Exams › JEE Main › Physics › Atoms
170 questions with worked solutions.
Answer: 4: 3
Number of spectral lines = n(n-1)/2, so 3 lines -> n1 = 3 and 6 lines -> n2 = 4. Orbital speed v is proportional to 1/n, so v1:v2 = (1/3):(1/4) = 4:3.
Answer: 2.10 × 10⁻³⁴ Js
E = -13.6/n^2 = -3.4 eV gives n = 2. Angular momentum L = n*hbar = 2 * 1.055 x 10^-34 = 2.11 x 10^-34 Js.
Answer: 2 lines in the Lyman series and 1 line in the Balmer series
From n=1, exciting to n=3 needs 12.09 eV (possible) but to n=4 needs 12.75 eV (>12.5 eV, not possible). Allowed transitions are 3->1, 2->1 (Lyman, 2 lines) and 3->2 (Balmer, 1 line): 2 Lyman + 1 Balmer.
Answer: L_H = L_Li and |E_H| < |E_Li|
Both are in the second excited state (n=3), so angular momentum L = nh/2pi is the same: L_H = L_Li. Energy |E| = 13.6 Z^2/n^2, and Li++ has Z=3 vs Z=1 for H, so |E_H| < |E_Li|.
Answer: rₙ is directly proportional to n
With V = V0 ln(r/r0), force F = V0/r. Setting mv^2/r = V0/r gives mv^2 = V0, so v is constant. Bohr quantization mvr = n*hbar then gives r_n ∝ n.
Answer: 823 nm
Longest UV is Lyman 2->1: 1/122 = R(3/4) -> R = 1/91.5 nm^-1. Shortest IR is the Paschen series limit (inf->3): lambda = 9/R = 9*91.5 = 823 nm.
Answer: three
Absorbing 12.1 eV from the ground state lifts the atom to E = -13.6 + 12.1 = -1.5 eV, i.e. n = 3. De-excitation from n = 3 gives 3(3-1)/2 = 3 spectral lines.
Answer: 20/7
The ratio of emitted wavelengths in transitions between energy levels in a hydrogen atom is inversely proportional to the energy differences between those levels. The energy difference for each transition can be calculated using the Rydberg formula, leading to the ratio of wavelengths being 20/7 for the specified transitions.
Answer: 1.46 × 10⁶ m/s
Orbital speed v_n = (Z/n)*2.18x10^6 m/s. For He+ with Z = 2, n = 3: v = (2/3)*2.18x10^6 ~ 1.46x10^6 m/s.
Answer: 2 × 10⁷ m/s
Redshift delta lambda = 706 - 656 = 50 nm. v = c (delta lambda / lambda) = 3 x 10^8 x (50/656) = 2.3 x 10^7 m/s ~ 2 x 10^7 m/s.
Answer: ν1 − ν2 = ν3
nu1 = Rc (Lyman limit), nu2 = Rc(1 - 1/4) = (3/4)Rc (first Lyman line), nu3 = Rc/4 (Balmer limit). Then nu1 - nu2 = Rc/4 = nu3.
Answer: -30.6 eV
E = -13.6*Z^2/n^2 eV. For Li2+ (Z = 3) in the first excited state (n = 2): E = -13.6*9/4 = -30.6 eV.
Answer: 6
Second Balmer line of H is 4->2: 1/lambda = R(1/4 - 1/16) = 3R/16. For Li2+ (Z=3): 1/lambda = 9R(1/x^2 - 1/12^2). Setting 9(1/x^2 - 1/144) = 3/16 gives 1/x^2 = 1/36, so x = 6.
Answer: Tₙ does not depend on n, and rₙ varies as n
For F = k/r, mv^2/r = k/r gives mv^2 = k (constant), so kinetic energy T_n = k/2 is independent of n. Bohr quantization mvr = n*hbar then gives r_n ∝ n.
Answer: 79.0
To remove both electrons from a neutral helium atom, you need to account for the energy required to remove the first electron (24.6 eV) and the increased energy needed to remove the second electron due to the positive charge of the helium ion formed after the first electron is removed. The total energy required is 24.6 eV for the first electron plus 54.4 eV for the second, resulting in 79.0 eV.
Answer: Its kinetic energy rises, while its potential energy and total energy both fall.
Dropping to a lower n makes total energy more negative (falls) and KE = -E_total increases (rises), while PE = 2*E_total becomes more negative (falls). So KE rises while PE and total energy both fall.
Q17. The formation of covalent bonds in compounds demonstrates the:
Answer: wave character of the electron
Covalent bonds involve the sharing of electron pairs between atoms, which is best described by the wave nature of electrons as it allows for the overlapping of atomic orbitals, leading to stable bond formation.
Answer: Tₙ does not depend on n, and rₙ varies as n
In the Bohr model, the kinetic energy of the electron in a hydrogen-like atom is constant for all orbits, meaning it does not depend on the principal quantum number n. However, the radius of the allowed orbits increases linearly with n, leading to the conclusion that Tₙ remains constant while rₙ varies with n.
