JEE Physics Nuclei MCQs Set 24

Physics Objective Questions and Answers: Nuclei

Access targeted multiple-choice questions for Nuclei designed to align with the latest JEE academic syllabus for JEE Physics. These objective practice sets help students evaluate their conceptual understanding and improve exam readiness.

Download Nuclei MCQs with Answers

View or download the dedicated Nuclei MCQ resource below. Practicing these 50 objective questions regularly builds familiarity with standard exam patterns and helps secure higher marks in final Physics evaluations.

Multiple Choice Questions

Question 1: Match List I with List II (parent nucleus and one end product of each process): P alpha decay, Q beta-plus decay, R fission, S proton emission; with 1. \( {}^{15}_{8}\mathrm{O} \) \( \to \) \( {}^{15}_{7}\mathrm{N} \) + ..., 2. \( {}^{238}_{92}\mathrm{U} \) \( \to \) \( {}^{234}_{90}\mathrm{Th} \) + ..., 3. \( {}^{185}_{83}\mathrm{Bi} \) \( \to \) \( {}^{184}_{82}\mathrm{Pb} \) + ..., 4. \( {}^{239}_{94}\mathrm{Pu} \) \( \to \) \( {}^{140}_{57}\mathrm{La} \) + .... Choose the correct pairing:
(a) P-2, Q-1, R-4, S-3
(b) P-4, Q-2, R-1, S-3
(c) P-1, Q-3, R-2, S-4
(d) P-4, Q-3, R-2, S-1
Show Answer & Explanation

Answer: (a) P-2, Q-1, R-4, S-3

Explanation:
1. U-238 to Th-234 loses 4 mass units and 2 charge units: alpha decay, so P-2.
2. O-15 to N-15 keeps A and lowers Z by one: beta-plus decay, so Q-1.
3. Pu-239 to La-140 is a big split into medium nuclei: fission, so R-4.
4. Bi-185 to Pb-184 loses one proton: proton emission, so S-3.

Teacher's Note:
1. I
2. d
3. e
4. n
5. t
6. i
7. f
8. y
9.
10. e
11. a
12. c
13. h
14.
15. p
16. r
17. o
18. c
19. e
20. s
21. s
22.
23. b
24. y
25.
26. t
27. h
28. e
29.
30. c
31. h
32. a
33. n
34. g
35. e
36.
37. i
38. n
39.
40. A
41.
42. a
43. n
44. d
45.
46. Z
47. .

Question 2: A nuclear power plant supplies electrical power to a village using radioactive fuel of half-life T years. The fuel at the beginning is such that the total power requirement of the village is 12.5% of the electrical power available from the plant at that time. If the plant can meet the total power needs of the village for a maximum period of nT years, the value of n is:
(a) 2
(b) 3
(c) 4
(d) 8
Show Answer & Explanation

Answer: (b) 3

Explanation:
1. Power available falls as \( P_0(1/2)^{t/T} \).
2. It stays enough until \( (1/2)^{t/T}=0.125=(1/2)^3 \), i.e. \( t=3T \), so \( n=3 \).

Teacher's Note:
1. P
2. o
3. w
4. e
5. r
6.
7. f
8. r
9. o
10. m
11.
12. a
13.
14. r
15. a
16. d
17. i
18. o
19. a
20. c
21. t
22. i
23. v
24. e
25.
26. s
27. o
28. u
29. r
30. c
31. e
32.
33. f
34. a
35. l
36. l
37. s
38.
39. b
40. y
41.
42. h
43. a
44. l
45. f
46.
47. e
48. v
49. e
50. r
51. y
52.
53. h
54. a
55. l
56. f
57. -
58. l
59. i
60. f
61. e
62. ;
63.
64. 1
65. 2
66. .
67. 5
68. %
69.
70. i
71. s
72.
73. o
74. n
75. e
76.
77. e
78. i
79. g
80. h
81. t
82. h
83. .

Question 3: The electrostatic energy of Z protons uniformly distributed in a sphere of radius R is \( E=\frac35\frac{Z(Z-1)e^2}{4\pi\varepsilon_0R} \). The masses of the neutron, \( {}^{1}_{1}\mathrm{H} \), \( {}^{15}_{7}\mathrm{N} \) and \( {}^{15}_{8}\mathrm{O} \) are 1.008665 u, 1.007825 u, 15.000109 u and 15.003065 u. The radii of N-15 and O-15 are equal, \( 1\ \mathrm{u}=931.5\ \mathrm{MeV}/c^2 \), \( e^2/(4\pi\varepsilon_0)=1.44\ \mathrm{MeV\,fm} \). If the difference in binding energies of N-15 and O-15 is purely electrostatic, the radius of either nucleus is:
(a) 2.85 fm
(b) 3.03 fm
(c) 3.42 fm
(d) 3.80 fm
Show Answer & Explanation

Answer: (c) 3.42 fm

Explanation:
1. B.E. of N-15 \( =(7\times1.007825+8\times1.008665-15.000109)\times931.5=115.49\ \mathrm{MeV} \); B.E. of O-15 \( =111.96\ \mathrm{MeV} \); the difference is 3.536 MeV.
2. Coulomb energies: \( \frac35\frac{1.44}{R}[8\times7-7\times6]=\frac{3\times1.44\times14}{5R}=\frac{12.1}{R}\ \mathrm{MeV} \).
3. Equating, \( R=12.1/3.536=3.42 \) fm.

