CUET UG Physics Booster Test 3- Spectral Series and Duality
📌 Answers are locked once submitted — results and explanations appear at the end.
QUESTION 1 OF 20
Consider the emission spectrum of hydrogen resulting from transitions to various levels. Which statements are analytically true?
1. In a classical model, an accelerating electron spiralling inward would emit a continuous spectrum.
2. According to Bohr's postulate, the frequency of the emitted photon strictly equals (Ei − Ef)/h.
3. For transitions between very large quantum numbers (n to n−1), the frequency of the emitted spectral line coincides with the frequency of revolution.
4. The frequency of the emitted photon is always exactly equal to the frequency of revolution of the electron in its initial orbit.
QUESTION 2 OF 20
When analyzing different transitions in a hydrogen atom, lines that are spaced progressively closer together correspond to transitions involving _______ energy levels, because the absolute energy difference between adjacent levels _______ as n increases.
QUESTION 3 OF 20
Correct statements concerning the transmitted light through a cold, rarefied atomic hydrogen gas:
1. It contains dark lines known collectively as the absorption spectrum.
2. Photons with exact energy differences between a lower and available higher state are actively absorbed.
3. Since most hydrogen atoms are in the ground state at room temperature, the gas primarily absorbs photons of discrete energies like 10.2 eV, 12.09 eV, etc.
4. The transmitted light visually appears as bright spectral lines superimposed on a completely dark background.
QUESTION 4 OF 20
The precise physical origin of dark lines in the absorption spectrum of a rarefied gas indicates that:
QUESTION 5 OF 20
Why is the line spectrum of an element essentially considered its unique identifying fingerprint?
QUESTION 6 OF 20
Given En = −13.6/n² eV, the maximum unique wavelength (λmax) corresponding to a transition out of the first excited state (n=2) down to the ground state (n=1) is derived from the energy difference ΔE = hc/λmax. The exact analytical expression for ΔE in joules is:
QUESTION 7 OF 20
If the orbital radius of an electron in a hydrogen atom is 5.3 × 10⁻¹¹ m in the ground state (n=1), what is the exact absolute energy required to remove the electron completely (Ef = 0) if it is currently orbiting in the n=2 excited state?
QUESTION 8 OF 20
Match the calculated total energy state in a hydrogen atom to its physical significance.
| List I | List II |
|---|---|
| 1. −13.6 eV | a. Energy of a completely removed electron at rest |
| 2. −3.40 eV | b. Energy required to excite a ground-state electron to the first excited state |
| 3. 0 eV | c. Minimum energy to ionise from ground state (expressed as a bound state value) |
| 4. 10.2 eV | d. First excited state bound energy |
QUESTION 9 OF 20
Incorrect statement about discrete transitions from highly excited states directly to the ground state (n=1):
QUESTION 10 OF 20
When an electron in a hydrogen atom falls to the n=3 state from a theoretically infinite quantum number (n → ∞), the energy of the emitted photon approaches a limiting mathematical value. This precise limit corresponds exactly to:
QUESTION 11 OF 20
Correct statements about the wave-particle dual nature implication for Bohr orbits:
1. Bohr's specific stable orbits are a direct mathematical consequence of the electron behaving as a particle wave that forms resonant standing waves.
2. The de Broglie wavelength strictly equals h/mvn when the electron speed is significantly less than the speed of light.
3. The wave-particle duality completely and entirely replaces the classical electrostatic force in determining physical orbit stability.
4. Only resonant standing waves uniquely avoid rapid destructive interference upon cyclic reflection within the orbit.
QUESTION 12 OF 20
Substituting the classical velocity expression vn = e / √(4πε₀mrn) into the fundamental de Broglie wavelength equation λ = h/mvn, we find λ strictly depends on the radius rn as:
QUESTION 13 OF 20
In analogizing de Broglie particle waves on a circular orbit to mechanical waves vibrating on a fixed string:
1. Both macroscopic and microscopic systems excite exactly a single wavelength when randomly disturbed.
2. Both require defined nodes at the boundary ends, translating to exactly an integer number of full wavelengths fitting the circumference.
3. Both necessarily result in a continuously changing broad spectrum of electromagnetic radiation.
4. Neither physical system relies fundamentally on the geometric dimensions of the string or orbit.
QUESTION 14 OF 20
Statements conceptually concerning the standing wave relation 2πrn = nλ:
1. It dictates that rn can dynamically take any continuous fractional value.
2. It leads directly to Bohr's specific quantisation condition of angular momentum.
3. It demonstrates why hypothetical orbits with non-integer wavelength fractions rapidly decay to zero amplitude.
4. It implies that the total distance travelled by the electron wave down the orbit and back is a perfect integer number of wavelengths.