Answer: 5 → 4
Transition energy scales with (1/nf^2 - 1/ni^2). For 4->3 it is 0.0486 (UV). The only transition with a SMALLER gap (longer wavelength = IR) is 5->4 (1/16 - 1/25 = 0.0225). 3->2, 4->2 and 2->1 all have larger gaps, so they are more energetic, not IR.
Q20. Energy required for the electron excitation in Li++ from the first to the third Bohr orbit is:
Answer: 108.8 eV
For Li++ (Z=3): E = 13.6*Z^2*(1/1^2 - 1/3^2) = 13.6*9*(8/9) = 108.8 eV.
Answer: 6
From an excited state n = 4 down to ground, the number of distinct spectral lines is n(n-1)/2 = 4*3/2 = 6.
Answer: 1/n³
E_n = -RhcZ^2/n^2, so for n -> (n-1) the energy gap ~ 2Rhc/n^3 for large n. Hence the emitted frequency is proportional to 1/n^3.
Answer: λ₁ = λ₂ = 4λ₃ = 9λ₄
For n=2->1, 1/lambda is proportional to Z^2*(3/4), so lambda ~ 1/Z^2. H and D both have Z=1 (same wavelength), He+ has Z=2 (1/4), Li2+ has Z=3 (1/9). Hence lambda1 = lambda2 = 4*lambda3 = 9*lambda4.
Answer: its kinetic energy increases but potential energy and total energy decrease
As the electron transitions to a lower energy state, it moves closer to the nucleus, which increases its kinetic energy due to the attractive force. However, the potential energy decreases because it is at a lower energy level, resulting in a decrease in total energy.
Answer: Λₙ ≈ A + B/λₙ²
For the n->1 transition, 1/Lam_n = R(1 - 1/n^2), so Lam_n = 1/[R(1-1/n^2)] ~= (1/R)(1 + 1/n^2). Since the de Broglie wavelength lam_n is proportional to n, 1/n^2 is proportional to 1/lam_n^2, giving Lam_n ~= A + B/lam_n^2.
Answer: ν_L/25
The series limit frequency of the P-fund series is derived from the energy levels of the hydrogen atom, specifically the transition from the n=5 level to the ionization limit, which results in a frequency that is 1/25th of the series limit frequency of the Lyman series, which corresponds to transitions from n=2 to the ionization limit.
Answer: 488.9 nm
The wavelength of the second Balmer line can be calculated using the Rydberg formula for hydrogen, which shows that the wavelengths decrease as the initial energy level increases. Since the first Balmer line corresponds to a transition from n=3 to n=2, the second line from n=4 to n=2 will have a shorter wavelength, which is correctly calculated to be 488.9 nm.
Answer: 7.8 × 10¹⁴
The frequency of revolution is inversely proportional to the time period of revolution. Since the time period for the ground state is given, we can use the relationship between energy levels and their corresponding frequencies to determine that the first excited state has a shorter time period, resulting in a higher frequency of 7.8 × 10¹⁴ s⁻¹.
Answer: 1/n³
The frequency of radiation emitted during a transition between energy levels in a hydrogen-like atom is determined by the difference in energy levels, which is inversely proportional to the square of the principal quantum number. For large n, this relationship simplifies to being proportional to 1/n³.
Answer: 1.214 × 10⁻⁷ m
The energy difference between the two levels (n=1 and n=2) in a hydrogen atom can be calculated using the formula provided, and then the wavelength can be determined using the relationship between energy and wavelength (E = hc/λ). The correct option corresponds to the wavelength that matches the calculated energy difference for the transition.
Answer: λ1 = λ2 = 4λ3 = 9λ4
The wavelengths of emitted radiation during electron transitions are inversely proportional to the energy levels of the electrons in the atoms. Since the energy levels depend on the atomic number and the electron configuration, the ratios of the wavelengths can be derived from the differences in these energy levels for each atom. In this case, the correct option reflects the relationship between the wavelengths based on the respective atomic structures and their transitions.
Answer: its kinetic energy increases but potential energy and total energy decrease
When an electron transitions from an excited state to the ground state, it releases energy, which results in a decrease in total energy. As it moves closer to the nucleus, its potential energy becomes more negative (increases in magnitude), while its kinetic energy increases due to the conservation of energy.
Answer: 79 eV
The energy to remove the first electron from a neutral Helium atom is approximately 24.6 eV. Since the energy required to remove the second electron from the singly ionized Helium atom is 2.2 times that, it amounts to about 54.6 eV. Adding these two values gives a total of approximately 79 eV for complete ionization.
Answer: Λₙ ≈ A + B/λₙ²
The correct option indicates that the wavelength of the emitted photon, Λₙ, is inversely related to the square of the de Broglie wavelength of the electron in the n^th state, which aligns with the principles of quantum mechanics where higher energy transitions result in shorter wavelengths of emitted radiation.
Answer: 20/27 λ
For M->L (3->2): 1/lambda = R(1/4 - 1/9) = 5R/36. For N->L (4->2): 1/lambda' = R(1/4 - 1/16) = 3R/16. So lambda'/lambda = (5/36)/(3/16) = 80/108 = 20/27. The emitted wavelength is (20/27) lambda.
Answer: Linear with slope R_H
Wave number nu-bar = R_H(1/n_f^2 - 1/n_i^2) = R_H(1/n^2) - R_H/64. Plotting nu-bar against (1/n^2) gives a straight line of slope +R_H and intercept -R_H/64, so it is linear with slope R_H.
Answer: 9.7 Å
Second excited state means n=3, r=4.65 A. de-Broglie wavelength lambda = 2*pi*r/n = 2*pi*4.65/3 = 9.7 A. So the answer is 9.7 A.
Answer: 20/7
3rd excited (n=4) -> 2nd excited (n=3): 1/lambda1 = R(1/9 - 1/16) = 7R/144. 2nd excited (n=3) -> 1st excited (n=2): 1/lambda2 = R(1/4 - 1/9) = 5R/36. lambda1/lambda2 = (5/36)/(7/144) = 20/7.
Q39. A He⁺ ion is in its first excited state. Its ionization energy is:
Answer: 13.60 eV
The ionization energy of a He⁺ ion in its first excited state corresponds to the energy required to remove an electron from that state, which is calculated using the formula for hydrogen-like atoms. For He⁺, the ionization energy from the ground state is 54.4 eV, and the first excited state corresponds to 13.6 eV, making option B the correct answer.
Answer: The total energy of the electron is maximum when it is at a distance a0 from the nucleus.
For the 1s electron, virial theorem (|PE|=2*KE), max probability density at the nucleus, and finite probability at 2a0 are all correct. The incorrect statement is that total energy is maximum at distance a0 -- the total (orbital) energy is constant and independent of position, so option (3) is the wrong statement.
Answer: 16a0
Photon energy = 12500/980 = 12.76 eV. From n=1 (-13.6 eV) the atom reaches E = -13.6 + 12.76 = -0.85 eV = -13.6/n^2, giving n^2 = 16, n = 4. Radius = n^2 * a0 = 16 a0.
Answer: Paschen, ∞ → 3
For Paschen series limit (infinity -> 3): 1/lambda = R_H/9 = (1e5 cm^-1)/9, giving lambda = 9e-5 cm = 900 nm. So the suitable line is Paschen, infinity -> 3. (Balmer infinity -> 2 gives 400 nm.)
Answer: 9λ₁/5
Shortest Lyman wavelength of H: 1/lambda1 = R(1) so lambda1 = 1/R. Longest Balmer line of He+ (Z=2) is 3->2: 1/lambda = R*4*(1/4 - 1/9) = 5R/9, so lambda = 9/(5R) = (9/5)lambda1.
Answer: 2: 3
Radius r = 0.529 n^2/Z. ΔR(3->4) = (16-9)/Z = 7/Z. For Li2+ (Z=3): ΔR1 = 7/3; for He+ (Z=2): ΔR2 = 7/2. ΔR1:ΔR2 = (7/3):(7/2) = 2:3.
Answer: 7.8 × 10¹⁴
The frequency of revolution is inversely proportional to the time period of revolution. Since the time period for the ground state is known, we can calculate the time period for the first excited state, which is longer due to the electron being further from the nucleus, resulting in a lower frequency. The correct option reflects this calculation, yielding a frequency of 7.8 × 10¹⁴ s⁻¹.
Answer: 11.4 nm
Ionization energy = 9 Ry gives Z^2 = 9. Energy of n=3 -> n=1 transition = Z^2 * 13.6 * (1 - 1/9) = 9*13.6*(8/9) = 108.8 eV. Wavelength = 1240/108.8 = 11.4 nm.
Answer: 6
For a one-electron ion E = -13.6 Z^2/n^2 eV. Carbon has Z = 6, so E = -13.6*36/n^2. Setting this equal to the hydrogen ground state (-13.6 eV) gives n^2 = 36, i.e. n = 6.
Answer: Balmer series
The Balmer series corresponds to electron transitions from higher energy levels to the second energy level, resulting in the emission of visible light, which is why it is the only series among the options that lies in the visible region of the spectrum.
Answer: 2815.2 eV
For a muonic hydrogen atom the ionization energy = 13.6 eV times the mass ratio = 13.6 x 207 = 2815.2 eV (the muon is ~207 times heavier, and energy is proportional to mass).
Q50. A certain orbital has no angular nodes and two radial nodes. The orbital is:
Answer: 3s
No angular nodes means l = 0 (an s orbital). Radial nodes = n - l - 1 = 2 gives n = 3. Hence the orbital is 3s.