Below are 68 practice questions on Nuclei, sorted Easy → Hard. Tap “Show answer & explanation” under any question to check yourself. Want the full theory first? Read the Nuclei notes.
Binding energy per nucleon rises sharply for light nuclei, peaks around iron-56 (the most stable nucleus), then slowly declines for heavier nuclei - which is exactly why fusing light nuclei or splitting heavy nuclei both release energy: each moves the products toward this stability peak.
Easy - 20 questions
Q1.
The nucleus of an atom consists of:
A Mainly protons
B Mainly neutrons
C Protons and neutrons
D Electrons and protons
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Answer: C. Protons and neutrons
Why: The nucleus contains protons (positive) and neutrons (neutral), collectively called nucleons.
Q2.
Atomic number Z of an element is:
A Number of neutrons
B Number of protons
C Mass number
D Number of electrons in outer shell
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Answer: B. Number of protons
Why: Atomic number Z = number of protons in the nucleus. It uniquely identifies an element.
Q3.
Alpha radiation consists of:
A Electrons ejected directly from the nucleus
B Helium-4 nuclei (2 protons + 2 neutrons)
C High energy photons emitted from nuclear transitions
D Free neutrons ejected from an unstable nucleus
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Answer: B. Helium-4 nuclei (2 protons + 2 neutrons)
Why: Iron-56 has maximum binding energy per nucleon (~8.8 MeV/nucleon). Elements lighter or heavier than iron release energy by fusion or fission respectively.
Q24.
Carbon-14 dating uses the decay: ¹⁴C → ¹⁴N + ?
A An alpha particle, which would instead reduce the mass number by four
B A gamma ray photon with no accompanying particle emission
C Beta minus particle (electron)
D A free proton ejected directly from the nucleus
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Answer: C. Beta minus particle (electron)
Why: C-14 decay: ¹⁴₆C → ¹⁴₇N + β⁻ + antineutrino. Used for dating organic matter (half-life 5730 years).
Q25.
Radioactive decay law: N(t) = N₀ e<sup>-lambda t</sup>. Activity A = dN/dt in magnitude is:
A lambda N(t)
B lambda/N(t)
C N(t)/lambda
D lambda²N(t)
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Answer: A. lambda N(t)
Why: Activity A = |dN/dt| = lambda × N(t). Activity is proportional to number of undecayed nuclei.
Q26.
After 3 half-lives, the fraction remaining is:
A 1/8
B 1/4
C 1/6
D 1/3
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Answer: A. 1/8
Why: After n half-lives: N/N₀ = (1/2)<sup>n.</sup> After 3: (1/2)³ = 1/8.
Q27.
Nuclear fission of U-235 releases energy by:
A Converting protons directly into neutrons within the nucleus
B Converting mass to energy via E=mc² (mass defect)
C Beta emission alone, with no associated mass-energy conversion
D Fusion of lighter nuclei into a single heavier nucleus
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Answer: B. Converting mass to energy via E=mc² (mass defect)
Why: Fission: heavy nucleus splits into fragments. Product masses total less than reactant masses. Difference (mass defect) appears as energy: E = delta_m × c².
Q28.
The moderator in a nuclear reactor:
A Absorbs neutrons permanently, removing them from the reaction
B Slows down (moderates) fast neutrons to thermal energies
C Controls the overall reaction rate by being inserted or withdrawn
D Cools the reactor core by directly carrying away heat
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Answer: B. Slows down (moderates) fast neutrons to thermal energies
Why: Moderator (heavy water, graphite): slows fast neutrons to thermal energies (~0.025 eV) where U-235 fission cross-section is highest.
Q29.
Critical mass in nuclear weapons/reactors refers to:
A Minimum mass for sustained chain reaction
B The total mass of the entire reactor core including shielding
C The maximum mass legally permitted to be stored at one site
D Exactly half the total mass of fissile material available
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Answer: A. Minimum mass for sustained chain reaction
Why: Critical mass: minimum amount of fissile material for self-sustaining chain reaction (each fission on average causes exactly one more fission).
