NEB Class 11 • Physics • Modern Physics
Nuclear Physics: NEB Class 11 Physics Guide
Connect the nucleus’s composition to stability, conservation, exponential decay and energy. Use notation and units carefully, and keep applications separate from safe handling.
- Nuclides, forces and stability
- Alpha, beta, gamma, half-life and activity
- Mass defect, binding energy, fission and fusion
Curriculum boundary
Study nuclear structure, transformation and energy as one system
The official CDC Physics Grade 11 page anchors the Nepal course context. Nuclear physics extends ideas from work and energy, electric charge and conservation laws. Institutional explanations from OpenStax nuclear structure and nuclear decay provide comparison.
Keep three levels separate: a single nucleus undergoes a random quantum event; a large sample follows a predictable statistical decay law; a nuclear reaction must balance conserved quantities and energy. Confusing these levels causes statements such as “each nucleus lives exactly one half-life,” which is false.
Nuclear structure
Read nuclide notation before describing stability
In AZX, Z is proton number and identifies the element; A is mass number, the total protons plus neutrons; N=A−Z is neutron number. Isotopes share Z but have different N and A. Ions differ in electron number, not nuclear identity.
Nuclide inventory
2311Na has 11 protons and 12 neutrons. A neutral atom has 11 electrons; Na+ has 10 electrons but the same nucleus. 24Na is an isotope because Z remains 11 while A changes.
The nucleus is roughly femtometre scale. Attractive short-range nuclear interaction competes with electric repulsion between protons. Neutrons contribute to nuclear binding without adding electric repulsion. Stability depends on proton–neutron balance and quantum structure, not simply “more neutrons means safer.”
Use atomic mass unit u and energy unit electron volt carefully: 1 u corresponds to about 931.5 MeV/c², while 1 eV=1.602×10⁻¹⁹ J. A mass unit and an energy unit are connected by E=mc² but are not interchangeable labels.
Radioactive transformations
Balance A and electric charge in every decay equation
| Mode | Emitted radiation | Daughter change | Penetration idea |
|---|---|---|---|
| Alpha | 42He nucleus | A−4, Z−2 | Strong ionisation, short range |
| Beta minus | electron + antineutrino | A same, Z+1 | Intermediate |
| Gamma | high-energy photon | A and Z unchanged | More penetrating; shielding matters |
Alpha balance
23892U → 23490Th + 42He. Mass numbers 238=234+4 and charges 92=90+2.
Beta-minus balance
146C → 147N + 0−1e + antineutrino. A remains 14 and total charge remains 6. At nucleon level, a neutron becomes a proton, electron and antineutrino.
Gamma emission removes nuclear excitation without changing nuclide identity. Alpha, beta and gamma are not merely three “strength levels”; they differ in composition, charge, interaction and shielding behaviour.
Decay law
Predict populations, not the exact death time of one nucleus
For a large sample with constant decay probability, N=N₀e−λt. Half-life T1/2=ln2/λ. After n whole half-lives, N=N₀(1/2)n. Activity is the decay rate: Act=λN, measured in becquerels (Bq), where 1 Bq is one decay per second. Activity follows the same fractional decrease as N.
Whole half-lives
A sample starts at 6400 Bq and has half-life 5.0 h. After 15 h, three half-lives have passed, so activity is 6400/2³=800 Bq.
Non-integer time
If T1/2=8.0 d and t=5.0 d, the remaining fraction is 2−t/T=2−5/8≈0.648. Do not round t/T to one half-life.
A half-life does not mean the sample becomes harmless after one interval, nor does the final half ever occur in the ideal exponential model. Safety depends on isotope, activity, radiation type, route and shielding, not half-life alone.
Mass defect and binding
Use Δmc² with a consistent mass convention
A bound nucleus has less mass than its separated constituents. The difference Δm is mass defect, and binding energy Eb=Δmc² is the energy required to separate the nucleus completely, also the energy released when it forms from free constituents. Binding energy per nucleon Eb/A is more useful for comparing nuclei of different size.
Convert mass defect to energy
If Δm=0.0300 u, binding energy is (0.0300)(931.5 MeV)=27.9 MeV. For A=4, this is 6.99 MeV per nucleon.
The OpenStax binding-energy curve rises rapidly for light nuclei, reaches a high region near iron-mass nuclei and then declines gradually for heavy nuclei. Therefore combining very light nuclei or splitting very heavy nuclei can move products toward greater binding energy per nucleon and release energy.
When atomic masses are used, electron bookkeeping must be consistent. Do not mix bare-nucleus masses, neutral-atom masses and proton masses without checking which electrons cancel.
Fission and fusion
Balance reactions and explain energy through binding
Nuclear fission splits a heavy nucleus into medium-mass fragments, often with neutrons and energy. Released neutrons may produce a chain reaction under suitable conditions. Nuclear fusion combines light nuclei; overcoming electric repulsion requires extreme conditions, while the more tightly bound products release energy. Review the institutional OpenStax fission and fusion section.