QUESTION 15 OF 20
If the orbital radius of a hydrogen atom in the ground state (n=1) is 5.3 × 10⁻¹¹ m, what is the exact analytical quantum condition required for the angular momentum in the second excited state (n=3)?
QUESTION 16 OF 20
The core physical reason an atom does not collapse continuously as originally predicted by classical electromagnetic theory is because the electron strictly resides in _______ states where its particle wave forms a completely _______ wave.
QUESTION 17 OF 20
Match the atomic system with its theoretical compatibility with Bohr's original model.
| List I | List II |
|---|---|
| 1. Hydrogen atom (Z = 1) | a. Fails completely due to electron-electron interactions |
| 2. Helium atom (2 electrons) | b. Hydrogenic model, gross features predicted correctly |
| 3. Singly ionised helium (He⁺) | c. Hydrogenic model, Z = 2 |
| 4. Doubly ionised lithium (Li²⁺) | d. Hydrogenic model, Z = 3 |
QUESTION 18 OF 20
Incorrect statement about the theoretical transition likelihoods in Bohr's model:
QUESTION 19 OF 20
When attempting to cleanly extend the Bohr model to complex multi-electron atoms, the theoretical analysis failed primarily because:
QUESTION 20 OF 20
How does modern quantum mechanics explicitly redefine the basic conceptual framework of the Bohr model?
Test Complete!
Answer Review
1 Consider the emission spectrum of hydrogen resulting from transitions to various levels. Which statements are analytically true?
1. In a classical model, an accelerating electron spiralling inward would emit a continuous spectrum.
2. According to Bohr's postulate, the frequency of the emitted photon strictly equals (Ei − Ef)/h.
3. For transitions between very large quantum numbers (n to n−1), the frequency of the emitted spectral line coincides with the frequency of revolution.
4. The frequency of the emitted photon is always exactly equal to the frequency of revolution of the electron in its initial orbit.
�� Classical theory predicts continuous radiation. �� Bohr frequency condition gives photon frequency. �� Correspondence principle applies at large n.
Statement 1 is correct because a classical accelerating electron would continuously lose energy and emit a continuous spectrum. Statement 2 is correct because Bohr's frequency condition states that the emitted photon frequency is given by ν = (Ei − Ef)/h. Statement 3 is correct due to Bohr's correspondence principle, according to which transitions between very large quantum numbers produce frequencies approaching the orbital frequency. Statement 4 is incorrect because the emitted photon frequency is generally determined by the energy difference between two states and is not always equal to the orbital frequency of the initial orbit. Therefore, statements 1, 2 and 3 are correct.
- �� Option B → Omits statements 1 and 3, which are correct.
- �� Option C → Includes statement 4, which is incorrect.
- �� Option D → Includes statement 4 and excludes statements 2 and 3.
Used
- Elimination
Application:
- Check each statement using Bohr's postulates and correspondence principle.
Final Logic:
- Only statements 1, 2 and 3 are correct.
Classical → Continuous, Bohr → Discrete
2 When analyzing different transitions in a hydrogen atom, lines that are spaced progressively closer together correspond to transitions involving _______ energy levels, because the absolute energy difference between adjacent levels _______ as n increases.
�� Energy levels crowd together at large n. �� Adjacent energy differences decrease. �� Spectral lines become closer.
For hydrogen, En = −13.6/n² eV. As n increases, the spacing between adjacent energy levels becomes smaller. Therefore, transitions involving higher energy levels produce spectral lines that are progressively closer together. This explains the convergence of spectral series. Hence, the correct combination is Higher energy levels and Decreases.
- �� Option A → Energy spacing does not increase at lower levels.
- �� Option C → Closely spaced lines occur at higher, not lower, levels.
- �� Option D → Energy difference decreases rather than increases.
Used
- Concept Application
Application:
- Use the hydrogen energy-level formula.
Final Logic:
- Higher n gives smaller level spacing and closer spectral lines.
Higher n → Narrow Gap
3 Correct statements concerning the transmitted light through a cold, rarefied atomic hydrogen gas:
1. It contains dark lines known collectively as the absorption spectrum.
2. Photons with exact energy differences between a lower and available higher state are actively absorbed.
3. Since most hydrogen atoms are in the ground state at room temperature, the gas primarily absorbs photons of discrete energies like 10.2 eV, 12.09 eV, etc.