Q30.
Gamma radiation is best shielded by:
A A sheet of paper, sufficient mainly for stopping alpha particles
B A thin sheet of aluminum, sufficient mainly for stopping beta particles
C Lead or concrete (dense material)
D A thick layer of ordinary air at atmospheric pressure
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Answer: C. Lead or concrete (dense material)
Why: Gamma rays are high-energy photons. Dense materials (lead, concrete) are effective shields. Alpha stopped by paper, beta by Al.
Q31.
Stable nuclei have mass number A such that:
A Z = A/2 exactly for every stable nucleus regardless of size
B Z is approximately A/2 for light nuclei, Z < A/2 for heavy nuclei
C The proton number Z is usually greater than the neutron number N
D The neutron number N is usually exactly zero as frequently observed in practice
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Answer: B. Z is approximately A/2 for light nuclei, Z < A/2 for heavy nuclei
Why: Light stable nuclei: Z ≈ N ≈ A/2. Heavy nuclei need more neutrons for stability (neutron-proton ratio > 1).
Q32.
The decay constant lambda and half-life T<sub>1</sub>/2 are related by:
A lambda = T<sub>1</sub>/2 / ln 2
B lambda = ln 2 / T<sub>1</sub>/2
C lambda = T<sub>1</sub>/2 × ln 2
D lambda = 1 / T<sub>1</sub>/2
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Answer: B. lambda = ln 2 / T<sub>1</sub>/2
Why: N = N₀ e<sup>-lambda t</sup>. At t = T<sub>1</sub>/2: 1/2 = e^(-lambda T<sub>1</sub>/2). lambda × T<sub>1</sub>/2 = ln 2. lambda = ln 2 / T<sub>1</sub>/2 = 0.693/T<sub>1</sub>/2.
Q33.
Neutrinos are emitted in:
A Alpha decay, which emits mainly a helium-4 nucleus
B Gamma decay, which emits mainly a high-energy photon
C Beta decay (along with electron/positron)
D Fission mainly, and rarely in any other type of nuclear decay
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Answer: C. Beta decay (along with electron/positron)
Why: Beta decay: nucleus emits electron + antineutrino (beta-minus) or positron + neutrino (beta-plus). Neutrino carries away some energy.
Q34.
The reaction: ²H + ²H → ³He + n is:
A Fission
B Fusion
C Alpha decay
D Beta decay
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Answer: B. Fusion
Why: Deuterium-deuterium fusion: two light nuclei combine to form heavier nucleus. Releases energy. Basis of hydrogen bomb and future fusion reactors.
Q35.
Specific activity refers to:
A Number of nuclei
B Activity per unit mass
C Total energy released
D Half-life per gram
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Answer: B. Activity per unit mass
Why: Specific activity = activity per unit mass (Bq/kg or Ci/g). Useful for comparing radioactivity of different materials.
Q36.
What is the product when ²³⁸U emits an alpha particle?
A ²³⁴Th
B ²³²Th
C ²³⁴Pa
D ²³⁶U
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Answer: A. ²³⁴Th
Why: Alpha emission: Z decreases by 2, A decreases by 4. U-238 (Z=92) → Th-234 (Z=90, A=234).
Q37.
In a chain reaction, the multiplication factor k represents:
A Number of neutrons per fission as frequently described
B Ratio of neutrons in successive generations
C Total energy per fission in most textbook accounts
D Control rod position during normal conditions
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Answer: B. Ratio of neutrons in successive generations
Why: Multiplication factor k = neutrons in next generation / neutrons in previous generation. k=1: critical, k>1: supercritical, k<1: subcritical.
Q38.
Nuclear radius R = R₀ × A<sup>1/3</sup>. R₀ ≈
A 1.2 fm (femtometers)
B 1.2 nm
C 12 pm
D 0.53 Angstrom
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Answer: A. 1.2 fm (femtometers)
Why: R = R₀ A<sup>1/3</sup> where R₀ ≈ 1.2-1.3 femtometers = 1.2 × 10⁻¹⁵ m. Nuclear density is roughly constant.
