Atoms Mock Test – Class 12 Physics
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Atoms Mock Test – Class 12 Physics

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Atoms – Progressive Test

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1. A hydrogen atom initially in absorbs a photon of energy . Since the ionisation energy from is , the kinetic energy of the emitted electron is

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2. A one-electron ion emits a photon in the transition . Its photon energy is equal to the hydrogen photon energy. The value of is

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3. Combining Bohr’s angular momentum rule with the circular force-balance condition is mainly used to derive

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4. A claim says, “Bohr’s model failed completely, so it has no useful value.” The better evaluation is that Bohr’s model

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5. The main purpose of an atomic model is to describe

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6. In a comparison of atomic spectra, a line spectrum differs from a continuous spectrum because a line spectrum has

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7. For absorption in Bohr’s model, the electron moves upward from energy to energy , where . The absorbed photon must satisfy

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8. In the context of atomic models, an electron revolving around a nucleus is undergoing accelerated motion because

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9. Bohr’s radius formula and speed formula show opposite dependences on because

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10. Use the energy-level description below.

A hydrogen atom has possible downward transitions from to , from to , and from to .

The transition that emits the longest-wavelength photon is

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11. The first line of the Paschen series corresponds to the transition

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12. A data sheet lists the following conversion: . The energy in joules is

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13. Starting with , if increases with , the speed must vary as for hydrogen because

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14. The allowed radius of the orbit in a hydrogen-like atom is

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15. A hydrogen atom initially in absorbs a photon of wavelength . Using , the atom can be excited to

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16. For corresponding transitions in hydrogen and , such as , the wavelength for is

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17. A circular electron orbit has circumference . In the de Broglie standing-wave picture, the orbit corresponds to

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18. For a hydrogen-like ion, and . If is doubled and is also doubled, then

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19. The key difference between Rutherford’s and Bohr’s treatment of a revolving electron is that Bohr’s model states that the electron

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20. A table compares Rutherford’s model and Bohr’s model.

Row Feature Suitable statement
P Rutherford model Explained the nuclear structure from scattering
Q Rutherford model Could not explain atomic stability classically
R Bohr model Introduced stationary orbits
S Bohr model Rejected the existence of the nucleus

The row that needs correction is

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21. In Bohr’s circular orbit, the centripetal force needed by the electron is supplied by

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22. In a Rutherford-scattering comparison, doubling the foil thickness approximately increases the number of scattered alpha particles because

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23. Hydrogen gas gives a line spectrum rather than a continuous spectrum. This means that hydrogen atoms

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24. The statement “an atom is neutral, so it contains no charged particles” is flawed because

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25. For , the transition emits a photon. Using , its wavelength is closest to

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26. The experimental chamber was evacuated in Rutherford’s scattering experiment mainly to

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27. Classical electromagnetic theory predicts that an electron revolving around a nucleus should

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28. In a Bohr orbit, the electron’s angular momentum is , and the orbit radius is . If the atom is hydrogen, the electron speed is

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29. A graph is described below.

The horizontal axis shows the principal quantum number . The vertical axis shows allowed angular momentum in units of .

The plotted points should lie at

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30. In a head-on approach of an -particle toward a positive nucleus, the deflection is maximum because

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31. The main reason Bohr’s model was not just a repetition of Rutherford’s model is that Bohr added

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32. A graph description is given below.

A bar graph compares two radii on a logarithmic scale. Bar P is at , and bar Q is at .

If the graph represents atomic and nuclear sizes, the correct identification is

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33. A thin foil and an evacuated chamber are both used in the scattering experiment. Their common purpose is to

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34. In the Bohr model, an excited state is a state for which

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35. The usual order of atomic radius is about , while the usual order of nuclear radius is about . This comparison shows that

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36. For the same orbit number , the radius of compared with hydrogen is

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37. For a fixed value of , increasing in the Rydberg formula makes the spectral lines of that series approach

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38. A hydrogen-like ion means an ion that

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39. In head-on alpha scattering, the relation is useful for estimating

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40. The hydrogen line has wavelength approximately . For the corresponding transition in , the wavelength is approximately

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41. A photon has energy . Using , its energy in is

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42. In Bohr’s model, radiation is emitted when the electron

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43. Assertion: Bohr’s model is more successful than Rutherford’s model in explaining the hydrogen spectrum.
Reason: Bohr’s model introduces discrete stationary energy states and photon emission during transitions.

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44. For head-on alpha scattering from the same nucleus, the initial kinetic energy is doubled. The new distance of closest approach becomes

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45. Two Rutherford scattering cases use the same target and the same scattering angle. Case P uses -particles of kinetic energy , while Case Q uses -particles of kinetic energy . If the scattered count varies as , then is

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46. Study the apparatus-function table and choose the fully matched row.

Row Part of setup Function
P Radioactive source Emits alpha particles
Q Collimator Produces a narrow alpha beam
R Gold foil Acts as a thin scattering target
S Zinc sulphide screen Detects alpha particles by scintillation

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47. The small correction ignored in the simplest introductory Bohr formula for hydrogen is mainly due to

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48. Assertion: Rutherford’s model could not explain the observed stability of atoms.
Reason: According to classical theory, an accelerated charged electron should radiate energy while revolving.

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49. The radius of the second Bohr orbit of hydrogen is

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50. Use the arrangement described below.

An -particle approaches a gold atom. Path P passes far from the atom’s centre, path Q passes moderately close to the centre, and path R is directed almost toward the centre.

The largest deflection is expected for

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