OCR A-Level Physics B H557
Planning
Implementing
Analysis
Evaluation
Practical Skills
Use of Apparatus and Techniques
Fundamental Data Analysis
Imaging and Signalling
Sensing
Mechanical Properties of Materials
Waves and Quantum Behaviour
Space, Time and Motion
Creating Models
Out Into Space
Our Place in the Universe
Matter: Very Simple
Matter: Hot or Cold
Electromagnetism
Charge and Field
Probing Deep Into Matter
Ionising Radiation and Risk
Probing Deep Into Matter
- 9 subtopics
- 27 things to know
- Components 01, 02 and 03
What Probing Deep Into Matter covers
Probing Deep Into Matter is examined in all three written papers — the specification states that Components 01, 02 and 03 each assess content from across all the teaching modules, so nothing is confined to one paper. It covers particle accelerators and high-energy beams, scattering and the nuclear atom, paths of scattered particles and closest approach, discrete energy levels in atoms, electron standing waves and the confined electron, quarks, hadrons and leptons, conservation laws and nuclear equations, charged particles in detectors and magnetic fields and relativistic energy and the relativistic factor.
Where it is assessed
Components 01, 02 and 03
Every module can be assessed on any of the three papers.
Check the OCR specification ↗The 9 subtopics
Each one has its own page.
- Particle accelerators and high-energy beamsRecall questions on why probing small structures needs high energy, how a linear accelerator works and why its voltage alternates, magnets and vacuum in a ring, and creating new particles.Open →
- Scattering and the nuclear atomRecall questions on the alpha-particle scattering arrangement, what most particles and a few particles did and what each shows, why a vacuum, a thin foil and gold were used, the sizes of atoms and nuclei and their volume ratio, the model it overturned, the negligible effect of electrons, high-energy electron scattering, and the nuclear atom as a model.Open →
- Paths of scattered particles and closest approachRecall questions on paths near and straight at a nucleus, the energy exchange on approach, calculating a closest approach, why it only bounds the nuclear radius, and how scattering varies with angle.Open →
- Discrete energy levels in atomsRecall questions on energy levels and the evidence of line spectra, ΔE = hf, frequency and wavelength calculations for a transition, absorption against emission spectra, electron collisions as evidence, electrons below the excitation energy, ionisation energy, negative energy values, ground and excited states, excitation against ionisation, and exciting an atom with a 10.4 V electron.Open →
- Electron standing waves and the confined electronRecall questions on why confinement gives discrete energies, the allowed wavelengths and resulting momentum and energy, nodes in higher states, why an atom has a definite size, and the model's limits.Open →
- Quarks, hadrons and leptonsRecall questions on the quark compositions and charges of protons, neutrons and antiprotons, the charges of up and down quarks, hadrons, leptons and gluons, antiparticles and the positron, lepton numbers, neutrinos and why they are hard to detect, why free quarks are never seen, and beta-minus decay at quark level.Open →
- Conservation laws and nuclear equationsRecall questions on the quantities that must balance, how alpha, beta and gamma emission change a nucleus, decay equations, annihilation and pair production, and why a further particle was proposed.Open →
- Charged particles in detectors and magnetic fieldsRecall questions on why tracks curve and what the curvature direction reveals, momentum from a track radius, tracks that spiral or appear from nowhere, invisible neutral particles, and charge-to-mass ratios.Open →
- Relativistic energy and the relativistic factorRecall questions on rest energy from rest mass, electron and proton values in MeV, evaluating the factor at high speeds, total and kinetic energy, and why no massive particle reaches light speed.Open →
What you need to know
Answer each one before you reveal it.
Why can a confined electron never have zero energy in this model?
Check that lepton number is conserved in the decay of a free neutron into a proton, an electron and an electron antineutrino.
Why must particles be given very high energies in order to probe small structures?
Describe the arrangement used in the alpha-particle scattering experiment.
How do line spectra provide evidence for discrete energy levels?
State the quark composition of a proton.
Why do the tracks of charged particles in a detector curve?
Write the relationship between the rest mass of a particle and its rest energy.
Calculate the de Broglie wavelength of a particle whose momentum is 1.0 × 10⁻²¹ N s.
What was the main observation in the alpha-scattering experiment?
Write the relationship used to calculate the distance of closest approach for a head-on collision.
Why is the emission spectrum of a gas a set of lines rather than a continuous band of colour?
Describe the simple model of an atom as an electron confined in a box.
State the quark composition of a neutron.
Name three quantities that must balance on both sides of a nuclear equation.
What quantity is obtained from the radius of a curved track in a known magnetic field?
Calculate the rest energy of an electron in joules.
Why must the accelerating voltage in a linear accelerator alternate?
What did a small number of the alpha particles do in the scattering experiment?
Calculate the charge on a gold nucleus, which has 79 protons.
Write the relationship between the energy difference of two levels and the frequency of the photon emitted.
Explain why confining an electron leads to a set of discrete energies.
State the charges of the up quark and the down quark.
What happens to the proton number and nucleon number of a nucleus when it emits an alpha particle?
A singly charged particle leaves a track of radius 0.25 m in a field of flux density 1.5 T. Calculate its momentum.
Express the rest energy of an electron in MeV.
Take Probing Deep Into Matter further
The same content, four other ways.
Commonly confused
Pairs that lose marks when they are blurred together.
Hadron vs Lepton
Hadron: a particle built from quarks and feeling the strong interaction, the proton and the neutron being the familiar examples. Lepton: a fundamental particle that is not made of quarks and takes no part in the strong interaction, such as the electron or the neutrino.
Excitation vs Ionisation
Excitation: lifting an electron to a higher level while it stays bound to the atom. Ionisation: giving an electron enough energy to escape the atom altogether, leaving the atom positively charged.
Rest energy vs Total energy
Rest energy: mc², what a particle has by virtue of its mass alone and the same whatever it is doing. Total energy: γmc², which already includes the kinetic contribution and grows without limit as the speed approaches c.
Questions from this topic
Each one with the model answer underneath.
- 1
Why must particles be given very high energies in order to probe small structures?
Model answer
The de Broglie wavelength of a particle is h/p, so only a large momentum gives a wavelength small enough to resolve detail on the scale of a nucleus or smaller.
- 2
Calculate the de Broglie wavelength of a particle whose momentum is 1.0 × 10⁻²¹ N s.
Model answer
λ = h/p = 6.63 × 10⁻³⁴ ÷ 1.0 × 10⁻²¹ = 6.6 × 10⁻¹³ m.
- 3
Describe how a linear accelerator increases the energy of a charged particle.
Model answer
The particle passes through a line of hollow electrodes and is accelerated across each gap by a potential difference, gaining energy qV at every gap so that its energy builds up along the line.
- 4
Why must the accelerating voltage in a linear accelerator alternate?
Model answer
The particle must always meet a field pointing the right way to speed it up, so the voltage on the electrodes has to reverse in step with the particle's arrival at each gap.
- 5
What is the role of magnetic fields in a ring accelerator?
Model answer
Magnetic fields provide the centripetal force through F = qvB that bends the beam round the ring, and further magnets focus the beam so it stays narrow.
- 6
Calculate the energy in joules gained by a proton accelerated through a potential difference of 2.0 × 10⁶ V.
Model answer
The energy gained is qV = 1.60 × 10⁻¹⁹ × 2.0 × 10⁶ = 3.2 × 10⁻¹³ J, which is 2.0 MeV.
What is inside Levo
Six ways to work the same material.
Probing Deep Into Matter revision questions
- What does Probing Deep Into Matter cover in OCR A-Level Physics B?
- 9 subtopics: particle accelerators and high-energy beams, scattering and the nuclear atom, paths of scattered particles and closest approach, discrete energy levels in atoms, electron standing waves and the confined electron, quarks, hadrons and leptons, conservation laws and nuclear equations, charged particles in detectors and magnetic fields and relativistic energy and the relativistic factor. Each one has its own page with questions and model answers.
- How is Probing Deep Into Matter organised?
- By the OCR H557 specification, subtopic by subtopic, so it matches the order you are taught it in.
Every question in Probing Deep Into Matter, on a schedule.
Attempt a question from memory, write the correct version, then attempt it again. Levo records the jump between your first attempt and your last, and brings each question back on the day you are due to forget it.
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