Reaction-energy method
For any reaction, first balance A and Z. Then compute Q=(minitial−mfinal)c² with consistent masses. Q>0 means net energy release; Q<0 means energy input is required. Momentum and total energy must also be conserved, so released energy appears as kinetic energy and radiation, not as “missing mass disappearing.”
Do not equate nuclear fission with radioactive decay generally. Spontaneous decay and induced reactions are related by nuclear physics but have different triggers, products and probability descriptions.
Applications and safety
Separate beneficial use from uncontrolled exposure
Ionising radiation is used in medicine, industry, agriculture, research and dating because it interacts predictably with matter and can be detected. Benefits depend on controlled activity, calibration, shielding and trained operation. A student article should not advise handling sources or improvising detection experiments.
The IAEA radiation-protection resources emphasise justified and optimised protection. General external-exposure principles include reducing unnecessary time, increasing distance and using appropriate shielding, but material and thickness depend on radiation type and energy. Follow institutional rules; never touch, move or open an unknown source.
Use the PhET Alpha Decay simulation to explore randomness and population patterns without physical radiation. Simulation supports concepts but is not evidence that every nucleus follows a timer.
Exam readiness
Common mistakes, practice tasks and study method
- Do not confuse isotope with ion.
- Find neutron number using N=A−Z.
- Balance both A and charge in nuclear equations.
- Include the antineutrino conceptually in beta-minus decay.
- Use exponential decay for non-integer half-lives.
- Distinguish activity in Bq from number of nuclei.
- Use consistent atomic or nuclear masses.
- Compare binding energy per nucleon, not total binding alone.
- Explain fission and fusion through the binding curve.
- Treat radiation safety as an institutional responsibility.
Study by linking representations: nuclide symbol → proton/neutron inventory → decay equation → population graph → mass-energy calculation → application and safety statement. After one worked example, change the isotope or elapsed time and solve independently.
- Inventory five nuclides and distinguish isotopes.
- Complete two alpha, two beta and two gamma equations.
- Find remaining fraction for whole and non-whole half-lives.
- Convert mass defect in u to MeV and J.
- Interpret a binding-energy-per-nucleon graph.
- Compare fission and fusion without saying either “creates energy.”
For online or physical NEB tuition, call 9846662070. Continue with the Nuclear Physics Study Guide.
Frequently asked questions
Questions students ask about nuclear physics
What is the difference between an isotope and an ion?
Isotopes differ in neutron number; ions differ in electron number. The nuclear element identity depends on proton number.
Does each nucleus decay after one half-life?
No. Individual decay is random; half-life describes the statistical decline of a large population.
Why is an antineutrino included in beta-minus decay?
It is required for complete conservation of energy, momentum, angular momentum and lepton-family accounting.
What does binding energy mean?
It is the energy required to separate a nucleus into free nucleons, equal to the mass defect times c squared.
Why can both fission and fusion release energy?
Both can form products with greater binding energy per nucleon than their reactants.
Where can I get Nuclear Physics tuition?
Call 9846662070 for current online or physical NEB tuition schedules and fees.
References and next steps
Sources and related study guides
- CDC Nepal: Physics Grade 11
- CDC Nepal: Secondary Education Curriculum
- OpenStax: Substructure of the Nucleus
- OpenStax: Nuclear Decay and Conservation Laws
- OpenStax: Half-Life and Activity
- OpenStax: Nuclear Binding Energy
- IAEA: Radiation Protection
Use the study guide to schedule retrieval and calculation practice. Curriculum scope and linked institutional sources were checked on 2 August 2026; follow current CDC, NEB, school and laboratory instructions if requirements change.
Ask about online or physical tuition
For focused Class 11 and Class 12 subject tuition, lesson clarification, worked-example practice and exam preparation, call 9846662070. Class mode, timetable, teacher availability and fees should be confirmed directly before enrolment.
Related Study Guides
- DC Circuits Practice Set: NEB 11 Physics
- Nuclear Physics Study Guide: NEB 11 Physics
- DC Circuits Study Guide: NEB 11 Physics
- NEB Class 11 Physics: Complete Guide and Study Plan
- DC Circuits: NEB Class 11 Physics Guide
- NEB Class 11 Physics: Chapters and Revision Roadmap
- Capacitors Practice Set: NEB 11 Physics
- Physical Quantities: NEB Class 11 Physics Guide
- Capacitors Study Guide: NEB 11 Physics
- Physical Quantities Study Guide: NEB 11 Physics
- Capacitors: NEB Class 11 Physics Guide
- Vectors: NEB Class 11 Physics Guide
- NEB Class 11 Physics: Complete Guide and Study Plan
MKS Education • Putalisadak
Plan Your Next Step After Grade 12
Ask MKS Education about IELTS, PTE, DET and SAT preparation or study-abroad pre-counselling. Confirm the current class mode, counselling schedule, fees and admission support directly before enrolling.
- Landline01-5921177
- Mobile9818173800
- Email[email protected]
- Websitemks.edu.np
- LocationPutalisadak, Kathmandu