Teacher's Note:
1. N
2. -
3. 1
4. 5
5.
6. h
7. a
8. s
9.
10. 7
11.
12. p
13. r
14. o
15. t
16. o
17. n
18. s
19.
20. a
21. n
22. d
23.
24. O
25. -
26. 1
27. 5
28.
29. h
30. a
31. s
32.
33. 8
34. ,
35.
36. s
37. o
38.
39. O
40. -
41. 1
42. 5
43.
44. h
45. a
46. s
47.
48. t
49. h
50. e
51.
52. l
53. a
54. r
55. g
56. e
57. r
58.
59. C
60. o
61. u
62. l
63. o
64. m
65. b
66.
67. e
68. n
69. e
70. r
71. g
72. y
73.
74. a
75. n
76. d
77.
78. t
79. h
80. e
81.
82. s
83. m
84. a
85. l
86. l
87. e
88. r
89.
90. b
91. i
92. n
93. d
94. i
95. n
96. g
97.
98. e
99. n
100. e
101. r
102. g
103. y
104. .

Question 4: Masses of neutral atoms: \( {}^{1}_{1}\mathrm{H} \) 1.007825 u, \( {}^{2}_{1}\mathrm{H} \) 2.014102 u, \( {}^{3}_{1}\mathrm{H} \) 3.016050 u, \( {}^{4}_{2}\mathrm{He} \) 4.002603 u, \( {}^{6}_{3}\mathrm{Li} \) 6.015123 u, \( {}^{7}_{3}\mathrm{Li} \) 7.016004 u, \( {}^{209}_{83}\mathrm{Bi} \) 208.980388 u, \( {}^{206}_{82}\mathrm{Pb} \) 205.974455 u, \( {}^{210}_{84}\mathrm{Po} \) 209.982876 u. A heavy nucleus of mass M can break into two light nuclei of masses \( m_1,m_2 \) only if \( m_1+m_2\lt M \); two light nuclei of masses \( m_3,m_4 \) can fuse completely into a heavy nucleus of mass M' only if \( m_3+m_4>M' \). Which statement is correct?
(a) Deuteron and alpha particle can undergo complete fusion
(b) The nucleus \( {}^{6}_{3}\mathrm{Li} \) can emit an alpha particle
(c) The nucleus \( {}^{210}_{84}\mathrm{Po} \) can emit a proton
(d) None of these
Show Answer & Explanation

Answer: (a) Deuteron and alpha particle can undergo complete fusion

Explanation:
1. Li-6 to He-4 + H-2: products \( 4.002603+2.014102=6.016705 \) u exceed \( 6.015123 \) u, so alpha emission is not possible.
2. Po-210 to Bi-209 + H-1: products \( 208.980388+1.007825=209.988213 \) u exceed \( 209.982876 \) u, so proton emission is not possible.
3. H-2 + He-4 forming Li-6: \( 6.016705>6.015123 \), so fusion is allowed.

Teacher's Note:
1. C
2. o
3. m
4. p
5. a
6. r
7. e
8.
9. t
10. h
11. e
12.
13. t
14. o
15. t
16. a
17. l
18.
19. m
20. a
21. s
22. s
23.
24. b
25. e
26. f
27. o
28. r
29. e
30.
31. a
32. n
33. d
34.
35. a
36. f
37. t
38. e
39. r
40. :
41.
42. a
43.
44. p
45. r
46. o
47. c
48. e
49. s
50. s
51.
52. r
53. e
54. l
55. e
56. a
57. s
58. e
59. s
60.
61. e
62. n
63. e
64. r
65. g
66. y
67.
68. o
69. n
70. l
71. y
72.
73. i
74. f
75.
76. t
77. h
78. e
79.
80. f
81. i
82. n
83. a
84. l
85.
86. m
87. a
88. s
89. s
90.
91. i
92. s
93.
94. s
95. m
96. a
97. l
98. l
99. e
100. r
101. .

Question 5: \( {}^{90}_{38}\mathrm{Sr} \) decays to \( {}^{90}_{39}\mathrm{Y} \) by beta decay (half-life 28 years); Y decays by beta decay to Zr with half-life 64 h. A pure sample of Sr-90 is allowed to decay. The ratio \( N_{Sr}/N_Y \) after 1 hour is:
(a) \( 3.56\times10^{5} \)
(b) \( 1.0\times10^{3} \)
(c) \( 3.8\times10^{3} \)
(d) \( 2.4\times10^{7} \)
Show Answer & Explanation

Answer: (a) \( 3.56\times10^{5} \)

Explanation:
1. \( N_Y=\frac{\lambda_{Sr}N_{Sr}}{\lambda_Y-\lambda_{Sr}}\left(1-e^{-(\lambda_Y-\lambda_{Sr})t}\right) \) approximately \( \frac{\lambda_{Sr}N_{Sr}}{\lambda_Y}(1-e^{-\lambda_Yt}) \) because \( \lambda_Y\gg\lambda_{Sr} \).
2. With \( \lambda_Y=0.693/64=0.01083\ \mathrm{h^{-1}} \) and \( \lambda_{Sr}=0.693/(28\times8760)=2.83\times10^{-6}\ \mathrm{h^{-1}} \), at t = 1 h: \( \frac{N_{Sr}}{N_Y}=\frac{\lambda_Y-\lambda_{Sr}}{\lambda_{Sr}(1-e^{-\lambda_Y t})}\approx3.56\times10^{5} \).

Teacher's Note:
1. E
2. a
3. r
4. l
5. y
6.
7. o
8. n
9. ,
10.
11. Y
12.
13. h
14. a
15. s
16.
17. h
18. a
19. d
20.
21. v
22. e
23. r
24. y
25.
26. l
27. i
28. t
29. t
30. l
31. e
32.
33. t
34. i
35. m
36. e
37.
38. t
39. o
40.
41. b
42. u
43. i
44. l
45. d
46.
47. u
48. p
49. ,
50.
51. s
52. o
53.
54. t
55. h
56. e
57.
58. S
59. r
60.
61. t
62. o
63.
64. Y
65.
66. r
67. a
68. t
69. i
70. o
71.
72. i
73. s
74.
75. v
76. e
77. r
78. y
79.
80. l
81. a
82. r
83. g
84. e
85. .

Question 6: The activity of a freshly prepared radioactive sample is \( 10^{10} \) disintegrations per second and its mean life is \( 10^{9}\ \mathrm{s} \). The mass of one atom of this radioisotope is \( 10^{-25}\ \mathrm{kg} \). The mass of the sample is:
(a) 0.1 mg
(b) 1 mg
(c) 10 mg
(d) 100 mg
Show Answer & Explanation

Answer: (b) 1 mg

Explanation:
1. Activity \( A=N/\tau \), so \( N=A\tau=10^{10}\times10^{9}=10^{19} \) atoms.
2. Mass \( =10^{19}\times10^{-25}=10^{-6}\ \mathrm{kg}=1\ \mathrm{mg} \).

Teacher's Note:
1. A
2. c
3. t
4. i
5. v
6. i
7. t
8. y
9.
10. t
11. i
12. m
13. e
14. s
15.
16. m
17. e
18. a
19. n
20.
21. l
22. i
23. f
24. e
25.
26. g
27. i
28. v
29. e
30. s
31.
32. t
33. h
34. e
35.
36. n
37. u
38. m
39. b
40. e
41. r
42.
43. o
44. f
45.
46. n
47. u
48. c
49. l
50. e
51. i
52.
53. p
54. r
55. e
56. s
57. e
58. n
59. t
60. .

Question 7: A neutron scatters elastically from an initially stationary deuteron such that the neutron is scattered at right angles to its original direction. The fraction of the neutron's kinetic energy lost is:
(a) 1/3
(b) 8/9
(c) 2/3
(d) 1/2
Show Answer & Explanation

Answer: (c) 2/3

Explanation:
1. Let the neutron have mass m and speed u, the deuteron 2m. After the collision the neutron moves at right angles with speed v, and the deuteron with speed w at angle \( \theta \).
2. Momentum: \( 2mw\cos\theta=mu,\ 2mw\sin\theta=mv \) and energy \( u^2=v^2+2w^2 \).
3. Solving gives \( v^2=u^2/3 \), so the neutron retains 1/3 of its energy and loses 2/3, \( =\frac{2m}{m+M} \).

Teacher's Note:
1. A
2. t
3.
4. r
5. i
6. g
7. h
8. t
9. -
10. a
11. n
12. g
13. l
14. e
15.
16. s
17. c
18. a
19. t
20. t
21. e
22. r
23. i
24. n
25. g
26.
27. t
28. h
29. e
30.
31. f
32. r
33. a
34. c
35. t
36. i
37. o
38. n
39.
40. l
41. o
42. s
43. t
44.
45. i
46. s
47.
48. \
49. (
50.
51. 2
52. m
53. /
54. (
55. m
56. +
57. M
58. )
59.
60. \
61. )
62.
63. f
64. o
65. r
66.
67. m
68. a
69. s
70. s
71.
72. r
73. a
74. t
75. i
76. o
77.
78. 1
79. :
80. 2
81. .

Question 8: If the binding energy per nucleon in \( {}^{7}_{3}\mathrm{Li} \) and \( {}^{4}_{2}\mathrm{He} \) nuclei are 5.60 MeV and 7.06 MeV respectively, then in the reaction \( p+{}^7_3\mathrm{Li}\to2\,{}^4_2\mathrm{He} \) the energy of the proton must be:
(a) 39.2 MeV
(b) 28.24 MeV
(c) 1.46 MeV
(d) 17.28 MeV
Show Answer & Explanation

Answer: (d) 17.28 MeV

Explanation:
1. Total B.E. of Li-7 \( =7\times5.60=39.2 \) MeV; of two He-4 \( =2\times4\times7.06=56.48 \) MeV.
2. Energy released \( =56.48-39.2=17.28 \) MeV.

Teacher's Note:
1. E
2. n
3. e
4. r
5. g
6. y
7.
8. r
9. e
10. l
11. e
12. a
13. s
14. e
15. d
16.
17. e
18. q
19. u
20. a
21. l
22. s
23.
24. t
25. h
26. e
27.
28. g
29. a
30. i
31. n
32.
33. i
34. n
35.
36. t
37. o
38. t
39. a
40. l
41.
42. b
43. i
44. n
45. d
46. i
47. n
48. g
49.
50. e
51. n
52. e
53. r
54. g
55. y
56. .

Question 9: Atomic masses: \( {}^{41}_{20}\mathrm{Ca} \) = 40.962278 u, \( {}^{42}_{20}\mathrm{Ca} \) = 41.958622 u, neutron = 1.008665 u. The energy needed to remove a neutron from \( {}^{42}_{20}\mathrm{Ca} \) is:
(a) 11.48 MeV
(b) 10.27 MeV
(c) 8.70 MeV
(d) 15.2 MeV
Show Answer & Explanation

Answer: (a) 11.48 MeV

Explanation:
1. \( {}^{42}_{20}\mathrm{Ca} \) \( \to \) \( {}^{41}_{20}\mathrm{Ca} \) + n.
2. Energy \( =(40.962278+1.008665-41.958622)\times931.5=0.012321\times931.5=11.48\ \mathrm{MeV} \).

Teacher's Note:
1. S
2. e
3. p
4. a
5. r
6. a
7. t
8. i
9. o
10. n
11.
12. e
13. n
14. e
15. r
16. g
17. y
18.
19. i
20. s
21.
22. t
23. h
24. e
25.
26. m
27. a
28. s
29. s
30.
31. e
32. x
33. c
34. e
35. s
36. s
37.
38. o
39. f
40.
41. t
42. h
43. e
44.
45. p
46. r
47. o
48. d
49. u
50. c
51. t
52. s
53.
54. o
55. v
56. e
57. r
58.
59. t
60. h
61. e
62.
63. o
64. r
65. i
66. g
67. i
68. n
69. a
70. l
71.
72. n
73. u
74. c
75. l
76. e
77. u
78. s
79. ,
80.
81. t
82. i
83. m
84. e
85. s
86.
87. \
88. (
89.
90. c
91. ^
92. 2
93.
94. \
95. )
96. .

Question 10: The 'rad' is the correct unit used to report the measurement of:
(a) the rate of decay of a radioactive source
(b) the energy delivered by radiation to a target
(c) the ability of a beam of gamma photons to produce ions in a target
(d) the biological effect of radiation
Show Answer & Explanation

Answer: (b) the energy delivered by radiation to a target

Explanation:
1. The rate of decay is measured in becquerel or curie, ionisation in air in roentgen, and biological effect in rem.
2. The rad is the unit of absorbed dose: 1 rad is 0.01 J of energy absorbed per kilogram.

Teacher's Note:
1. A
2. b
3. s
4. o
5. r
6. b
7. e
8. d
9.
10. d
11. o
12. s
13. e
14.
15. m
16. e
17. a
18. s
19. u
20. r
21. e
22. s
23.
24. t
25. h
26. e
27.
28. e
29. n
30. e
31. r
32. g
33. y
34.
35. d
36. e
37. l
38. i
39. v
40. e
41. r
42. e
43. d
44.
45. p
46. e
47. r
48.
49. u
50. n
51. i
52. t
53.
54. m
55. a
56. s
57. s
58.
59. o
60. f
61.
62. t
63. h
64. e
65.
66. a
67. b
68. s
69. o
70. r
71. b
72. i
73. n
74. g
75.
76. m
77. a
78. t
79. e
80. r
81. i
82. a
83. l
84. .

Question 11: An accident in a nuclear laboratory left radioactive material of half-life 18 days inside the laboratory. The radiation was 64 times the permissible level. The minimum number of days after which the laboratory can be considered safe is:
(a) 64
(b) 90
(c) 108
(d) 120
Show Answer & Explanation

Answer: (c) 108

Explanation:
1. Required reduction factor 64 \( =2^6 \), so 6 half-lives are needed.
2. Time \( =6\times18=108 \) days.

Teacher's Note:
1. E
2. a
3. c
4. h
5.
6. h
7. a
8. l
9. f
10. -
11. l
12. i
13. f
14. e
15.
16. h
17. a
18. l
19. v
20. e
21. s
22.
23. t
24. h
25. e
26.
27. r
28. a
29. d
30. i
31. a
32. t
33. i
34. o
35. n
36.
37. l
38. e
39. v
40. e
41. l
42. ;
43.
44. c
45. o
46. u
47. n
48. t
49.
50. h
51. o
52. w
53.
54. m
55. a
56. n
57. y
58.
59. h
60. a
61. l
62. v
63. i
64. n
65. g
66. s
67.
68. g
69. i
70. v
71. e
72.
73. a
74.
75. f
76. a
77. c
78. t
79. o
80. r
81.
82. o
83. f
84.
85. 6
86. 4
87. .

Question 12: Atomic masses: \( {}^{41}_{19}\mathrm{K} \) = 40.961825 u, \( {}^{42}_{20}\mathrm{Ca} \) = 41.958622 u, proton (hydrogen atom) = 1.007826 u. The energy needed to remove a proton from \( {}^{42}_{20}\mathrm{Ca} \) is:
(a) 11.48 MeV
(b) 9.1 MeV
(c) 13.5 MeV
(d) 10.27 MeV
Show Answer & Explanation

Answer: (d) 10.27 MeV

Explanation:
1. \( {}^{42}_{20}\mathrm{Ca} \) \( \to \) \( {}^{41}_{19}\mathrm{K} \) + p (using atomic masses with hydrogen).
2. Energy \( =(40.961825+1.007826-41.958622)\times931.5=0.011029\times931.5=10.27\ \mathrm{MeV} \).

Teacher's Note:
1. R
2. e
3. m
4. o
5. v
6. i
7. n
8. g
9.
10. a
11.
12. p
13. r
14. o
15. t
16. o
17. n
18.
19. t
20. a
21. k
22. e
23. s
24.
25. l
26. e
27. s
28. s
29.
30. e
31. n
32. e
33. r
34. g
35. y
36.
37. t
38. h
39. a
40. n
41.
42. r
43. e
44. m
45. o
46. v
47. i
48. n
49. g
50.
51. a
52.
53. n
54. e
55. u
56. t
57. r
58. o
59. n
60.
61. h
62. e
63. r
64. e
65.
66. b
67. e
68. c
69. a
70. u
71. s
72. e
73.
74. t
75. h
76. e
77.
78. p
79. r
80. o
81. t
82. o
83. n
84. '
85. s
86.
87. e
88. l
89. e
90. c
91. t
92. r
93. o
94. s
95. t
96. a
97. t
98. i
99. c
100.
101. r
102. e
103. p
104. u
105. l
106. s
107. i
108. o
109. n
110.
111. a
112. l
113. r
114. e
115. a
116. d
117. y
118.
119. l
120. o
121. w
122. e
123. r
124. s
125.
126. i
127. t
128. s
129.
130. b
131. i
132. n
133. d
134. i
135. n
136. g
137. .

Question 13: A radioactive nucleus A with half-life T decays into a nucleus B. At t = 0 there is no nucleus B. At some time t, the ratio of the number of B to that of A is 0.3. Then t is given by:
(a) \( t=T\,\frac{\log1.3}{\log2} \)
(b) \( t=\frac{T}{\log1.3} \)
(c) \( t=\frac{T}{2}\frac{\log2}{\log1.3} \)
(d) \( t=T\log1.3 \)
Show Answer & Explanation

Answer: (a) \( t=T\,\frac{\log1.3}{\log2} \)

Explanation:
1. \( N_A=N_0e^{-\lambda t},\ N_B=N_0(1-e^{-\lambda t}) \).
2. \( \frac{N_B}{N_A}=e^{\lambda t}-1=0.3 \), so \( e^{\lambda t}=1.3 \).
3. \( t=\frac{\ln1.3}{\lambda}=T\frac{\ln1.3}{\ln2} \).

Teacher's Note:
1. E
2. v
3. e
4. r
5. y
6.
7. B
8.
9. n
10. u
11. c
12. l
13. e
14. u
15. s
16.
17. c
18. o
19. m
20. e
21. s
22.
23. f
24. r
25. o
26. m
27.
28. a
29.
30. d
31. e
32. c
33. a
34. y
35. e
36. d
37.
38. A
39.
40. n
41. u
42. c
43. l
44. e
45. u
46. s
47. ,
48.
49. s
50. o
51.
52. \
53. (
54.
55. N
56. _
57. B
58. =
59. N
60. _
61. 0
62. -
63. N
64. _
65. A
66.
67. \
68. )
69. .

Question 14: A nucleus of mass \( M+\Delta m \) at rest decays into two daughter nuclei of equal mass \( M/2 \) each. The binding energy per nucleon of the parent is \( E_1 \) and of the daughters is \( E_2 \). Then:
(a) \( E_1>E_2 \)
(b) \( E_2>E_1 \)
(c) \( E_1=2E_2 \)
(d) \( E_2=2E_1 \)
Show Answer & Explanation

Answer: (b) \( E_2>E_1 \)

Explanation:
1. The parent has more mass than the daughters, \( \Delta m>0 \), so energy is released in the decay.
2. Energy is released only when the daughters are more tightly bound per nucleon, so \( E_2>E_1 \).

Teacher's Note:
1. D
2. e
3. c
4. a
5. y
6.
7. t
8. h
9. a
10. t
11.
12. r
13. e
14. l
15. e
16. a
17. s
18. e
19. s
20.
21. e
22. n
23. e
24. r
25. g
26. y
27.
28. a
29. l
30. w
31. a
32. y
33. s
34.
35. e
36. n
37. d
38. s
39.
40. i
41. n
42.
43. m
44. o
45. r
46. e
47.
48. t
49. i
50. g
51. h
52. t
53. l
54. y
55.
56. b
57. o
58. u
59. n
60. d
61.
62. n
63. u
64. c
65. l
66. e
67. i
68. .

Question 15: Masses of neutral atoms: \( {}^{1}_{1}\mathrm{H} \) 1.007825 u, \( {}^{2}_{1}\mathrm{H} \) 2.014102 u, \( {}^{3}_{1}\mathrm{H} \) 3.016050 u, \( {}^{4}_{2}\mathrm{He} \) 4.002603 u, \( {}^{6}_{3}\mathrm{Li} \) 6.015123 u, \( {}^{7}_{3}\mathrm{Li} \) 7.016004 u, \( {}^{209}_{83}\mathrm{Bi} \) 208.980388 u, \( {}^{206}_{82}\mathrm{Pb} \) 205.974455 u, \( {}^{210}_{84}\mathrm{Po} \) 209.982876 u. A heavy nucleus of mass M can break into two light nuclei of masses \( m_1,m_2 \) only if \( m_1+m_2\lt M \); two light nuclei of masses \( m_3,m_4 \) can fuse completely into a heavy nucleus of mass M' only if \( m_3+m_4>M' \). The kinetic energy (in keV) of the alpha particle when \( {}^{210}_{84}\mathrm{Po} \) at rest undergoes alpha decay to \( {}^{206}_{82}\mathrm{Pb} \) is nearly:
(a) 5422
(b) 5707
(c) 5319
(d) 5818
Show Answer & Explanation

Answer: (c) 5319

Explanation:
1. \( Q=(209.982876-205.974455-4.002603)\times931.5=0.005818\times931.5=5.42\ \mathrm{MeV} \).
2. Momentum conservation shares Q inversely with mass: \( K_\alpha=Q\times\frac{206}{210}=5.32\ \mathrm{MeV}\approx5319\ \mathrm{keV} \).

Teacher's Note:
1. T
2. h
3. e
4.
5. l
6. i
7. g
8. h
9. t
10. e
11. r
12.
13. f
14. r
15. a
16. g
17. m
18. e
19. n
20. t
21.
22. g
23. e
24. t
25. s
26.
27. t
28. h
29. e
30.
31. l
32. a
33. r
34. g
35. e
36. r
37.
38. s
39. h
40. a
41. r
42. e
43.
44. o
45. f
46.
47. t
48. h
49. e
50.
51. d
52. e
53. c
54. a
55. y
56.
57. e
58. n
59. e
60. r
61. g
62. y
63. ,
64.
65. a
66.
67. f
68. r
69. a
70. c
71. t
72. i
73. o
74. n
75.
76. \
77. (
78.
79. M
80. _
81. {
82. d
83. a
84. u
85. g
86. h
87. t
88. e
89. r
90. }
91. /
92. (
93. M
94. _
95. {
96. d
97. a
98. u
99. g
100. h
101. t
102. e
103. r
104. }
105. +
106. m
107. _
108. \
109. a
110. l
111. p
112. h
113. a
114. )
115.
116. \
117. )
118. .

Question 16: In the fission \( {}^{236}_{92}\mathrm{U} \) \( \to \) \( {}^{140}_{54}\mathrm{Xe} \) + \( {}^{94}_{38}\mathrm{Sr} \) + x + y, the U-236 is at rest, x and y are two particles with kinetic energies \( K_x=K_y=2\ \mathrm{MeV} \). Binding energies per nucleon of U-236, Xe-140 and Sr-94 are 7.5, 8.5 and 8.5 MeV. Which option is correct?
(a) x = n, y = n, \( K_{Sr}=86 \) MeV, \( K_{Xe}=129 \) MeV
(b) x = p, y = n, \( K_{Sr}=129 \) MeV, \( K_{Xe}=86 \) MeV
(c) x = n, y = e\( ^- \), \( K_{Sr}=129 \) MeV, \( K_{Xe}=86 \) MeV
(d) x = n, y = n, \( K_{Sr}=129 \) MeV, \( K_{Xe}=86 \) MeV
Show Answer & Explanation

Answer: (d) x = n, y = n, \( K_{Sr}=129 \) MeV, \( K_{Xe}=86 \) MeV

Explanation:
1. Charge: 92 = 54 + 38, so x and y carry no net charge; mass number: 236 = 140 + 94 + 2, so both are neutrons.
2. Energy released \( Q=140(8.5)+94(8.5)-236(7.5)=219 \) MeV; neutrons take 4 MeV, leaving 215 MeV for Xe and Sr.
3. Equal momenta: \( K\propto1/m \), so \( K_{Sr}=215\times\frac{140}{234}=129 \) MeV and \( K_{Xe}=215\times\frac{94}{234}=86 \) MeV.

Teacher's Note:
1. C
2. h
3. e
4. c
5. k
6.
7. c
8. h
9. a
10. r
11. g
12. e
13.
14. a
15. n
16. d
17.
18. m
19. a
20. s
21. s
22.
23. n
24. u
25. m
26. b
27. e
28. r
29.
30. f
31. i
32. r
33. s
34. t
35. ,
36.
37. t
38. h
39. e
40. n
41.
42. s
43. p
44. l
45. i
46. t
47.
48. t
49. h
50. e
51.
52. e
53. n
54. e
55. r
56. g
57. y
58.
59. b
60. e
61. t
62. w
63. e
64. e
65. n
66.
67. t
68. h
69. e
70.
71. t
72. w
73. o
74.
75. h
76. e
77. a
78. v
79. y
80.
81. f
82. r
83. a
84. g
85. m
86. e
87. n
88. t
89. s
90.
91. i
92. n
93. v
94. e
95. r
96. s
97. e
98. l
99. y
100.
101. a
102. s
103.
104. t
105. h
106. e
107. i
108. r
109.
110. m
111. a
112. s
113. s
114. e
115. s
116. .

Question 17: In beta-minus decay of a neutron, \( n\to p+e^-+\bar\nu_e \), the neutron is at rest and the anti-neutrino is assumed massless with negligible energy. Momentum and energy conservation then give the maximum kinetic energy of the electron as \( 0.8\times10^6\ \mathrm{eV} \), the kinetic energy carried by the proton being only the recoil energy. If the anti-neutrino had a mass of \( 3\ \mathrm{eV}/c^2 \) instead of zero mass, what would be the range of the electron's kinetic energy K?
(a) \( 0\le K<0.8\times10^6\ \mathrm{eV} \)
(b) \( 0\le K\le0.8\times10^6\ \mathrm{eV} \)
(c) \( 3.0\ \mathrm{eV}\le K\le0.8\times10^6\ \mathrm{eV} \)
(d) \( 3.0\ \mathrm{eV}< K<0.8\times10^6\ \mathrm{eV} \)
Show Answer & Explanation

Answer: (a) \( 0\le K<0.8\times10^6\ \mathrm{eV} \)

Explanation:
1. The electron can still have almost no energy, so the lower limit stays at 0.
2. With a massive anti-neutrino, at least \( 3\ \mathrm{eV} \) of rest energy must be created, so the electron can no longer reach the full \( 0.8\times10^6\ \mathrm{eV} \): the upper limit is not attained.

Teacher's Note:
1. A
2.
3. m
4. a
5. s
6. s
7. i
8. v
9. e
10.
11. a
12. n
13. t
14. i
15. -
16. n
17. e
18. u
19. t
20. r
21. i
22. n
23. o
24.
25. n
26. e
27. e
28. d
29. s
30.
31. r
32. e
33. s
34. t
35.
36. e
37. n
38. e
39. r
40. g
41. y
42. ,
43.
44. s
45. o
46.
47. t
48. h
49. e
50.
51. e
52. l
53. e
54. c
55. t
56. r
57. o
58. n
59. '
60. s
61.
62. m
63. a
64. x
65. i
66. m
67. u
68. m
69.
70. e
71. n
72. e
73. r
74. g
75. y
76.
77. i
78. s
79.
80. s
81. l
82. i
83. g
84. h
85. t
86. l
87. y
88.
89. b
90. e
91. l
92. o
93. w
94.
95. t
96. h
97. e
98.
99. m
100. a
101. s
102. s
103. l
104. e
105. s
106. s
107. -
108. c
109. a
110. s
111. e
112.
113. v
114. a
115. l
116. u
117. e
118. .

Question 18: In a radioactive decay chain, \( {}^{232}_{90}\mathrm{Th} \) decays to \( {}^{212}_{82}\mathrm{Pb} \). Let \( N_\alpha \) and \( N_\beta \) be the numbers of alpha and beta-minus particles emitted. Which is correct?
(a) \( N_\alpha=6 \) and \( N_\beta=4 \) together
(b) \( N_\alpha=5 \) and \( N_\beta=2 \) together
(c) \( N_\alpha=5 \) and \( N_\beta=4 \) together
(d) \( N_\alpha=6 \) and \( N_\beta=2 \) together
Show Answer & Explanation

Answer: (b) \( N_\alpha=5 \) and \( N_\beta=2 \) together

Explanation:
1. Mass number change \( 232-212=20 \), so \( N_\alpha=20/4=5 \).
2. Charge: \( 90-2\times5=80 \) but the final Z is 82, so \( N_\beta=2 \).

Teacher's Note:
1. A
2. l
3. p
4. h
5. a
6.
7. e
8. m
9. i
10. s
11. s
12. i
13. o
14. n
15. s
16.
17. f
18. i
19. x
20.
21. t
22. h
23. e
24.
25. m
26. a
27. s
28. s
29.
30. n
31. u
32. m
33. b
34. e
35. r
36.
37. c
38. h
39. a
40. n
41. g
42. e
43. ;
44.
45. b
46. e
47. t
48. a
49.
50. e
51. m
52. i
53. s
54. s
55. i
56. o
57. n
58. s
59.
60. t
61. h
62. e
63. n
64.
65. c
66. o
67. r
68. r
69. e
70. c
71. t
72.
73. t
74. h
75. e
76.
77. c
78. h
79. a
80. r
81. g
82. e
83. .

Question 19: The half-lives of two radioactive elements A and B are 20 minutes and 40 minutes. Initially the samples have equal numbers of nuclei. After 80 minutes, the ratio of decayed numbers of A and B nuclei will be:
(a) 4 : 1
(b) 1 : 4
(c) 5 : 4
(d) 1 : 16
Show Answer & Explanation

Answer: (c) 5 : 4

Explanation:
1. A: 80 min is 4 half-lives, so the fraction decayed is \( 1-\frac1{16}=\frac{15}{16} \).
2. B: 2 half-lives, fraction decayed \( 1-\frac14=\frac34 \).
3. Ratio \( \frac{15/16}{3/4}=\frac54 \).

Teacher's Note:
1. C
2. o
3. m
4. p
5. a
6. r
7. e
8.
9. t
10. h
11. e
12.
13. d
14. e
15. c
16. a
17. y
18. e
19. d
20.
21. f
22. r
23. a
24. c
25. t
26. i
27. o
28. n
29. s
30. ,
31.
32. n
33. o
34. t
35.
36. t
37. h
38. e
39.
40. r
41. e
42. m
43. a
44. i
45. n
46. i
47. n
48. g
49.
50. f
51. r
52. a
53. c
54. t
55. i
56. o
57. n
58. s
59. .

Question 20: A proton is fired from very far away towards a nucleus of charge \( Q=120e \) and its closest approach is 10 fm. Its de Broglie wavelength (in fm) at the start is: (take \( m_p=\frac53\times10^{-27}\ \mathrm{kg} \), \( h/e=4.2\times10^{-15}\ \mathrm{J\,s/C} \), \( \frac{1}{4\pi\varepsilon_0}=9\times10^9\ \mathrm{m/F} \))
(a) 3
(b) 5
(c) 10
(d) 7
Show Answer & Explanation

Answer: (d) 7

Explanation:
1. All the initial kinetic energy turns into electrostatic potential energy at closest approach: \( K=\frac{(120e)(e)}{4\pi\varepsilon_0 r}=\frac{9\times10^9\times120\times(1.6\times10^{-19})^2}{10^{-14}}=2.76\times10^{-12}\ \mathrm{J} \).
2. \( p=\sqrt{2mK}=\sqrt{2\times\frac53\times10^{-27}\times2.76\times10^{-12}}=9.6\times10^{-20}\ \mathrm{kg\,m/s} \).
3. \( \lambda=h/p=\frac{6.72\times10^{-34}}{9.6\times10^{-20}}=7\times10^{-15}\ \mathrm{m}=7\ \mathrm{fm} \).

Teacher's Note:
1. E
2. n
3. e
4. r
5. g
6. y
7.
8. c
9. o
10. n
11. s
12. e
13. r
14. v
15. a
16. t
17. i
18. o
19. n
20.
21. g
22. i
23. v
24. e
25. s
26.
27. t
28. h
29. e
30.
31. i
32. n
33. i
34. t
35. i
36. a
37. l
38.
39. m
40. o
41. m
42. e
43. n
44. t
45. u
46. m
47. ,
48.
49. a
50. n
51. d
52.
53. t
54. h
55. e
56.
57. d
58. e
59.
60. B
61. r
62. o
63. g
64. l
65. i
66. e
67.
68. r
69. e
70. l
71. a
72. t
73. i
74. o
75. n
76.
77. t
78. h
79. e
80. n
81.
82. g
83. i
84. v
85. e
86. s
87.
88. t
89. h
90. e
91.
92. w
93. a
94. v
95. e
96. l
97. e
98. n
99. g
100. t
101. h
102. .

Question 21: A neutron collides elastically and head-on with an initially stationary deuteron. The fraction of its kinetic energy lost by the neutron is:
(a) 0.89
(b) 0.67
(c) 0.50
(d) 0.11
Show Answer & Explanation

Answer: (a) 0.89

Explanation:
1. For a head-on elastic collision the fractional loss is \( \frac{4mM}{(m+M)^2} \).
2. With \( m=1,\ M=2 \): \( \frac{8}{9}=0.89 \).

Teacher's Note:
1. U
2. s
3. e
4.
5. t
6. h
7. e
8.
9. s
10. t
11. a
12. n
13. d
14. a
15. r
16. d
17.
18. e
19. l
20. a
21. s
22. t
23. i
24. c
25.
26. c
27. o
28. l
29. l
30. i
31. s
32. i
33. o
34. n
35.
36. l
37. o
38. s
39. s
40.
41. f
42. o
43. r
44. m
45. u
46. l
47. a
48.
49. w
50. i
51. t
52. h
53.
54. m
55. a
56. s
57. s
58.
59. r
60. a
61. t
62. i
63. o
64.
65. 1
66. :
67. 2
68. .

Question 22: \( {}^{90}_{38}\mathrm{Sr} \) decays to \( {}^{90}_{39}\mathrm{Y} \) by beta decay (half-life 28 years); Y decays to Zr with half-life 64 h. A pure sample of Sr-90 is allowed to decay. The ratio \( N_{Sr}/N_Y \) after 10 years is nearly:
(a) \( 3.6\times10^{5} \)
(b) \( 3.8\times10^{3} \)
(c) \( 1.0\times10^{2} \)
(d) \( 2.4\times10^{4} \)
Show Answer & Explanation

Answer: (b) \( 3.8\times10^{3} \)

Explanation:
1. After 10 years Y is in transient equilibrium: \( e^{-\lambda_Yt}\approx0 \).
2. \( \frac{N_{Sr}}{N_Y}=\frac{\lambda_Y-\lambda_{Sr}}{\lambda_{Sr}}\approx\frac{T_{Sr}}{T_Y}=\frac{28\times8760}{64}=3.8\times10^3 \).

Teacher's Note:
1. A
2. t
3.
4. l
5. o
6. n
7. g
8.
9. t
10. i
11. m
12. e
13. s
14.
15. t
16. h
17. e
18.
19. r
20. a
21. t
22. i
23. o
24.
25. o
26. f
27.
28. n
29. u
30. c
31. l
32. e
33. i
34.
35. e
36. q
37. u
38. a
39. l
40. s
41.
42. t
43. h
44. e
45.
46. r
47. a
48. t
49. i
50. o
51.
52. o
53. f
54.
55. h
56. a
57. l
58. f
59. -
60. l
61. i
62. v
63. e
64. s
65. ,
66.
67. a
68. s
69.
70. i
71. n
72.
73. t
74. r
75. a
76. n
77. s
78. i
79. e
80. n
81. t
82.
83. e
84. q
85. u
86. i
87. l
88. i
89. b
90. r
91. i
92. u
93. m
94. .

Question 23: On the plot of binding energy per nucleon against mass number, nuclei A and B are light (low B.E. per nucleon), nuclei C, D and E lie near the broad maximum, and F is a heavy nucleus with lower B.E. per nucleon than D and E. Consider: (i) A + B \( \to \) C + \( \varepsilon \); (ii) C \( \to \) A + B + \( \varepsilon \); (iii) D + E \( \to \) F + \( \varepsilon \); (iv) F \( \to \) D + E + \( \varepsilon \). In which are the energies released positive?
(a) (i) and (iii)
(b) (ii) and (iv)
(c) (i) and (iv)
(d) (ii) and (iii)
Show Answer & Explanation

Answer: (c) (i) and (iv)

Explanation:
1. Energy is released when the products have a higher B.E. per nucleon than the reactants.
2. (i) light nuclei fuse into a nucleus near the peak: positive. (iv) a heavy nucleus splits into nuclei near the peak: positive.
3. (ii) and (iii) go away from the peak, so they need energy.

Teacher's Note:
1. R
2. e
3. a
4. c
5. t
6. i
7. o
8. n
9. s
10.
11. t
12. h
13. a
14. t
15.
16. m
17. o
18. v
19. e
20.
21. t
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Question 24: When \( {}^{7}_{3}\mathrm{Li} \) nuclei are bombarded by protons and the resulting nuclei are \( {}^{8}_{4}\mathrm{Be} \), the emitted particles will be:
(a) neutrons
(b) alpha particles
(c) beta particles
(d) gamma photons
Show Answer & Explanation

Answer: (d) gamma photons

Explanation:
1. \( {}^7_3\mathrm{Li}+{}^1_1\mathrm{H}\to{}^8_4\mathrm{Be}+X \): mass number 8 = 8 and charge 4 = 4, so X has zero mass number and zero charge.
2. That is a gamma photon.

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Question 25: The half-lives of uranium and radium are \( 4.5\times10^{9} \) years and 1620 years. In uranium ore at equilibrium, \( N_{Ra}/N_U \) is:
(a) \( 3.6\times10^{-7} \)
(b) \( 2.8\times10^{-3} \)
(c) \( 3.6\times10^{-4} \)
(d) \( 2.8\times10^{6} \)
Show Answer & Explanation

Answer: (a) \( 3.6\times10^{-7} \)

Explanation:
1. At secular equilibrium the activities are equal: \( \lambda_{Ra}N_{Ra}=\lambda_UN_U \).
2. So \( \frac{N_{Ra}}{N_U}=\frac{T_{Ra}}{T_U}=\frac{1620}{4.5\times10^{9}}=3.6\times10^{-7} \).

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