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

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2. A hydrogen atom is excited to . The maximum number of distinct emission lines that end specifically in is

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3. A passage describes two alpha-particle paths near the same nucleus.

Case 1: The alpha particle passes at a distance from the nucleus. Case 2: The alpha particle passes at a distance from the nucleus. In both cases, the alpha particle speed far from the nucleus is the same.

Ignoring other complications, the ratio of repulsive force in Case 2 to that in Case 1 at those stated distances is

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4. Consider the following statements about Rutherford’s scattering observations.
I. Most -particles passed through the foil without appreciable deflection.
II. A few -particles were scattered through large angles.
III. All -particles bounced back from the foil.

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5. The Lyman series lies in the ultraviolet region mainly because its transitions end at , giving

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6. In a head-on scattering calculation, the target nucleus changes from charge to , while the alpha-particle kinetic energy remains the same. The closest approach distance changes from to

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7. A proposed orbit contains complete de Broglie wavelengths around its circumference. In the Bohr-de Broglie interpretation, the corresponding value of is

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8. Study the following size-comparison table.

Row Quantity Typical order
P Atomic radius
Q Nuclear radius
R
S

The row that gives an incorrect comparison is

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9. A neutral helium atom has two electrons. The main reason Bohr’s simple one-electron formula cannot be applied directly to it is that

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10. The most complete statement about Bohr’s model is that it

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

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12. For the series limit of a hydrogen series with fixed , the value of is taken as

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13. A hydrogen atom emits a photon when its electron moves from to . Using and , the photon energy is closest to

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14. The radius of the orbit of hydrogen is

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15. A student compares kinetic energy and potential energy in atomic models. Kinetic energy is most directly associated with

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16. For a fixed target and fixed scattering angle in Rutherford scattering, increasing the kinetic energy of the incident -particles reduces large-angle scattering mainly because

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17. A hydrogen atom in the ground state receives of energy. The electron can be

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18. A table gives possible descriptions of electron motion in Bohr’s model.

Row Description Bohr-model status
P Electron in an allowed orbit No radiation while it remains there
Q Electron changes from one allowed orbit to another Radiation may be emitted or absorbed
R Electron in a stationary state Energy remains constant
S Electron in every possible circular orbit All orbits are allowed

The row that conflicts with Bohr’s model is

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

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20. A claim states, “Large deflection occurs because the nucleus attracts the -particle strongly.” The claim should be rejected because

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21. The statement “impact parameter is the distance between the nucleus and the final scattered path” is inaccurate because is measured from

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22. A table compares model features with spectral explanation.

Row Model feature Effect on spectra
P Small positive nucleus Explains large-angle alpha scattering
Q Mostly empty atom Explains most alpha particles passing through
R No quantised energy levels Cannot explain sharp spectral lines
S Classical continuous radiation rule only Naturally gives selected discrete wavelengths

The row that gives an unsuitable spectral statement is

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23. A photon has wavelength . Take , , and . Its energy is closest to

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24. If an electron in Rutherford’s atom were allowed to radiate energy continuously while revolving, the emitted radiation would be expected to have

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25. Assertion: Bohr’s model kept the central nucleus of Rutherford’s model.
Reason: Bohr’s model was built by adding quantum postulates to the nuclear atom.

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26. The empirical Rydberg formula for hydrogen is used mainly to calculate

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27. A graph description is given below.

Horizontal lines represent hydrogen energy levels. The lines are closer together as they approach from below.

This spacing pattern means that transitions between very high neighbouring levels have

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28. A student writes the Rydberg formula for hydrogen as with . The main problem is that this gives

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29. An atomic model that includes charged particles, circular motion, and radiation must be able to deal with all of the following ideas except

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

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31. A graph of hydrogen energy levels shows the levels getting closer together as increases. The correct reason is that

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32. The total energy of a bound electron in the Bohr orbit of a hydrogen-like atom is

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33. A graph of hydrogen energy levels is drawn with at the top and negative levels below it. A transition arrow points upward from to . This arrow represents

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34. A claim says, “An electron in a circular orbit has constant speed, so it has no acceleration and should not radiate.” The flaw is that

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35. Use the situation below.

White light passes through a cool gas and then enters a spectroscope. The observed spectrum has dark lines at some of the same wavelengths that the hot gas emits as bright lines.

The best interpretation is that the cool gas

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36. A hydrogen line has and . Its wavenumber is

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37. Let denote the electron speed in the first Bohr orbit of hydrogen. For , the electron speed in the first orbit is

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38. The energy of the level of hydrogen is

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39. A table lists four claims about bound Bohr states.

Row Claim
P Bound-state total energies are negative when is taken at .
Q Higher levels of hydrogen are less negative.
R Ionisation means taking the electron to or beyond.
S A more negative energy level is less tightly bound.

The row that needs correction is

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40. For a head-on -particle approach, increasing the initial kinetic energy while keeping the target nucleus unchanged makes the closest approach distance

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41. The ionisation energy of from its ground state is

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

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43. A head-on alpha-scattering case has initial kinetic energy . The target nucleus has charge . The alpha particle has charge . The electrostatic potential energy at closest approach is

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44. A graph description is given below.

For the Balmer series, points are plotted for successive upper levels . The vertical axis is wavenumber .

As increases, the plotted points

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45. The idea of de Broglie wavelength enters atomic structure because an electron can show

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46. The observed stability of ordinary atoms means that

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47. A table lists changes in head-on scattering conditions.

Case Nuclear charge factor Alpha kinetic energy factor Effect on
P unchanged doubled of original
Q doubled unchanged times original
R doubled doubled unchanged
S unchanged halved of original

The row that gives the wrong effect on is

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48. For the Balmer series limit, the wavenumber is . Taking , the limiting wavelength is closest to

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49. An atom absorbs a photon of energy and moves from an initial level . The final energy level is

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50. 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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