CUET UG Physics Booster Test 3-Mass-Energy and Binding
📌 Answers are locked once submitted — results and explanations appear at the end.
QUESTION 1 OF 20
In a high-energy nuclear reaction, the strict classical conservation of total rest mass is ________, entirely because mass and energy are ________ according to special relativity.
QUESTION 2 OF 20
Match List I with List II regarding the practical implications of E = mc²
| List I | List II |
|---|---|
| 1. Chemical reaction mass defect | a. Extra energy ΔMc² has to be supplied |
| 2. Nuclear reaction mass defect | b. Almost a million times smaller than in nuclear reactions |
| 3. Exothermic fusion reaction | c. Final binding energy > Initial binding energy |
| 4. Endothermic separation process | d. Directly dictates energy scale of MeV per reaction |
QUESTION 3 OF 20
If an isolated nuclear fragment of mass m travels with classical velocity v, its kinetic energy is (1/2)mv². If an identical mass m is completely converted to rest energy E, the algebraic ratio of the converted energy to the kinetic energy is
QUESTION 4 OF 20
Burning 1 kg of coal gives 10⁷ J. Fission of 1 kg of uranium generates 10¹⁴ J. How many kilograms of coal must be completely burned to exactly match the energy released by the total conversion of merely 1 gram of matter into pure energy? (Note: complete mass conversion of 1g = 9 × 10¹³ J).
QUESTION 5 OF 20
Incorrect statement about mass defect in isotopes
QUESTION 6 OF 20
Regarding the analytical mass defect formula
ΔM = [Zmₚ + (A − Z)mₙ] − M
Statements:
1. M represents the rest mass of the fully bound nucleus.
2. The term Zmₚ represents the total mass of isolated protons.
3. ΔMc² represents the binding energy holding the nucleus together.
4. The formula assumes nucleons are in an unbound free state initially.
QUESTION 7 OF 20
Statements regarding the unified conservation law conceptually
1. Strict mass and strict energy are always conserved entirely separately in high energy nuclear reactions.
2. The measurable difference in chemical binding energies technically implies tiny mass-energy conversion occurs in chemical reactions too.
3. What is strictly conserved in realm of very high energies is total charge and total baryon number.
4. The unified law proves that mass defect conceptually exists in molecules as well, just a million times smaller.
QUESTION 8 OF 20
In a nuclear reaction where the total binding energy of the nuclei on the right side is substantially greater than that on the left side, the physical difference in these binding energies
QUESTION 9 OF 20
Let EJ be the calculated energy in Joules and EeV be the identical energy in eV. Given the fundamental charge of an electron is e, the strict algebraic relation is
QUESTION 10 OF 20
Statements regarding energy units mapped to nuclear physics scales
1. 1 u of mass defect equates to 931.5 MeV of binding energy.
2. The binding energy of ¹⁶₈O is roughly 127.5 MeV.
3. 1 MeV is defined identically as 1.6 × 10⁻¹³ J.
4. Energy released in typical nuclear fission is of the macroscopic order of purely electron volts.
QUESTION 11 OF 20
Incorrect statement about conceptual nucleus separation
QUESTION 12 OF 20
Assembling a tightly bound nucleus directly from free protons and neutrons leads to a ________ in total system mass, thereby functioning fundamentally as an ________ process.
QUESTION 13 OF 20
A heavy nucleus X of mass number A = 240 with E_bn = 7.6 MeV breaks into two identical fragments Y of A = 120 with E_bn = 8.5 MeV. What is the absolute total energy released in the process?
QUESTION 14 OF 20
Statements about E_bn as an analytical measure of stability
1. The saturation property of nuclear forces limits E_bn in large nuclei.
2. Continually adding more nucleons to a heavy nucleus linearly increases its E_bn.
3. The value of E_bn directly determines which exothermic reactions are energetically possible.
4. Fission is possible because heavy nuclei have higher E_bn than middle-mass nuclei.
QUESTION 15 OF 20
If a nucleon can have a maximum of p neighbours within the limited range of the nuclear force, and the interaction energy with one such neighbour is k, the binding energy of a single nucleon well inside the plateau region of the nucleus is approximately
QUESTION 16 OF 20
Characteristics of the prominent maximum at Iron (A = 56)
Statements:
1. It represents the single most tightly bound nucleus per nucleon.
2. Its experimentally derived E_bn value is approximately 8.75 MeV.
3. Fission of iron into lighter nuclei would heavily release spontaneous energy.
4. It lies physically within the flat middle region of the overall curve.
QUESTION 17 OF 20
The markedly low binding energy per nucleon for A < 30 implies that when two such light nuclei successfully fuse to form a heavier nucleus,
QUESTION 18 OF 20
For analytically mapping heavy nuclei (A > 170)
Statements:
1. They possess significantly lower E_bn compared to nuclei with A = 120.
2. Their breaking into two lighter fragments naturally increases the total binding energy of the system.
3. Fission functions as an entirely endothermic process for them.
4. They are far more tightly bound per nucleon than iron-56.
QUESTION 19 OF 20
Match List I with List II regarding nuclear binding curves and conceptual features
| List I | List II |
|---|---|
| 1. Smooth E_bn curve feature | a. Decreased binding due to Coulomb repulsion dominating strong force |
| 2. Local peak at ⁴He | b. Considered evidence of atom-like shell structure |
| 3. Gradual drop at A > 170 | c. Due strictly to saturation property of nuclear force |
| 4. Constancy for 30 < A < 170 | d. Shows nuclear force does not depend on electric charge directly |
QUESTION 20 OF 20
Incorrect statement about shell evidence extrapolated from the binding energy curve
Test Complete!
Answer Review
1 In a high-energy nuclear reaction, the strict classical conservation of total rest mass is ________, entirely because mass and energy are ________ according to special relativity.
�� Mass and energy are equivalent. �� Nuclear reactions involve mass-energy conversion. �� Total mass alone is not conserved.
According to Einstein's special relativity, mass and energy are interconvertible and related by E = mc². In nuclear reactions, a small amount of mass can be converted into energy or vice versa. Therefore, the classical law of strict rest-mass conservation is violated. However, the total mass-energy of the system remains conserved. Option B correctly states that strict mass conservation is violated because mass and energy are interconvertible.
- �� Option A → Mass and energy are not independent according to relativity.
- �� Option C → Strict rest mass is not conserved in nuclear reactions.
- �� Option D → Mass and energy are not independent quantities.
Used
- Elimination
Application:
- Check whether mass-energy equivalence is accepted.
Final Logic:
- Mass and energy are interconvertible, so strict mass conservation is violated.
E = mc² → Mass ↔ Energy
2 Match List I with List II regarding the practical implications of E = mc²
| List I | List II |
|---|---|
| 1. Chemical reaction mass defect | a. Extra energy ΔMc² has to be supplied |
| 2. Nuclear reaction mass defect | b. Almost a million times smaller than in nuclear reactions |
| 3. Exothermic fusion reaction | c. Final binding energy > Initial binding energy |
| 4. Endothermic separation process | d. Directly dictates energy scale of MeV per reaction |
�� Chemical mass defects are tiny. �� Nuclear reactions release MeV-scale energy. �� Fusion increases binding energy.
1 → a : Chemical reaction mass defects are almost a million times smaller than nuclear mass defects. 2 → b : Nuclear mass defects determine the MeV energy scale through E = mc². 3 → c : In exothermic fusion, final nuclei have greater binding energy than initial nuclei. 4 → d : Endothermic separation requires external energy equal to ΔMc². Thus, Option A is correct.
- �� Option B → Statements 1 and 2 are interchanged.
- �� Option C → Nuclear mass defect does not correspond directly to binding-energy comparison.
- �� Option D → Multiple incorrect pairings occur.
Used
- Option Grouping
Application:
- Match each physical process with its energy implication.
Final Logic:
- Chemical → tiny defect, Nuclear → MeV scale, Fusion → higher binding energy, Separation → energy input.
Chemical = Small, Nuclear = MeV
3 If an isolated nuclear fragment of mass m travels with classical velocity v, its kinetic energy is (1/2)mv². If an identical mass m is completely converted to rest energy E, the algebraic ratio of the converted energy to the kinetic energy is
�� Rest energy = mc². �� Kinetic energy = ½mv². �� Mass cancels in ratio.
Rest energy: E = mc² Kinetic energy: K = ½mv² Ratio: E/K = mc²/(½mv²) = 2c²/v² Hence option A is correct.
- �� Option B → Inverse factor is incorrect.
