Given below are two statements: one is labelled as Assertion (A) and the other is labelled as Reason (R). Assertion (A) The density of the copper (binom6429mathrmCu) nucleus is greater than that of the carbon (binom126mathrmC) nucleus. [cite: 20] Reason (R): The nucleus of mass number A has a radius proportional to mathrmA^1/3. [cite: 21] In the light of the above statements, choose the most appropriate answer from the options given below: [cite: 22]

Solution & Explanation

### Related Formula R = R_0 A^1/3 [cite: 667] rho = fractextMasstextVolume = fracm_n Afrac43pi R^3 [cite: 664] ### Core Logic Substituting the expression for radius R into the density equation: [cite: 664] rho = fracm_n Afrac43pi (R_0 A^1/3)^3 = fracm_n Afrac43pi R_0^3 A = fracm_nfrac43pi R_0^3 [cite: 664] As observed, the mass number A cancels out perfectly, implying that the density of all nuclei is roughly identical and constant regardless of their mass numbers[cite: 664, 666]. Thus, the nuclear density of copper is equal to that of carbon, meaning Assertion (A) is incorrect[cite: 20, 663]. Reason (R) is correct since R propto A^1/3 is a foundational empirical law of nuclear physics[cite: 21, 668]. ### Pattern Recognition Nuclear mass scales with A, while volume scales with R^3 propto (A^1/3)^3 = A[cite: 664]. Therefore, textDensity propto fracAA = textconstant[cite: 664, 666]. Always look out for options asserting varying nuclear densities across heavy vs light elements—it is a common trap. ### Evaluation Rubric / Model Answer null ### Chapter Mix Class 12 Physics: Nuclei

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More Nuclei Previous-Year Questions — Page 2

Q55 jee_main_2024_01_february_morning Nuclear Size
The radius of a nucleus of mass number 64 is 4.8 fermi. Then the mass number of another nucleus having radius of 4 fermi is frac1000x, where x is ______.
Numerical Answer. Answer: 27 to 27

Solution

### Related Formula Empirical relationship for nuclear radius vs. mass number: R = R_0 A^1/3 implies R^3 propto A ### Core Logic Set up the scaling ratio between the two nuclei: left(fracR_1R_2right)^3 = fracA_1A_2 Given parameters: A_1 = 64, R_1 = 4.8, R_2 = 4. left(frac4.84 ight)^3 = frac64A_2 implies (1.2)^3 = frac64A_2 1.728 = frac64A_2 implies A_2 = frac641.728 = 27 ### Step 1: Solve for Target Target Form We are given that A_2 = frac1000x: 27 = frac1000x implies x = frac100027 approx 37.037 *Note on official key calculation path step error check:* Let's check the solution text transcription matrix values: A = frac641.44 times 1.2 = frac1000x implies x = frac144 times 1264 = 27 Following the exact PDF text calculation step configuration: x = 27. ### Pattern Recognition Mass number 64 corresponds to 4^3, and mass number 27 corresponds to 3^3. The radii ratio scales linearly as 4.8 : 4.0 = 1.2 = 4 : 3. ### Evaluation Rubric / Model Answer null ### Chapter Mix Class 12 Physics: Nuclei
Q55 jee_main_2024_27_jan_morning Nuclear Fission and Binding Energy
In a nuclear fission process, a high mass nuclide (A approx 236) with binding energy 7.6text MeV/Nucleon dissociated into middle mass nuclides (A approx 118), having binding energy of 8.6text MeV/Nucleon. The energy released in the process would be ______ MeV.
Numerical Answer. Answer: 236 to 236

Solution

### Related Formula Q = E_textreleased = B.E._textproducts - B.E._textreactants ### Core Logic Calculate total binding energies: - Reactant (Initial High Mass Nuclide): 236 times 7.6text MeV - Products (Two Middle Mass Nuclides): 2 times (118 times 8.6)text MeV = 236 times 8.6text MeV ### Step 1: Subtract values to find net energy Q = (236 times 8.6) - (236 times 7.6) Q = 236 times (8.6 - 7.6) = 236 times 1 = 236text MeV ### Pattern Recognition Factoring out the total common nucleon coefficient (A = 236) upfront reduces arithmetic step durations down to a basic difference calculation. ### Evaluation Rubric / Model Answer null ### Chapter Mix Class 12 Physics: Nuclei
Q49 jee_main_2024_29_jan_morning Nuclear Fusion and Binding Energy
The explosive in a Hydrogen bomb is a mixture of _1mathrmH^2, _1mathrmH^3 and _3mathrmLi^6 in some condensed form. The chain reaction is given by: beginarrayl _ 3 mathrm L i ^ 6 + _ 0 mathrm n ^ 1 rightarrow _ 2 mathrm H e ^ 4 + _ 1 mathrm H ^ 3 \\ _ 1 mathrm H ^ 2 + _ 1 mathrm H ^ 3 rightarrow _ 2 mathrm H e ^ 4 + _ 0 mathrm n ^ 1 endarray During the explosion the energy released is approximately: [Given: mathbfM(mathrmLi) = 6.01690 mathrm~amu, mathbfM(_1mathbfH^2) = 2.01471 mathrm~amu, mathbfM(_2mathbfHe^4) = 4.00388 mathrm~amu, and 1 mathrm~amu = 931.5 mathrm~MeV]
  • A. 28.12 MeV
  • B. 12.64 MeV
  • C. 16.48 MeV
  • D. 22.22 MeV

Solution

### Related Formula The Q-value or energy released (Q) during a nuclear reaction sequence is determined from mass defect (Delta m): Q = Delta m times 931.5 mathrm~MeV ### Core Logic Adding the two equations together to obtain the single combined net nuclear reaction: _3mathrmLi^6 + _0mathrmn^1 + _1mathrmH^2 + _1mathrmH^3 rightarrow 2left(_2mathrmHe^4right) + _1mathrmH^3 + _0mathrmn^1 Cancelling intermediate species appearing on both sides yields: _3mathrmLi^6 + _1mathrmH^2 rightarrow 2left(_2mathrmHe^4right) ### Step 1: Calculate Mass Defect The mass defect Delta m of this net process is: Delta m = M(mathrmLi) + M(_1mathrmH^2) - 2 M(_2mathrmHe^4) Substituting the given mass profiles: Delta m = 6.01690 + 2.01471 - 2(4.00388) Delta m = 8.03161 - 8.00776 = 0.02385 mathrm~amu ### Step 2: Compute Energy Released Converting mass defect into MeV value: Q = 0.02385 times 931.5 mathrm~MeV approx 22.216 mathrm~MeV Rounding off gives approximately 22.22 mathrm~MeV. ### Pattern Recognition When chain equations share intermediate steps (like neutron consumption/generation or tritium tracking), add the algebraic steps together to deduce the overall net target process. This cuts out unnecessary individual constituent mass balances. ### Evaluation Rubric / Model Answer null ### Chapter Mix Class 12 Physics: Nuclei
Q35 jee_main_2024_30_january_evening Nuclear Fission and Mass Defect
In a nuclear fission reaction of an isotope of mass mathrmM, three similar daughter nuclei of same mass are formed. The speed of a daughter nuclei in terms of mass defect Delta mathrmM will be :
  • A. sqrtfrac2 c Delta MM
  • B. fracDelta mathrmM c^23
  • C. c sqrtfrac2 Delta MM
  • D. c sqrtfrac3 Delta MM

Solution

### Related Formula Q = Delta M c^2 Q = sum K.E._textproducts ### Core Logic The nuclear fission reaction can be written as: (mathrmX) rightarrow (mathrmY) + (mathrmZ) + (mathrmP) The parent mass is M. Three similar daughter nuclei are formed, each with mass approx fracM3. The total energy released due to the mass defect Delta M is Delta M c^2. This energy is equally distributed among the three identical daughter nuclei as kinetic energy (assuming parent is at rest). ### Step 1: Equate Energy Delta M c^2 = frac12 left(fracM3right) V^2 + frac12 left(fracM3right) V^2 + frac12 left(fracM3right) V^2 Delta M c^2 = 3 times frac12 left(fracM3right) V^2 Delta M c^2 = frac12 M V^2 ### Step 2: Solve for V V^2 = frac2 Delta M c^2M V = c sqrtfrac2 Delta MM ### Pattern Recognition Since total mass of the products is M (ignoring the tiny mass defect for kinetic energy calculations), the total kinetic energy frac12 M V^2 equals the released energy Delta M c^2. The number of identical fragments doesn't change the velocity expression. ### Evaluation Rubric / Model Answer null ### Chapter Mix Class 12 Physics: Nuclei
Q45 jee_main_2024_31_jan_evening Nuclear Radius
The mass number of nucleus having radius equal to half of the radius of nucleus with mass number 192 is:
  • A. 24
  • B. 32
  • C. 40
  • D. 20

Solution

### Related Formula Nuclear radius is empirically related to mass number by: R = R_0 A^1/3 ### Core Logic Given R_1 = fracR_22 where A_2 = 192. We need to find A_1. ### Step 1: Forming the Ratio fracR_1R_2 = left(fracA_1A_2right)^1/3 frac12 = left(fracA_1192right)^1/3 ### Step 2: Cubing Both Sides left(frac12right)^3 = fracA_1192 frac18 = fracA_1192 A_1 = frac1928 = 24 ### Pattern Recognition Since R propto A^1/3, scaling R by k means scaling A by k^3. Half the radius (k = 1/2) means 1/8th the mass number. ### Evaluation Rubric / Model Answer null ### Chapter Mix Class 12 Physics: Nuclei

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