4. The transmitted light visually appears as bright spectral lines superimposed on a completely dark background.
�� Absorption produces dark lines. �� Only specific photon energies are absorbed. �� Ground-state atoms dominate absorption.
Statement 1 is correct because absorption spectra consist of dark lines in a continuous spectrum. Statement 2 is correct because atoms absorb only photons whose energies match allowed transitions. Statement 3 is correct because most hydrogen atoms are in the ground state and absorb photons corresponding to excitation from n = 1. Statement 4 is incorrect because bright lines on a dark background represent an emission spectrum, not an absorption spectrum. Therefore, statements 1, 2 and 3 are correct.
- �� Option A → Includes statement 4, which is incorrect.
- �� Option C → Includes statement 4 and excludes statement 2.
- �� Option D → Includes statement 4, which is incorrect.
Used
- Elimination
Application:
- Distinguish absorption spectra from emission spectra.
Final Logic:
- Only statements 1, 2 and 3 describe absorption correctly.
Absorption = Dark Lines
4 The precise physical origin of dark lines in the absorption spectrum of a rarefied gas indicates that:
�� Absorption occurs at specific frequencies. �� Electrons move to higher levels. �� Missing frequencies appear as dark lines.
Dark absorption lines arise because atoms absorb photons whose energies exactly match the energy differences between allowed electronic states. The absorbed photons excite electrons to higher levels, removing those frequencies from the transmitted light. Therefore, option C correctly explains the origin of absorption lines.
- �� Option A → Dark lines are not produced by destructive interference.
- �� Option B → Absorption is not equivalent to all photons being scattered at 90°.
- �� Option D → Electromagnetic radiation is not converted entirely into mass.
Used
- Elimination
Application:
- Identify the actual mechanism behind absorption spectra.
Final Logic:
- Selective absorption of specific frequencies produces dark lines.
Dark Line = Missing Photon
5 Why is the line spectrum of an element essentially considered its unique identifying fingerprint?
�� Each element has unique energy levels. �� Unique transitions produce unique wavelengths. �� Spectra identify elements.
Every element possesses a unique electronic structure and hence a unique set of allowed energy levels. The wavelengths emitted during transitions between these levels form a characteristic line spectrum. This makes the spectrum a fingerprint for identifying the element.
- �� Option A → Different elements have different numbers of electrons.
- �� Option C → Continuous spectra do not explain line-spectrum uniqueness.
- �� Option D → Spectral lines arise from quantized transitions, not random collisions.
Used
- Concept Application
Application:
- Relate atomic structure to spectral lines.
Final Logic:
- Unique energy levels produce unique spectral fingerprints.
Unique Levels = Unique Lines
6 Given En = −13.6/n² eV, the maximum unique wavelength (λmax) corresponding to a transition out of the first excited state (n=2) down to the ground state (n=1) is derived from the energy difference ΔE = hc/λmax. The exact analytical expression for ΔE in joules is:
�� E₁ = −13.6 eV. �� E₂ = −3.4 eV. �� ΔE = 10.2 eV.
ΔE = E₂ − E₁ = (−3.4) − (−13.6) = 10.2 eV = 13.6 × (3/4) eV Converting to joules: ΔE = 13.6 × (3/4) × 1.6 × 10⁻¹⁹ J Thus option A is correct.
- �� Option B → Gives only half of 13.6 eV.
- �� Option C → Energy emitted is positive, not negative.
- �� Option D → Represents 3.4 eV, not 10.2 eV.
Used
- Substitution
Application:
- Substitute n = 1 and n = 2 into the energy formula.
Final Logic:
- Energy difference equals 10.2 eV.
2 → 1 = 10.2 eV
7 If the orbital radius of an electron in a hydrogen atom is 5.3 × 10⁻¹¹ m in the ground state (n=1), what is the exact absolute energy required to remove the electron completely (Ef = 0) if it is currently orbiting in the n=2 excited state?
�� Ionisation energy depends on present state. �� E₂ = −3.4 eV. �� Need 3.4 eV to reach zero energy.
The total energy of hydrogen in the n-th orbit is En = −13.6/n² eV For n = 2, E₂ = −13.6/4 = −3.4 eV To remove the electron completely, it must be brought to E = 0 eV. Required energy = 0 − (−3.4) = 3.4 eV Hence option C is correct.
- �� Option A → Ionisation energy from ground state.
- �� Option B → Excitation energy from n = 1 to n = 2.
- �� Option D → Energy of n = 3 bound state magnitude.
Used
- Substitution
Application:
- Use En = −13.6/n² eV directly.
Final Logic:
- Ionisation energy equals magnitude of bound-state energy.
Ionise from n = 2 → 3.4 eV
8 Match the calculated total energy state in a hydrogen atom to its physical significance.
| List I | List II |
|---|---|
| 1. −13.6 eV | a. Energy of a completely removed electron at rest |
| 2. −3.40 eV | b. Energy required to excite a ground-state electron to the first excited state |
| 3. 0 eV | c. Minimum energy to ionise from ground state (expressed as a bound state value) |
| 4. 10.2 eV | d. First excited state bound energy |
�� −13.6 eV is ground-state energy. �� −3.4 eV is first excited state. �� 0 eV corresponds to free electron.
1 → c : −13.6 eV represents the ground-state bound energy and its magnitude equals the ionisation energy. 2 → d : −3.40 eV is the first excited-state energy. 3 → a : 0 eV corresponds to a completely free electron. 4 → b : 10.2 eV is the excitation energy from n = 1 to n = 2. Thus, option B is correct.
- �� Option A → Multiple incorrect assignments.
- �� Option C → Ground state and free-electron energies are mismatched.
- �� Option D → Incorrect pairing of first excited state and free electron.
Used
- Option Grouping
Application:
- Match each energy value with its physical meaning.
Final Logic:
- Only option B correctly matches all four quantities.
Ground, Excited, Free, Excitation
9 Incorrect statement about discrete transitions from highly excited states directly to the ground state (n=1):
�� Bohr orbits are stable. �� Transitions are discrete. �� Spectra are line spectra.
Bohr's model states that electrons occupy stable stationary states and do not spiral into the nucleus. Radiation is emitted only during transitions between allowed energy levels. Therefore, the emitted frequency is discrete and not continuously varying. Hence option B is correct.
- �� Option A → Correct for the first Lyman transition.
- �� Option C → Correctly states Bohr's frequency condition.
- �� Option D → Hydrogen produces discrete spectral lines.
Used
- Elimination
Application:
- Identify the statement inconsistent with Bohr theory.
Final Logic:
- Continuous spiralling radiation belongs to classical theory, not Bohr theory.
Bohr = Jumps, Not Spirals
10 When an electron in a hydrogen atom falls to the n=3 state from a theoretically infinite quantum number (n → ∞), the energy of the emitted photon approaches a limiting mathematical value. This precise limit corresponds exactly to:
�� E∞ = 0 eV. �� E₃ = −1.51 eV. �� Limit equals |E₃|.
For n → ∞, E∞ = 0 eV For n = 3, E₃ = −13.6/9 = −1.51 eV Energy emitted: ΔE = 0 − (−1.51) = 1.51 eV Thus the series limit for transitions ending at n = 3 equals 1.51 eV. Therefore option B is correct.
- �� Option A → Refers to ground-state ionisation energy (13.6 eV).
- �� Option C → Represents 10.2 eV transition energy.
- �� Option D → E∞ equals zero, not infinite bound energy.
Used
- Substitution
Application:
- Use the hydrogen energy-level formula for n = 3 and n = ∞.
Final Logic:
- Series limit equals the ionisation energy from the final level.
Paschen Limit = |E₃|
11 Correct statements about the wave-particle dual nature implication for Bohr orbits:
1. Bohr's specific stable orbits are a direct mathematical consequence of the electron behaving as a particle wave that forms resonant standing waves.
2. The de Broglie wavelength strictly equals h/mvn when the electron speed is significantly less than the speed of light.
3. The wave-particle duality completely and entirely replaces the classical electrostatic force in determining physical orbit stability.
4. Only resonant standing waves uniquely avoid rapid destructive interference upon cyclic reflection within the orbit.
�� Electron exhibits wave nature. �� Stable orbits correspond to standing waves. �� Coulomb force still governs orbital motion.
Statement 1 is correct because de Broglie's hypothesis explains Bohr's stable orbits as standing matter waves. Statement 2 is correct because for non-relativistic speeds, λ = h/mv. Statement 3 is incorrect because wave-particle duality does not replace the electrostatic attraction between the electron and nucleus. Statement 4 is correct because only standing-wave configurations remain self-consistent and avoid destructive interference. Therefore, statements 1, 2 and 4 are correct.
- �� Option B → Includes statement 3, which is incorrect.
- �� Option C → Includes statement 3, which is incorrect.
- �� Option D → Includes statement 3, which is incorrect.
Used
- Elimination
Application:
- Check each statement using de Broglie's interpretation of Bohr orbits.
Final Logic:
- Only statements 1, 2 and 4 are valid.
Standing Wave = Stable Orbit
12 Substituting the classical velocity expression vn = e / √(4πε₀mrn) into the fundamental de Broglie wavelength equation λ = h/mvn, we find λ strictly depends on the radius rn as:
�� λ = h/mv �� v ∝ 1/√r �� Therefore λ ∝ √r
Given v ∝ 1/√rn and λ = h/mv Therefore, λ ∝ 1/v ∝ √rn Hence, the de Broglie wavelength varies as the square root of the orbital radius. Therefore, option A is correct.
- �� Option B → No quadratic dependence exists.
- �� Option C → Wavelength increases, not decreases, with radius.
- �� Option D → Dependence is square root, not linear.
Used
- Substitution
Application:
- Substitute the velocity-radius relation into the de Broglie equation.
Final Logic:
- λ varies directly as √rn.
v ↓ ⇒ λ ↑
13 In analogizing de Broglie particle waves on a circular orbit to mechanical waves vibrating on a fixed string:
1. Both macroscopic and microscopic systems excite exactly a single wavelength when randomly disturbed.
2. Both require defined nodes at the boundary ends, translating to exactly an integer number of full wavelengths fitting the circumference.
3. Both necessarily result in a continuously changing broad spectrum of electromagnetic radiation.
4. Neither physical system relies fundamentally on the geometric dimensions of the string or orbit.
�� Standing waves require boundary conditions. �� Integer wavelengths fit the path. �� Geometry determines allowed modes.
Statement 2 is correct because standing waves are formed only when an integral number of wavelengths fit the allowed length or circumference. Statement 1 is incorrect because multiple harmonics can be excited. Statement 3 is incorrect because standing waves do not necessarily produce electromagnetic radiation. Statement 4 is incorrect because the dimensions of the string or orbit determine the allowed wavelengths. Therefore, only statement 2 is correct.
- �� Option A → Statement 1 is incorrect.
- �� Option C → Statement 3 is incorrect.
- �� Option D → Statements 1 and 4 are incorrect.
Used
- Elimination
Application:
- Compare standing waves on strings with de Broglie standing waves.
Final Logic:
- Only statement 2 correctly describes both systems.
Integer λ Fits
14 Statements conceptually concerning the standing wave relation 2πrn = nλ:
1. It dictates that rn can dynamically take any continuous fractional value.
2. It leads directly to Bohr's specific quantisation condition of angular momentum.
3. It demonstrates why hypothetical orbits with non-integer wavelength fractions rapidly decay to zero amplitude.
4. It implies that the total distance travelled by the electron wave down the orbit and back is a perfect integer number of wavelengths.
�� Circumference must contain integer wavelengths. �� Leads to angular momentum quantisation. �� Non-resonant waves cancel out.
Statement 1 is incorrect because quantisation restricts allowed radii. Statement 2 is correct since 2πr = nλ directly leads to mvr = nh/2π. Statement 3 is correct because non-integer wavelength fitting causes destructive interference. Statement 4 is correct because the orbital path accommodates an integral number of wavelengths. Therefore, statements 2, 3 and 4 are correct.
- �� Option A → Includes statement 1, which is incorrect.
- �� Option C → Includes statement 1, which is incorrect.
- �� Option D → Includes statement 1, which is incorrect.
Used
- Elimination
Application:
- Apply the standing-wave condition.
Final Logic:
- Only statements 2, 3 and 4 follow from 2πr = nλ.
Integer λ → Quantisation
15 If the orbital radius of a hydrogen atom in the ground state (n=1) is 5.3 × 10⁻¹¹ m, what is the exact analytical quantum condition required for the angular momentum in the second excited state (n=3)?
�� Second excited state means n = 3. �� Bohr condition: L = nh/2π. �� L = 3h/2π = 1.5h/π.
Bohr's quantisation condition is L = mvr = nh/2π For n = 3, L = 3h/2π = 1.5h/π Hence, option B is correct.
- �� Option A → Twice the correct value.
- �� Option C → Corresponds to n = 1.
- �� Option D → Corresponds to n = 9.
Used
- Substitution
Application:
- Substitute n = 3 into Bohr's angular momentum equation.
Final Logic:
- Second excited state corresponds to n = 3.
n = 3 ⇒ 3h/2π
16 The core physical reason an atom does not collapse continuously as originally predicted by classical electromagnetic theory is because the electron strictly resides in _______ states where its particle wave forms a completely _______ wave.
�� Electrons occupy stationary states. �� Matter waves form standing waves. �� Stable configurations persist.
Modern quantum interpretation explains atomic stability through stationary states associated with standing matter waves. In such states, electrons do not radiate continuously as predicted classically. Therefore, the correct pair is Stationary, Standing.
- �� Option A → Continuous travelling waves do not explain atomic stability.
- �� Option B → Spiral motion is contrary to stable atomic structure.
- �� Option C → Accelerated continuous motion reflects classical collapse.
Used
- Contextual/Tonal Matching
Application:
- Identify the terminology associated with atomic stability.
Final Logic:
- Stable atoms require stationary states and standing waves.
Stationary = Stable
17 Match the atomic system with its theoretical compatibility with Bohr's original model.
| List I | List II |
|---|---|
| 1. Hydrogen atom (Z = 1) | a. Fails completely due to electron-electron interactions |
| 2. Helium atom (2 electrons) | b. Hydrogenic model, gross features predicted correctly |
| 3. Singly ionised helium (He⁺) | c. Hydrogenic model, Z = 2 |
| 4. Doubly ionised lithium (Li²⁺) | d. Hydrogenic model, Z = 3 |
�� Bohr model works for one-electron systems. �� Helium has electron-electron interactions. �� Hydrogenic ions follow Bohr predictions.
1 → b : Hydrogen atom is the ideal Bohr system. 2 → a : Helium contains two electrons, causing electron-electron interactions neglected by Bohr theory. 3 → c : He⁺ is a one-electron hydrogenic ion with Z = 2. 4 → d : Li²⁺ is a one-electron hydrogenic ion with Z = 3. Thus, option A is correct.
- �� Option B → Hydrogen and helium are mismatched.
- �� Option C → He⁺ is incorrectly matched.
- �� Option D → Hydrogen atom is incorrectly assigned.
Used
- Option Grouping
Application:
- Identify which systems contain only one electron.
Final Logic:
- Only option A correctly matches all systems.
One Electron = Bohr Works
18 Incorrect statement about the theoretical transition likelihoods in Bohr's model:
�� Bohr model predicts energies. �� It does not predict intensities. �� Transition probabilities require quantum mechanics.
A major limitation of Bohr's model is that it cannot predict transition probabilities or relative spectral line intensities. These quantities are explained by quantum mechanics through selection rules and wave functions. Hence, option A is correct.
- �� Option B → Experimentally observed spectral intensities vary.
- �� Option C → This is a known limitation of Bohr theory.
- �� Option D → Correctly describes the hybrid nature of the model.
Used
- Elimination
Application:
- Identify a known limitation of Bohr's theory.
Final Logic:
- Intensity prediction lies beyond the Bohr model.
Bohr Gives Energy, Not Intensity
19 When attempting to cleanly extend the Bohr model to complex multi-electron atoms, the theoretical analysis failed primarily because:
�� Multi-electron atoms involve repulsion. �� Electron-electron interaction is significant. �� Bohr model ignores this effect.
Bohr's model successfully describes hydrogen-like atoms with one electron. In multi-electron atoms, electron-electron repulsion significantly affects energy levels, and Bohr's theory cannot account for these interactions. Therefore, option B is correct.
- �� Option A → Classical physics alone cannot explain atomic structure.
- �� Option C → Multi-electron atoms still possess a nucleus.
- �� Option D → Electrical forces dominate gravitational forces.
Used
- Elimination
Application:
- Identify the major limitation in extending Bohr's model.
Final Logic:
- Electron-electron interactions are the key difficulty.
Many Electrons = Many Interactions
20 How does modern quantum mechanics explicitly redefine the basic conceptual framework of the Bohr model?
�� Electrons are described by wave functions. �� Orbitals replace fixed orbits. �� Probability replaces exact trajectories.
Modern quantum mechanics describes electrons through wave functions and probability distributions. Instead of definite Bohr orbits, electrons occupy orbitals, which are regions of high probability of finding the electron. Therefore, option B is correct.
- �� Option A → Exact classical trajectories are not accepted.
- �� Option C → Quantised energy levels remain fundamental.
- �� Option D → For hydrogen-like atoms, energy primarily depends on n in a pure Coulomb field.
Used
- Odd One Out
Application:
- Identify the statement consistent with modern quantum mechanics.
Final Logic:
- Orbitals and probability distributions replace fixed Bohr orbits.
Orbit → Orbital