- �� Option C → Reciprocal of correct expression.
- �� Option D → Incorrect reciprocal and factor.
Used
- Substitution
Application:
- Substitute standard formulas directly.
Final Logic:
- mc² ÷ (½mv²) = 2c²/v².
Rest/Kinetic → Double c²/v²
4 Burning 1 kg of coal gives 10⁷ J. Fission of 1 kg of uranium generates 10¹⁴ J. How many kilograms of coal must be completely burned to exactly match the energy released by the total conversion of merely 1 gram of matter into pure energy? (Note: complete mass conversion of 1g = 9 × 10¹³ J).
�� 1 g mass → 9 × 10¹³ J. �� Coal gives 10⁷ J/kg. �� Divide total energy by energy per kg.
Energy from complete conversion of 1 g: = 9 × 10¹³ J Coal energy output: = 10⁷ J/kg Required coal: = (9 × 10¹³)/(10⁷) = 9 × 10⁶ kg Hence option B is correct.
- �� Option A → Underestimates by factor 1000.
- �� Option C → Does not match exact calculation.
- �� Option D → Overestimates by factor 1000.
Used
- Substitution
Application:
- Apply direct ratio of energies.
Final Logic:
- 9 × 10¹³ ÷ 10⁷ = 9 × 10⁶ kg.
13 − 7 = 6
5 Incorrect statement about mass defect in isotopes
�� Bound nucleus has lower mass. �� Mass defect produces binding energy. �� Equality never holds for stable nuclei.
A bound nucleus possesses less mass than the sum of its free nucleons because part of the mass is converted into binding energy. This difference is called mass defect. Option D is incorrect because the mass of a bound nucleus is not equal to the simple sum of proton and neutron masses.
- �� Option A → Correct statement about mass defect.
- �� Option B → Correct definition of mass defect.
- �� Option C → Correct method for obtaining nuclear mass from atomic mass.
Used
- Elimination
Application:
- Identify statement contradicting mass defect concept.
Final Logic:
- Bound nucleus mass is always less than free nucleon mass sum.
Bound = Less Mass
6 Regarding the analytical mass defect formula
ΔM = [Zmₚ + (A − Z)mₙ] − M
Statements:
1. M represents the rest mass of the fully bound nucleus.
2. The term Zmₚ represents the total mass of isolated protons.
3. ΔMc² represents the binding energy holding the nucleus together.
4. The formula assumes nucleons are in an unbound free state initially.
�� Formula compares free and bound states. �� Mass defect gives binding energy. �� All statements are correct.
Statement 1 is correct because M denotes the mass of the bound nucleus. Statement 2 is correct because Zmₚ represents total mass of Z free protons. Statement 3 is correct because binding energy = ΔMc². Statement 4 is correct because the formula compares free nucleons with the bound nucleus. Therefore all four statements are correct.
- �� Option A → Omits statement 3, which is correct.
- �� Option B → Omits statement 2, which is correct.
- �� Option C → Omits statement 1, which is correct.
Used
- Elimination
Application:
- Verify each statement using the mass defect formula.
Final Logic:
- All four statements correctly describe the formula.
Defect × c² = Binding Energy
7 Statements regarding the unified conservation law conceptually
1. Strict mass and strict energy are always conserved entirely separately in high energy nuclear reactions.
2. The measurable difference in chemical binding energies technically implies tiny mass-energy conversion occurs in chemical reactions too.
3. What is strictly conserved in realm of very high energies is total charge and total baryon number.
4. The unified law proves that mass defect conceptually exists in molecules as well, just a million times smaller.
�� Mass-energy is conserved jointly. �� Chemical reactions also involve tiny mass defects. �� Molecular binding energy implies mass defect.
Statement 1 is incorrect because mass and energy are not conserved separately in high-energy processes. Statement 2 is correct because chemical binding energy corresponds to extremely small mass changes. Statement 3 is correct because charge and baryon number remain conserved in nuclear reactions. Statement 4 is correct because molecular binding energy also implies a tiny mass defect. Hence statements 2, 3 and 4 are correct.
- �� Option A → Omits statement 4.
- �� Option B → Includes statement 1, which is incorrect.
- �� Option D → Includes statement 1, which is incorrect.
Used
- Elimination
Application:
- Reject statements that assume separate conservation of mass and energy.
Final Logic:
- Only statements 2, 3 and 4 remain valid.
Energy Bound → Mass Found
8 In a nuclear reaction where the total binding energy of the nuclei on the right side is substantially greater than that on the left side, the physical difference in these binding energies
�� Greater binding energy means greater stability. �� Excess energy is released. �� Positive Q-value results.
If final nuclei possess greater total binding energy than initial nuclei, the difference appears as released energy. Such reactions are exothermic and have positive Q-values. Mass-energy conservation remains valid. Therefore option A is correct.
- �� Option B → Opposite of actual situation.
- �� Option C → Final rest mass decreases rather than increases.
- �� Option D → Conservation law remains valid.
Used
- Elimination
Application:
- Higher binding energy corresponds to energy release.
Final Logic:
- Increase in binding energy leads to positive Q-value.
More Binding → More Release
9 Let EJ be the calculated energy in Joules and EeV be the identical energy in eV. Given the fundamental charge of an electron is e, the strict algebraic relation is
�� 1 eV = e joules. �� Convert eV to joules by multiplication. �� e = 1.6 × 10⁻¹⁹ C.
By definition, 1 eV = 1.6 × 10⁻¹⁹ J Therefore, EJ = EeV × e Hence option A is correct.
- �� Option B → Gives incorrect dimensional conversion.
- �� Option C → Uses inverse relation.
- �� Option D → Physical meaning is invalid.
Used
- Dimensional/Unit Analysis
Application:
- Use the definition of electron volt.
Final Logic:
- eV × e gives energy in joules.
eV → Multiply by e
10 Statements regarding energy units mapped to nuclear physics scales
1. 1 u of mass defect equates to 931.5 MeV of binding energy.
2. The binding energy of ¹⁶₈O is roughly 127.5 MeV.
3. 1 MeV is defined identically as 1.6 × 10⁻¹³ J.
4. Energy released in typical nuclear fission is of the macroscopic order of purely electron volts.
�� 1 u corresponds to 931.5 MeV. �� Oxygen-16 binding energy is about 127 MeV. �� MeV is the standard nuclear energy unit.
Statement 1 is correct because 1 u corresponds to approximately 931.5 MeV. Statement 2 is correct because the total binding energy of Oxygen-16 is approximately 127.5 MeV. Statement 3 is correct because 1 MeV = 1.6 × 10⁻¹³ J. Statement 4 is incorrect because fission releases energies of the order of MeV, not eV. Therefore statements 1, 2 and 3 are correct.
- �� Option A → Includes statement 4, which is incorrect.
- �� Option C → Includes statement 4, which is incorrect.
- �� Option D → Includes statement 4, which is incorrect and omits statement 2.
Used
- Elimination
Application:
- Check each statement using standard nuclear energy values.
Final Logic:
- Only statements 1, 2 and 3 are correct.
1 u → 931.5 MeV
11 Incorrect statement about conceptual nucleus separation
�� Binding energy must be supplied for separation. �� Free nucleons have greater mass. �� Bound nuclei are more stable.
When a nucleus is separated into free nucleons, energy equal to the binding energy must be supplied. This added energy increases the total mass-energy of the system. Therefore, the total mass of separated nucleons is greater than that of the original bound nucleus. Hence, statement B is incorrect because separation does not decrease the total mass; it increases it.
- �� Option A → Correct because binding energy must be supplied to break the nucleus.
- �� Option C → Correct because free nucleons possess greater total rest mass.
- �� Option D → Correct because binding energy is a measure of nuclear stability.
Used
- Elimination
Application:
- Compare masses before and after nuclear separation.
Final Logic:
- Separated nucleons have greater mass, not lower mass.
Break Nucleus → Add Energy
12 Assembling a tightly bound nucleus directly from free protons and neutrons leads to a ________ in total system mass, thereby functioning fundamentally as an ________ process.
�� Binding releases energy. �� Released energy corresponds to mass defect. �� Final nucleus has lower mass.
During nucleus formation, free nucleons combine and release binding energy. Since energy leaves the system, the final bound nucleus has less mass than the sum of the individual nucleons. Thus mass decreases and the process is exothermic.
- �� Option B → Mass does not increase during binding.
- �� Option C → Binding is not endothermic.
- �� Option D → Exothermic is correct but mass does not increase.
Used
- Contextual/Tonal Matching
Application:
- Nuclear binding always corresponds to energy release.
Final Logic:
- Energy released ⇒ mass reduced ⇒ exothermic process.
Bind → Release → Defect
13 A heavy nucleus X of mass number A = 240 with E_bn = 7.6 MeV breaks into two identical fragments Y of A = 120 with E_bn = 8.5 MeV. What is the absolute total energy released in the process?
�� Binding energy per nucleon increases. �� Final nuclei are more stable. �� Energy released equals increase in total binding energy.
Initial total binding energy: = 240 × 7.6 = 1824 MeV Final total binding energy: = 240 × 8.5 = 2040 MeV Energy released: = 2040 − 1824 = 216 MeV Therefore, option A is correct.
- �� Option B → Only difference per nucleon is considered.
- �� Option C → Half of the actual energy released.
- �� Option D → Incorrect calculation.
Used
- Substitution
Application:
- Calculate total binding energies before and after fission.
Final Logic:
- 240 × (8.5 − 7.6) = 216 MeV.
ΔE = A × Δ(E/A)
14 Statements about E_bn as an analytical measure of stability
1. The saturation property of nuclear forces limits E_bn in large nuclei.
2. Continually adding more nucleons to a heavy nucleus linearly increases its E_bn.
3. The value of E_bn directly determines which exothermic reactions are energetically possible.
4. Fission is possible because heavy nuclei have higher E_bn than middle-mass nuclei.
�� Saturation limits binding energy. �� Binding energy per nucleon determines stability. �� Heavy nuclei have lower E_bn than medium nuclei.
Statement 1 is correct because nuclear force saturation prevents unlimited growth of E_bn. Statement 2 is incorrect because E_bn does not increase linearly for heavy nuclei. Statement 3 is correct because energy release depends on changes in binding energy. Statement 4 is incorrect because heavy nuclei have lower E_bn than nuclei near iron. Therefore, statements 1 and 3 are correct.
- �� Option B → Includes statement 2, which is incorrect.
- �� Option C → Includes statements 2 and 4, both incorrect.
- �� Option D → Includes statement 4, which is incorrect.
Used
- Elimination
Application:
- Check each statement using the binding-energy-per-nucleon curve.
Final Logic:
- Only statements 1 and 3 agree with the stability curve.
Iron Peak = Maximum Stability
15 If a nucleon can have a maximum of p neighbours within the limited range of the nuclear force, and the interaction energy with one such neighbour is k, the binding energy of a single nucleon well inside the plateau region of the nucleus is approximately
�� Nuclear force is short ranged. �� Each nucleon interacts with limited neighbours. �� Total interaction energy adds approximately.
Inside a large nucleus, a nucleon interacts with approximately p neighbouring nucleons. If interaction energy with each neighbour is k, total binding contribution becomes: E ≈ p × k Therefore option A is correct.
- �� Option B → Incorrect dimensional relationship.
- �� Option C → Interaction energies do not divide.
- �� Option D → Double counting interaction contribution.
Used
- Substitution
Application:
- Multiply number of interactions by energy per interaction.
Final Logic:
- Total energy = p interactions × k energy.
Neighbours × Energy
16 Characteristics of the prominent maximum at Iron (A = 56)
Statements:
1. It represents the single most tightly bound nucleus per nucleon.
2. Its experimentally derived E_bn value is approximately 8.75 MeV.
3. Fission of iron into lighter nuclei would heavily release spontaneous energy.
4. It lies physically within the flat middle region of the overall curve.
�� Iron lies near the peak. �� Binding energy per nucleon is maximum. �� Extremely stable nucleus.
Statement 1 is correct because nuclei around iron are the most tightly bound. Statement 2 is correct because E_bn is approximately 8.75 MeV. Statement 3 is incorrect because fission of iron would require energy rather than release it. Statement 4 is correct because iron lies within the broad middle plateau region. Therefore statements 1, 2 and 4 are correct.
- �� Option B → Includes statement 3, which is incorrect.
- �� Option C → Includes statement 3, which is incorrect.
- �� Option D → Includes statement 3, which is incorrect.
Used
- Elimination
Application:
- Recall the binding-energy-per-nucleon curve maximum.
Final Logic:
- Iron is already near maximum stability.
Iron = Peak Stability
17 The markedly low binding energy per nucleon for A < 30 implies that when two such light nuclei successfully fuse to form a heavier nucleus,
�� Light nuclei have lower E_bn. �� Fusion increases stability. �� Energy is released.
For light nuclei, fusion generally moves the products toward the peak of the binding-energy curve. As binding energy per nucleon increases, the excess energy is released. Thus option A is correct.
- �� Option B → Opposite of fusion energetics.
- �� Option C → Final mass defect is larger, not smaller.
- �� Option D → High temperatures can overcome the Coulomb barrier.
Used
- Contextual/Tonal Matching
Application:
- Move toward higher E_bn on the stability curve.
Final Logic:
- Fusion of light nuclei increases binding energy per nucleon.
Light Fuse → Energy Loose
18 For analytically mapping heavy nuclei (A > 170)
Statements:
1. They possess significantly lower E_bn compared to nuclei with A = 120.
2. Their breaking into two lighter fragments naturally increases the total binding energy of the system.
3. Fission functions as an entirely endothermic process for them.
4. They are far more tightly bound per nucleon than iron-56.
�� Heavy nuclei lie on descending side of curve. �� Fission increases total binding energy. �� Energy is released.
Statement 1 is correct because E_bn decreases for very heavy nuclei. Statement 2 is correct because fission products are more tightly bound. Statement 3 is incorrect because fission is generally exothermic. Statement 4 is incorrect because iron-56 is more tightly bound. Hence statements 1 and 2 are correct.
- �� Option B → Includes statement 3, which is incorrect.
- �� Option C → Includes statement 4, which is incorrect.
- �� Option D → Includes statement 4, which is incorrect.
Used
- Elimination
Application:
- Use the heavy-nuclei region of the binding-energy curve.
Final Logic:
- Heavy nuclei release energy through fission.
Heavy Split → Energy Emit
19 Match List I with List II regarding nuclear binding curves and conceptual features
| List I | List II |
|---|---|
| 1. Smooth E_bn curve feature | a. Decreased binding due to Coulomb repulsion dominating strong force |
| 2. Local peak at ⁴He | b. Considered evidence of atom-like shell structure |
| 3. Gradual drop at A > 170 | c. Due strictly to saturation property of nuclear force |
| 4. Constancy for 30 < A < 170 | d. Shows nuclear force does not depend on electric charge directly |
�� Binding-energy curve reflects nuclear stability. �� Helium-4 shows exceptional stability. �� Saturation produces the plateau region.
1 → d : The smooth nature of the binding-energy curve indicates that nuclear force is largely independent of electric charge. 2 → b : The local peak at ⁴He is considered evidence of shell-like nuclear structure and exceptional stability. 3 → a : For very heavy nuclei, Coulomb repulsion becomes increasingly important, reducing binding energy per nucleon. 4 → c : The near constancy of E_bn for 30 < A < 170 arises from the saturation property of nuclear forces. Therefore, option A is correct.
- �� Option B → Incorrectly matches smooth curve feature and heavy-nucleus behavior.
- �� Option C → Incorrectly associates the helium peak with Coulomb-repulsion effects.
- �� Option D → Incorrectly matches the plateau and heavy-nucleus regions.
Used
- Option Grouping
Application:
- Match each curve feature with the physical principle responsible for it.
Final Logic:
- Smooth curve → charge independence, He-4 peak → shell effect, heavy drop → Coulomb repulsion, plateau → saturation.
Peak → Shell, Plateau → Saturation
20 Incorrect statement about shell evidence extrapolated from the binding energy curve
�� Local peaks indicate enhanced stability. �� Peaks support shell structure. �� Density information is not inferred.
The binding-energy curve primarily provides information about nuclear stability and binding energy per nucleon. Peaks at ⁴He and ¹⁶O indicate unusually stable nuclei, often associated with shell effects. These peaks do not imply that oxygen has a much higher nuclear mass density than iron. Therefore option D is correct.
- �� Option A → Correct description of the overall curve.
- �� Option B → Correctly describes local deviations from the smooth trend.
- �� Option C → Correctly interprets enhanced local stability.
Used
- Elimination
Application:
- Separate stability information from density-related properties.
Final Logic:
- Binding-energy peaks indicate stability, not unusually high density.
Peak = Stable, Not Dense