Q39.
The mass defect of a nucleus is:
A Mass of nucleus - sum of component nucleon masses
B Usually exactly zero for any stable or unstable nucleus
C Usually negative in magnitude for every known nucleus
D The mass of the constituent protons mainly, ignoring neutrons
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Answer: A. Mass of nucleus - sum of component nucleon masses
Why: Mass defect: delta_m = Z m<sub>p</sub> + N m<sub>n</sub> - M<sub>nucleus</sub>. This is positive for stable nuclei. Binding energy = delta_m × c².
Q40.
Radioactive dating works because:
A The decay constant of the isotope changes predictably over time as generally observed
B The initial amount of radioactive isotope is assumed known and decay is predictable
C The daughter products formed gradually disappear from the sample in typical laboratory settings
D All radioactive isotopes decay at exactly the same fixed rate under usual circumstances
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Answer: B. The initial amount of radioactive isotope is assumed known and decay is predictable
Why: Dating: knowing initial ratio (from atmospheric C-14/C-12 for carbon dating), measuring current ratio, and knowing half-life allows calculation of elapsed time.
Hard - 28 questions
Q41.
The binding energy of Fe-56 is approximately 492 MeV. Binding energy per nucleon:
A 8.79 MeV/nucleon
B 5.6 MeV/nucleon
C 14 MeV/nucleon
D 56 MeV/nucleon
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Answer: A. 8.79 MeV/nucleon
Why: BE/A = 492/56 ≈ 8.79 MeV/nucleon. This is the maximum for any stable nucleus, explaining why iron is the endpoint of stellar fusion.
Q42.
The semi-empirical mass formula (Bethe-Weizsacker) has terms for:
A Volume, surface, Coulomb, asymmetry, and pairing
B Mainly the volume term and the surface term, with nothing else
C Mainly the Coulomb repulsion term, with little other contributions
D Just a single overall binding energy term with little further structure
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Answer: A. Volume, surface, Coulomb, asymmetry, and pairing
Tunneling in alpha decay: the alpha particle tunnels through:
A The nucleus itself, as though it tunneled through its own point of origin
B The Coulomb barrier surrounding the nucleus
C The surrounding electron cloud orbiting around the parent atom
D A magnetic confinement barrier generated by the nuclear spin
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Answer: B. The Coulomb barrier surrounding the nucleus
Why: Alpha decay: alpha particle trapped inside but quantum tunnels through the Coulomb potential barrier. Gamow theory explains the wide range of half-lives.
Q44.
Geiger-Nuttall law for alpha decay relates log(decay constant) to:
A The absolute temperature of the decaying sample
B 1/sqrt(Q) (inverse square root of Q-value)
C The mass number A of the parent nucleus alone
D The atomic number Z of the parent nucleus squared
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Answer: B. 1/sqrt(Q) (inverse square root of Q-value)
Why: Geiger-Nuttall law: log(lambda) = A + B/sqrt(E<sub>alpha</sub>) where E<sub>alpha</sub> is alpha energy. Explains dramatic variation of half-lives with energy.
Q45.
The strong nuclear force acts:
A Between protons only, with no effect on neutrons at all
B At long range, extending across the entire size of an atom
C At short range (< 2-3 fm), between any nucleons
D Between nucleons and electrons, mediating their mutual attraction
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Answer: C. At short range (< 2-3 fm), between any nucleons
Why: Strong force (residual from QCD): short range (~1-3 fm), attractive at ~1-3 fm, repulsive below ~0.7 fm. Holds nucleus together against Coulomb repulsion.
Q46.
