong interactions.

Strange particles contain strange quarks and have non-zero strangeness values. They're created in pairs through strong interactions (to conserve strangeness) but decay individually through weak interactions wherestrangenesscanchangeby0,+1,or1where strangeness can change by 0, +1, or -1.

Quarks are the building blocks of hadrons and come in six flavours, but you mainly need to know up, down, and strange quarks for A-level. They combine in groups of three (baryons) or quark-antiquark pairs (mesons) - you never find isolated quarks in nature.

Different lepton numbers exist for each lepton family: electron number LeL_e and muon number LμL_μ. These are conserved in all interactions, helping you predict what particles can be produced in various processes.

Strangeness Rule: Strange particles are always produced in pairs (to conserve strangeness) but can decay alone because weak interactions allow strangeness to change.

3.2.1.1
Isotope → A form of an
atom with same.
but
a different number.
neutrons.
Carbon-14-a radioactive
isotope of carbon.
Can be used to a

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Wave-Particle Duality

Everything in the universe exhibits wave-particle duality - particles can behave like waves and waves can behave like particles. This isn't just theoretical; it's a fundamental property of matter and energy that you can observe in experiments.

The de Broglie wavelength λ=h/mvλ = h/mv tells you the wavelength associated with any moving particle. Electrons, protons, even entire atoms have wavelengths, though they're incredibly tiny for large objects. This explains why you don't notice the wave properties of everyday objects.

Light demonstrates this duality perfectly: the photoelectric effect shows light's particle nature (photons), whilst diffraction experiments reveal its wave properties. Both aspects are real and fundamental to how electromagnetic radiation behaves.

Scale Matters: Wave properties become noticeable when the de Broglie wavelength is similar to the size of obstacles or gaps the particle encounters.

3.2.1.1
Isotope → A form of an
atom with same.
but
a different number.
neutrons.
Carbon-14-a radioactive
isotope of carbon.
Can be used to a

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The Photoelectric Effect

When light hits a metal surface, it can knock electrons out - but only if the light's frequency is high enough. This threshold frequency depends on the metal's work function (φ) - the minimum energy needed to free an electron from the metal's surface.

The photoelectric equation E = hf = φ + E_k(max) explains everything. Each photon gives all its energy (hf) to one electron: some energy overcomes the work function, and any leftover becomes the electron's kinetic energy.

Stopping potential VsV_s is the voltage needed to stop the fastest photoelectrons, related to their maximum kinetic energy by E_k(max) = eV_s. This lets you measure the electrons' energy experimentally and verify Einstein's photon model.

Increasing light intensity (keeping frequency constant) produces more photoelectrons per second but doesn't change their individual energies. Only increasing frequency gives each electron more kinetic energy.

Counter-intuitive: Bright red light won't eject electrons from zinc, but dim ultraviolet light will - frequency matters more than intensity for the photoelectric effect.

3.2.1.1
Isotope → A form of an
atom with same.
but
a different number.
neutrons.
Carbon-14-a radioactive
isotope of carbon.
Can be used to a

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Energy Levels and Spectra

Electrons in atoms can only exist at specific discrete energy levels - they can't hang around anywhere in between. When electrons jump between these levels, they absorb or emit photons with energies exactly equal to the energy difference between levels.

Line spectra provide brilliant evidence for these energy levels. Each bright or dark line corresponds to a specific photon frequency, showing that electrons can only make certain allowed transitions. No in-between energies appear because no in-between levels exist.

Ionisation energy is the energy needed to completely remove an electron from an atom's ground state (lowest energy level). Different elements have different ionisation energies because their electron arrangements vary.

The patterns in atomic spectra are unique to each element, making spectroscopy a powerful tool for identifying substances. Astronomers use this to determine what distant stars are made of just by analysing their light.

Think of it like stairs: Electrons can only stand on the steps (energy levels), never floating between them - and they emit or absorb specific amounts of energy when changing steps.

3.2.1.1
Isotope → A form of an
atom with same.
but
a different number.
neutrons.
Carbon-14-a radioactive
isotope of carbon.
Can be used to a

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Electron Collisions and Excitation

When fast-moving electrons collide with atoms, they can transfer energy to the atom's electrons, causing excitation - bumping electrons up to higher energy levels. The excited electrons quickly fall back down, releasing photons as they cascade through the energy levels.

Electron volts (eV) are handy energy units in atomic physics. One eV equals 1.6 × 10⁻¹⁹ joules - it's the kinetic energy gained by an electron accelerated through a 1V potential difference. Convert between eV and joules by multiplying or dividing by 1.6 × 10⁻¹⁹.

If the colliding electron has enough energy (greater than the ionisation energy), it can completely knock an electron out of the atom, creating an ion. This process requires more energy than just exciting electrons to higher levels.

Fluorescent tubes demonstrate these principles perfectly: high voltage accelerates electrons that collide with mercury atoms, exciting them to emit UV light. The phosphor coating then absorbs the UV and re-emits visible light through its own excitation process.

Energy Threshold: Excitation and ionisation only happen when the colliding electron has at least the exact energy needed - there's no partial credit in quantum mechanics!

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