Atomic Structure, Radiation, and Nuclear Reactions

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Comprehensive practice flashcards covering atomic structure, radioactive decay, alpha, beta, and gamma radiation, background radiation, nuclear fission, and nuclear fusion.

100 Terms

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Background radiation

Weak radiation that can be detected from natural and man-made sources in the environment.

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Cosmic rays

A natural source of background radiation originating from outer space, contributing approximately 8%8\% to total background radiation.

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Radiation from underground rocks

A natural source of terrestrial background radiation that contributes approximately 8%8\% to overall background exposure.

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Nuclear fallout

A man-made source of background radiation resulting from past nuclear weapons testing or nuclear incidents.

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Medical rays

A man-made source of background radiation (such as diagnostic X-rays) contributing approximately 15%15\% of total background radiation.

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Radon

A radioactive gas originating naturally from rocks and soil that accounts for the largest proportion (54%54\%) of background radiation.

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Internal radiation

Natural background radiation originating from radioactive isotopes within the human body, contributing approximately 11%11\% of total exposure.

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Consumer products (radiation source)

A man-made source contributing approximately 3%3\% of the total background radiation dose.

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Other sources of radiation

Minor miscellaneous sources accounting for approximately 1%1\% of total background radiation.

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Sievert (Sv)

The standard scientific unit used for the measurement of radiation dose.

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Chernobyl

A historical nuclear disaster site demonstrating how radioactive contamination can significantly increase local background radiation.

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Factors affecting background radiation and dose

An individual's occupation and geographical location, both of which affect background radiation levels and radiation dose received.

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Cellular effects of ionising radiation

Nuclear radiation ionises chemicals within the human body, altering cell behaviour and causing mutations that can lead to cancer.

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Energy deposition tissue damage

The process by which nuclear radiation deposits large amounts of energy into bodily tissue, damaging or destroying cells completely.

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Shielding (radiation protection)

A protective safety measure of placing absorbing barriers between a radioactive source and an individual to reduce the radiation dose received.

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Exposure time limitation

A safety protocol of minimising the duration spent near a radioactive source to limit cumulative radiation dose.

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Tongs (radiation handling)

A safety tool used to handle radioactive materials at a distance to minimise radiation exposure.

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Contamination protective wear

Protective equipment including masks, gloves, and specialised clothing worn to prevent radioactive substances from getting onto or into the body.

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Radiation badge

A wearable dose-monitoring badge that changes colour when exposed to high doses of radiation to measure personal exposure.

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Short half-life

A radioactive property where a source has very high initial activity that quickly reduces to safe levels, presenting less long-term risk.

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Long half-life

A radioactive property where a source remains weakly radioactive for a long duration, presenting a persistent risk that requires secure storage against contamination.

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Timescale of half-lives

The span of half-life durations across different radioisotopes, which can range from fractions of a second to many thousands of years.

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Radioactive decay

The spontaneous process in which unstable radioactive isotopes decay and emit nuclear radiation.

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Random nature of radioactive decay

The principle that radioactive decay occurs without predictability, meaning one cannot forecast when an individual nucleus will disintegrate.

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Activity

The rate of radioactive decay, defined as the number of disintegrations or counts per second, measured in becquerels (Bq\text{Bq}).

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Becquerel (Bq)

The scientific unit of radioactive activity, equal to one nuclear decay or count per second.

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Count rate

The number of individual radiations detected by an instrument per second.

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Half-life

The time taken for half of the radioactive nuclei in an unstable sample to decay, or for the activity to reach half of its original value.

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Ionising radiation

High-energy nuclear radiation that interacts with neutral atoms or molecules by adding or removing electrons to produce ions.

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Solid Sphere Model (Dalton, 1803)

The atomic model proposed by John Dalton in 1803 depicting the atom as a single, solid, indivisible particle.

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Plum Pudding Model (Thomson, 1904)

The atomic model proposed by J.J. Thomson in 1904 following the discovery of the electron, picturing negative charges distributed inside a positive sphere.

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Nuclear Model (Rutherford, 1911)

The atomic model proposed by Ernest Rutherford in 1911 showing that positive charge and mass are concentrated in a tiny central nucleus.

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Alpha scattering off gold leaf

The 1911 experiment where alpha particles were directed at thin gold leaf; the observed deflections detected the existence of the atomic nucleus.

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Shell Model (Bohr, 1913)

The atomic model proposed by Niels Bohr in 1913 describing electrons orbiting the nucleus in discrete shells to explain energy absorption and emission.

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Modern atom model (Chadwick, 1932)

The atomic model finalized in 1932 when James Chadwick discovered the neutron, following the earlier discovery of protons in the nucleus.

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Atomic empty space

The structural reality that atoms consist primarily of empty space surrounding a tiny, highly concentrated central nucleus.

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Atomic nucleus

The tiny, dense central core of an atom composed of positively charged protons and neutral neutrons.

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Electron shells

Concentric orbits or quantized energy levels surrounding the nucleus where electrons reside.

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Electron shell transitions

The movement of electrons between energy shells caused by absorbing or emitting energy, often in the form of light.

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Electrical neutrality of atoms

The neutral state of an atom where the total number of protons equals the total number of electrons.

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Mass number

The total number of protons and neutrons contained within an atom's nucleus.

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Atomic number

The proton number representing the total count of protons in a nucleus, which also equals the number of electrons in a neutral atom.

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Calculation of neutron number

The arithmetic formula used to determine neutrons: Number of neutrons=Mass number−Proton number\text{Number of neutrons} = \text{Mass number} - \text{Proton number}.

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Proton

A subatomic particle located in the nucleus with a relative mass of 11 and a positive electrical charge of +1+1.

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Neutron

A subatomic particle located in the nucleus with a relative mass of 11 and an electrical charge of 00.

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Electron

A subatomic particle orbiting the nucleus in shells with a relative mass of 00 and a negative electrical charge of −1-1.

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Ion

An electrically charged entity formed when a neutral atom gains or loses electrons, acquiring an overall negative or positive charge.

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Isotopes

Atoms of the same chemical element that possess identical numbers of protons but different numbers of neutrons.

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Irradiation

The process of exposing an object or body to nuclear radiation without radioactive material getting onto or into it.

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Radioactive contamination

The unwanted presence of radioactive substances settling onto or getting inside an object or organism.

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Balancing nuclear equations

The fundamental requirement that both total mass numbers and total atomic numbers balance equally on either side of the decay arrow.

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Alpha particle nature

A form of nuclear radiation consisting of a helium nucleus (24He^4_2\text{He}) containing two protons and two neutrons.

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Alpha particle speed

A relatively low speed of approximately 0.1c0.1c (ten percent of the speed of light).

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Alpha particle range in air

A short travel range through air spanning approximately 3–5 cm3\text{--}5\,\text{cm}.

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Alpha particle charge

An overall positive electrical charge of +2+2.

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Alpha particle penetration

Low penetrating ability, easily stopped and absorbed by a single sheet of paper or human skin.

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Alpha particle ionising power

The strongest ionising capacity among alpha, beta, and gamma radiation types.

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Alpha decay equation

The nuclear decay reaction represented by: ZAX→Z−2A−4Y+24He^A_Z\text{X} \rightarrow ^{A-4}_{Z-2}\text{Y} + ^4_2\text{He}.

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Beta particle nature

A form of nuclear radiation consisting of a fast-moving electron (−10e^0_{-1}\text{e}) ejected from an unstable nucleus.

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Beta particle speed

A medium speed of approximately 0.5c0.5c (half the speed of light).

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Beta particle range in air

A medium travel range through air spanning approximately 0.5–1 m0.5\text{--}1\,\text{m}.

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Beta particle charge

A negative electrical charge of −1-1.

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Beta particle penetration

Medium penetrating ability, capable of penetrating skin and paper but stopped by a few millimetres of aluminium.

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Beta particle ionising power

A medium ionising ability, intermediate between alpha particles and gamma rays.

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Beta decay equation

The nuclear decay reaction represented by: ZAX→Z+1AY+−10e^A_Z\text{X} \rightarrow ^A_{Z+1}\text{Y} + ^0_{-1}\text{e}.

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Gamma ray nature

High-energy electromagnetic radiation emitted from an unstable nucleus carrying away surplus energy.

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Gamma ray speed

The maximum physical speed, travelling precisely at the speed of light (cc).

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Gamma ray range in air

A long travel range through air extending over distances greater than a kilometre (>km>\text{km}).

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Gamma ray charge

An electrical charge of 00, as it consists of electromagnetic radiation rather than matter.

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Gamma ray penetration

High penetrating ability, requiring thick lead or metres of concrete to absorb and reduce its intensity.

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Gamma ray ionising power

The weakest ionising capability among alpha, beta, and gamma radiation types.

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Nuclear effect of gamma emission

Causes no change to the mass number or atomic number of the parent nucleus, representing only a loss of surplus energy.

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Smoke alarms (alpha use)

A domestic safety application utilizing an alpha source to ionise air, triggering an alarm when smoke interrupts the ionisation current.

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Thickness monitoring of aluminium and paper (beta use)

An industrial control system where beta particles pass through rolled sheets to a detector, providing feedback to computer-controlled rollers.

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Radiotherapy (gamma use)

A targeted medical application using penetrating gamma radiation to destroy cancerous cells.

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Nuclear fission

The splitting of a large atomic nucleus into smaller daughter nuclei accompanied by the release of energy and neutrons.

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Mass deficit in fission

The principle where the mass of the parent nucleus is greater than the combined mass of the resulting daughter nuclei.

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E=Δmc2E = \Delta m c^2 (in fission)

The mass-energy equivalence equation showing that lost mass is converted directly into energy released as radiation during fission.

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Stimulated fission

An artificially induced nuclear split caused when a low-speed neutron is fired at and absorbed by a heavy nucleus such as Uranium-235 or plutonium.

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Uranium-235

A fissile isotope utilized in nuclear reactor fuel that absorbs a neutron to trigger stimulated nuclear fission.

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Uranium-236

The highly unstable intermediate nucleus formed when Uranium-235 absorbs a neutron, which promptly undergoes fission.

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Fission neutrons

The 22 or 33 free neutrons ejected when an unstable heavy nucleus splits, capable of colliding with further uranium nuclei.

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Fission chain reaction

A self-sustaining series of fission events where neutrons produced from initial splits trigger successive fissions in nearby nuclei.

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Fuel rods

Rods in a nuclear reactor containing uranium fuel that split and release thermal energy when bombarded with neutrons.

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Graphite moderator

A core component in a nuclear reactor that slows fast fission neutrons down to the correct speed required for fission.

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Boron control rods

Neutron-absorbing rods in a nuclear reactor core that are inserted to reduce the rate of fission or removed to allow the rate to increase.

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Nuclear reactor coolant

A fluid circulated through a nuclear reactor to transfer heat away from the core to produce steam to drive electricity-generating turbines.

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Nuclear reactor waste

Spent reactor material that is intensely radioactive, hot, and possesses very long half-lives, requiring secure containment to prevent contamination.

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Nuclear fusion

The process where two small atomic nuclei collide and fuse together to form a heavier nucleus, releasing large amounts of energy.

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Mass deficit in fusion

The condition where the sum of the masses of the two initial nuclei is greater than the final mass of the combined heavier nucleus.

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Natural fusion reactor

A star, such as our Sun, that naturally and continuously generates heat and light energy via nuclear fusion.

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Net energy barrier in fusion

The current technological limitation wherein human-made fusion reactors consume at least as much energy as they produce, yielding no net energy release.

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Proton repulsion in fusion

The electrostatic repulsive force between positive protons that requires nuclei to collide at extremely high speeds to undergo fusion.

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Plasma temperature threshold for fusion

The extreme thermal condition of at least 150,000,000 ∘C150,000,000\,^{\circ}\text{C} required for hot gas or plasma to allow nuclear fusion to occur.

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Fusion of Hydrogen-1 and Hydrogen-2

A specific fusion collision where a Hydrogen-1 nucleus and a Hydrogen-2 nucleus collide and fuse together to form Helium-3.

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Nuclear stability ratio

The fundamental requirement that stable atomic nuclei must maintain a correct ratio of protons and neutrons.

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Neutron proportion in heavy nuclei

The physical rule that the heavier an atomic nucleus is, the greater the proportion of neutrons it requires to be stable.

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Fusing tendency of light nuclei

The natural tendency of atomic nuclei lighter than iron to fuse together to achieve a more stable configuration.

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Fission tendency of heavy nuclei

The natural tendency of atomic nuclei heavier than iron to undergo nuclear fission to become more stable.

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Iron-56

The most stable atomic nucleus; nuclei lighter than it tend to fuse, whereas nuclei heavier than it tend to split via fission.