Beta-minus decay: n → p + e⁻ + antineutrino. The antineutrino is needed for:
A Charge conservation, which is already satisfied by the electron alone
B Conservation of total rest mass before and after the decay
C Energy and momentum conservation (and lepton number)
D Baryon number conservation, which is unaffected by lepton emission
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Answer: C. Energy and momentum conservation (and lepton number)
Why: Antineutrino is needed to conserve energy (continuous electron spectrum), momentum, angular momentum, and lepton number in beta decay. Pauli proposed it 1930.
Q47.
In nuclear reactions using liquid drop model, fission occurs when:
A A < 50, a mass number range where stable light nuclei are common
B Electrostatic energy exceeds surface energy (fissility parameter x > 1 approx)
C A = 56, the mass number of the most stable nucleus, iron-56
D Temperature exceeds 10⁹ K, a condition relevant to stellar fusion instead
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Answer: B. Electrostatic energy exceeds surface energy (fissility parameter x > 1 approx)
Why: Liquid drop: fission favorable when deformation energy cost (surface) < energy gain (Coulomb reduction). Fissility x = E<sub>C</sub>/(2E<sub>S</sub>) > 1 means spontaneous fission possible.
A Isotopes with equal protons and neutrons according to standard textbooks
B Nuclei with closed shell structure (extra stability)
C Number of isotopes in general practice as frequently described
D Decay products in most textbook accounts during normal conditions
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Answer: B. Nuclei with closed shell structure (extra stability)
Why: Magic numbers: closed shells in nuclear shell model (analogous to noble gas electronic structure). Nuclei with magic Z or N are exceptionally stable.
Q49.
The pion (pi meson) is the particle primarily responsible for:
A Mediating the weak interaction responsible for beta decay
B Mediating the nuclear force (residual strong force)
C Mediating the electron capture process within the nucleus
D Causing spontaneous radioactivity in unstable nuclei generally
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Answer: B. Mediating the nuclear force (residual strong force)
Why: Yukawa (1935): nuclear force mediated by pion exchange. Heavier mediator (compared to photon) gives short range. Pion mass ~ 140 MeV.
Q50.
Nuclear fission vs fusion: which releases more energy per unit mass?
A Fission
B Fusion
C Equal
D Depends on temperature
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Answer: B. Fusion
Why: Fusion releases more energy per unit mass. D-T fusion yields ~14.1 MeV per event with ~5 amu total, ~ 3 MeV/amu. Fission: U-235 yields ~200 MeV with 236 amu, ~ 0.85 MeV/amu.
Q51.
Radioactive equilibrium (secular) occurs when:
A The decay constants of parent and daughter are exactly equal
B Daughter activity equals parent activity (after many daughter half-lives)
C The half-lives of the parent and daughter nuclei are exactly equal
D The total measured activity of the sample falls to zero
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Answer: B. Daughter activity equals parent activity (after many daughter half-lives)
Why: Secular equilibrium: when parent half-life much longer than daughter. Eventually daughter decays as fast as it is produced. A<sub>daughter</sub> = A<sub>parent</sub>.
Q52.
The electron capture process is:
A An electron being emitted directly from inside the nucleus
B Atomic electron absorbed by nucleus (p + e⁻ → n + neutrino)
C A positron being emitted from the nucleus instead of absorbed
D A gamma ray photon emitted following nuclear excitation
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Answer: B. Atomic electron absorbed by nucleus (p + e⁻ → n + neutrino)
Why: Electron capture: inner atomic electron captured by nucleus. Proton + electron → neutron + electron neutrino. Competes with positron emission.
Q53.
In a nuclear reactor, the four-factor formula k∞ =
A eta × epsilon × p × f
B A × B × C × D as generally observed
C n × p × f × e in typical laboratory settings
D power × time under usual circumstances
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Answer: A. eta × epsilon × p × f
Why: Four-factor formula (infinite medium): k∞ = eta × epsilon × p × f where eta = reproduction factor, epsilon = fast fission factor, p = resonance escape probability, f = thermal utilization.
Q54.
The thermonuclear reaction in stars: Proton-proton chain. Net reaction: