33 Years NEET-AIPMT Chapterwise Solutions - Physics 2020
All previous year questions , and these are downloaded from the sources in the internet. I don't own these resources and these are copyrighted by MTG. All previous year questions , and these are downloaded from the sources in the internet. I don't own these resources and these are copyrighted by MTG.
Telegram @unacademyplusdiscounts102 NEET-AIPMT Chapterwise Topicwise Solutions PhysicsANSWER KEY1. (d) 2. (a) 3. (c) 4. (c) 5. (b) 6. (a) 7. (a) 8. (b) 9. (b) 10. (b)11. (d) 12. (c) 13. (b) 14. (b) 15. (a) 16. (d) 17. (c) 18. (d) 19. (b) 20. (b)21. (c) 22. (a) 23. (a) 24. (a) 25. (d) 26. (d) 27. (a) 28. (a,d) 29. (d) 30. (b)31. (c) 32. (d) 33. (b) 34. (a) 35. (b) 36. (b) 37. (b) 38. (c) 39. (a) 40. (b)41. (c) 42. (d) 43. (d) 44. (a) 45. (a) 46. (d) 47. (b) 48. (d) 49. (b) 50. (a)51. (a) 52. (a) 53. (a) 54. (d) 55. (a) 56. (c) 57. (*) 58. (a) 59. (b) 60. (a)61. (a) 62. (b) 63. (d) 64. (c) 65. (a) 66. (a) 67. (a) 68. (c) 69. (a) 70. (d)71. (b) 72. (c) 73. (d) 74. (d) 75. (a) 76. (*) 77. (c) 78. (d) 79. (a) 80. (a)81. (c) 82. (c) 83. (a) 84. (d) 85. (a) 86. (a) 87. (a)Hints & Explanations1. (d) : When a beam of cathode rays (or electrons) aresubjected to crossed electric (E) and magnetic (B) fields,the beam is not deflected, ifForce on electron due to magnetic field = Force onelectron due to electric fieldEBev = eE or v = ...(i)BIf V is the potential difference between the anode and thecathode, then21 2 e vmv = eV or = ...(ii)2m 2VSubstituting the value of v from equation (i) in equation(ii),we get2e E=m 22VB2e ESpecific charge of the cathode rays =m 22VB2. (a) : Collisions of the charged particles with theatoms in the gas.3. (c) 4. (c)5. (b) : Cathode rays are basically negatively chargedparticles (electrons). If the cathode rays are allowed topass between two plates kept at a difference of potential,the rays are found to be deflected from the rectilinearpath. The direction of deflection shows that the rayscarry negative charges.6. (a) 7. (a)8. (b) : Thermionic emission : When a metal is heatedto a high temperature, the free electron gain kineticenergy and escape from the surface of the metal.Secondary emission : When an electron strikes thesurface of a metallic plate, it emits other electrons fromthe surface.Photoelectric emission : Emission of electrons from themetal surface on irradiation with radiation of suitablefrequency.X-rays emission : They are due to transitions in the innerenergy levels of the atom.9. (b) : When a metal is heated, electrons are ejectedout of it, which are called thermions.10. (b) : By changing the position of source of lightfrom photo cell, there will be a change in the intensity oflight falling on photo cell.As stopping potential is independent of the intensityof the incident light, hence stopping potential remainssame i.e., V 0 .11. (d) : The photoelectic emission occurs only whenthe incident light has more than a certain minimumfrequency. This minimum frequency is called thresholdfrequency.12. (c) : The stopping potential V s is related to themaximum kinetic energy of the emitted electrons K maxthrough the relationK max = eV s0.5 eV = eV s or V s = 0.5 V13. (b) : The number of photoelectrons ejected isdirectly proportional to the intensity of incident light.Maximum kinetic energy is independent of intensity ofincident light but depends upon the frequency of light.Hence option (b) is correct.14. (b) : The number of photoelectrons decide thephotocurrent. Assuming that the number of electronsemitted depends on the number of photons incident,the number of photoelectrons depend on the intensity oflight.15. (a)16. (d) : For a light source of power P watt, the intensityPat a distance d is given by I =42πdwhere we assume light to spread out uniformly in alldirections i.e., it is a spherical source.
Telegram @unacademyplusdiscountsDual Nature of Radiation and Matter1031 I1d2 11∴ I ∝ or =h( 5υ 2d I2d1 0)= hυ0 + mv2 ⇒ 4hυ0 = mv2 ...(ii)2221 vI11I1I1or,= ⎛ 1 2 v11or, 4 or, I2.I2⎝ ⎜ ⎞Dividing (i)by(ii), = or05 . ⎠⎟ = =422 2 = .v v2I2428. (a, d) : The maximum kinetic energy is given asIn a photoelectric emission, the number of photoelectronshc hcliberated per second from a photosensitive metallic Kmax h 0 = h h 0 = λ − λsurface is proportional to the intensity of the light. When0where la intensity of source is reduced by a factor of four, the0 = threshold wavelengthnumber of photoelectrons is also reduced by a factor of 4. or 1 2 hc hcmv = −2 λ λ17. (c) : The photoelectric current is directly0proportional to the intensity of illumination. ThereforeHere, h = 4.14 × 10 –15 eV s, c = 3 × 10 8 m s –1a change in the intensity of the incident radiation will l o = 3250 × 10 –10 m = 3250 Åchange the photocurrent.l = 2536 × 10 –10 m = 2536 Å,1equation,2in the first case isE= W0+ mv2hcKmax = −φWhen frequency of incident light is 2u 0 .1 0λ11and that in the second case ish( 2υ0)= hυ0 + mv1 ⇒ hυ0 = mv1 ...(i)hc 2hc22K = − φ0 = −φWhen frequency of incident light is 5u λ0λ0m = 9.1 × 1018. (d) : Photoelectric current I ∝ intensity of light andkghc = 4.14 × 101eV s × 3 × 10 8 m s –1 = 12420 eV Åintensity ∝122 ⎡ 1 1 ⎤(distance)∴ mv = 12420 ⎢ − ⎥ eV=1.076 eV2⎣25363250⎦1∴ I ∝−1922 2. 152 eV 2. 152 × 16 . × 10(distance)v = =19. (b) 20. (b)m−3191 . × 1021. (c) : If the intensity of light of a given frequency \ v ≈ 6 × 10 5 m s –1 = 0.6 × 10 6 m s –1is increased, then the number of photons striking the Note: Options (a) and (d) are same. So both are correct.surface per second will increase in the same ratio. Thisincreased number of photons strikes more electrons ofmetals and hence number of photoelectrons emitted29. (d) : According to Einstein’s photoelectric equationmaximum kinetic energy of photoelectrons,KE max = E v – fthrough the surface increase and hence photoelectric or 2 = 5 – f \ f = 3 eVcurrent increases.When E v = 6 eV then, KE max = 6 – 3 = 3 eV22. (a) : Since the emission of photoelectrons is directly or e(V cathode – V anode ) = 3 eVproportional to the intensity of the incident light, or V cathode – V anode = 3 V = –V stoppingtherefore photocurrent increases with the intensity of \ V stopping = –3 Vlight.30. (b) : According to Einstein’s photoelectric equation,23. (a) : Photoelectric current is directly proportionalhc hceVs to the intensity of incident light.λ − λ 0hc hc24. (a) : The work function has no effect on photoelectric ∴ As perquestion, eV = − ...(i)current so long as hu > W 0 . The photoelectric current isλ λ 0proportional to the intensity of incident light. Since there eV hc hc= −is no change in the intensity of light, hence I 1 = I 2 .4 2λ λ ...(ii)025. (d) : Initially, u = 1.5 u 0From equations (i) and (ii), we getIf the frequency is halved, u′ = υ 15υ0= . hc hc hc hc< u − = −02 22λ 4λ λ0 4λ0Hence, no photoelectric emission will take place.hc 3hc⇒ = or λ0= 3λ26. (d) : Required wavelength of light,4λ4λ0λ0 = 1240 eV nm31. (c) : Let f 0 be the work function of the surface of≈ 310 nmthe material.φ 4 eVAccording to Einstein’s photoelectric equation, the27. (a) : According to the Einstein’s photoelectric maximum kinetic energy of the emitted photoelectronsmax 22
- Page 215 and 216: Telegram @unacademyplusdiscountsJoi
- Page 217 and 218: Electromagnetic InductionTelegram @
- Page 219 and 220: Electromagnetic InductionTelegram @
- Page 221 and 222: Electromagnetic InductionTelegram @
- Page 223 and 224: Telegram @unacademyplusdiscounts62
- Page 225 and 226: Telegram @unacademyplusdiscounts64
- Page 227 and 228: Telegram @unacademyplusdiscounts66
- Page 229 and 230: Telegram @unacademyplusdiscounts68
- Page 231 and 232: Telegram @unacademyplusdiscounts70
- Page 233 and 234: Telegram @unacademyplusdiscounts72
- Page 235 and 236: Telegram @unacademyplusdiscounts74
- Page 237 and 238: Telegram @unacademyplusdiscountsRay
- Page 239 and 240: Telegram @unacademyplusdiscountsRay
- Page 241 and 242: Telegram @unacademyplusdiscountsRay
- Page 243 and 244: Telegram @unacademyplusdiscountsRay
- Page 245 and 246: Telegram @unacademyplusdiscountsRay
- Page 247 and 248: Telegram @unacademyplusdiscountsRay
- Page 249 and 250: Telegram @unacademyplusdiscountsRay
- Page 251 and 252: Telegram @unacademyplusdiscounts88
- Page 253 and 254: Telegram @unacademyplusdiscounts90
- Page 255 and 256: Telegram @unacademyplusdiscounts92
- Page 257 and 258: Telegram @unacademyplusdiscounts94
- Page 259 and 260: Telegram @unacademyplusdiscountsJoi
- Page 261 and 262: Telegram @unacademyplusdiscountsDua
- Page 263 and 264: Telegram @unacademyplusdiscountsDua
- Page 265: Telegram @unacademyplusdiscountsDua
- Page 269 and 270: Telegram @unacademyplusdiscountsDua
- Page 271 and 272: Telegram @unacademyplusdiscountsDua
- Page 273 and 274: AtomsTelegram @unacademyplusdiscoun
- Page 275 and 276: AtomsTelegram @unacademyplusdiscoun
- Page 277 and 278: AtomsTelegram @unacademyplusdiscoun
- Page 279 and 280: AtomsTelegram @unacademyplusdiscoun
- Page 281 and 282: Telegram @unacademyplusdiscounts116
- Page 283 and 284: Telegram @unacademyplusdiscounts118
- Page 285 and 286: Telegram @unacademyplusdiscounts120
- Page 287 and 288: Telegram @unacademyplusdiscounts122
- Page 289 and 290: Telegram @unacademyplusdiscounts124
- Page 291 and 292: Telegram @unacademyplusdiscounts126
- Page 293 and 294: Telegram @unacademyplusdiscountsSem
- Page 295 and 296: Telegram @unacademyplusdiscountsSem
- Page 297 and 298: Telegram @unacademyplusdiscountsSem
- Page 299 and 300: Telegram @unacademyplusdiscountsSem
- Page 301 and 302: Telegram @unacademyplusdiscountsSem
- Page 303 and 304: Telegram @unacademyplusdiscountsSem
- Page 305 and 306: Telegram @unacademyplusdiscountsSem
- Page 307 and 308: Telegram @unacademyplusdiscountsSem
- Page 309: Telegram @unacademyplusdiscountsJoi
Telegram @unacademyplusdiscounts
102 NEET-AIPMT Chapterwise Topicwise Solutions Physics
ANSWER KEY
1. (d) 2. (a) 3. (c) 4. (c) 5. (b) 6. (a) 7. (a) 8. (b) 9. (b) 10. (b)
11. (d) 12. (c) 13. (b) 14. (b) 15. (a) 16. (d) 17. (c) 18. (d) 19. (b) 20. (b)
21. (c) 22. (a) 23. (a) 24. (a) 25. (d) 26. (d) 27. (a) 28. (a,d) 29. (d) 30. (b)
31. (c) 32. (d) 33. (b) 34. (a) 35. (b) 36. (b) 37. (b) 38. (c) 39. (a) 40. (b)
41. (c) 42. (d) 43. (d) 44. (a) 45. (a) 46. (d) 47. (b) 48. (d) 49. (b) 50. (a)
51. (a) 52. (a) 53. (a) 54. (d) 55. (a) 56. (c) 57. (*) 58. (a) 59. (b) 60. (a)
61. (a) 62. (b) 63. (d) 64. (c) 65. (a) 66. (a) 67. (a) 68. (c) 69. (a) 70. (d)
71. (b) 72. (c) 73. (d) 74. (d) 75. (a) 76. (*) 77. (c) 78. (d) 79. (a) 80. (a)
81. (c) 82. (c) 83. (a) 84. (d) 85. (a) 86. (a) 87. (a)
Hints & Explanations
1. (d) : When a beam of cathode rays (or electrons) are
subjected to crossed electric (E) and magnetic (B) fields,
the beam is not deflected, if
Force on electron due to magnetic field = Force on
electron due to electric field
E
Bev = eE or v = ...(i)
B
If V is the potential difference between the anode and the
cathode, then
2
1 2 e v
mv = eV or = ...(ii)
2
m 2V
Substituting the value of v from equation (i) in equation
(ii),we get
2
e E
=
m 2
2VB
2
e E
Specific charge of the cathode rays =
m 2
2VB
2. (a) : Collisions of the charged particles with the
atoms in the gas.
3. (c) 4. (c)
5. (b) : Cathode rays are basically negatively charged
particles (electrons). If the cathode rays are allowed to
pass between two plates kept at a difference of potential,
the rays are found to be deflected from the rectilinear
path. The direction of deflection shows that the rays
carry negative charges.
6. (a) 7. (a)
8. (b) : Thermionic emission : When a metal is heated
to a high temperature, the free electron gain kinetic
energy and escape from the surface of the metal.
Secondary emission : When an electron strikes the
surface of a metallic plate, it emits other electrons from
the surface.
Photoelectric emission : Emission of electrons from the
metal surface on irradiation with radiation of suitable
frequency.
X-rays emission : They are due to transitions in the inner
energy levels of the atom.
9. (b) : When a metal is heated, electrons are ejected
out of it, which are called thermions.
10. (b) : By changing the position of source of light
from photo cell, there will be a change in the intensity of
light falling on photo cell.
As stopping potential is independent of the intensity
of the incident light, hence stopping potential remains
same i.e., V 0 .
11. (d) : The photoelectic emission occurs only when
the incident light has more than a certain minimum
frequency. This minimum frequency is called threshold
frequency.
12. (c) : The stopping potential V s is related to the
maximum kinetic energy of the emitted electrons K max
through the relation
K max = eV s
0.5 eV = eV s or V s = 0.5 V
13. (b) : The number of photoelectrons ejected is
directly proportional to the intensity of incident light.
Maximum kinetic energy is independent of intensity of
incident light but depends upon the frequency of light.
Hence option (b) is correct.
14. (b) : The number of photoelectrons decide the
photocurrent. Assuming that the number of electrons
emitted depends on the number of photons incident,
the number of photoelectrons depend on the intensity of
light.
15. (a)
16. (d) : For a light source of power P watt, the intensity
P
at a distance d is given by I =
4
2
πd
where we assume light to spread out uniformly in all
directions i.e., it is a spherical source.