Stationary Orbits
Electrons revolve only in selected orbits without radiating electromagnetic energy.
A complete exam-oriented study of Bohr's postulates, quantised orbits, radius, velocity, energy, ionisation and hydrogen spectral series.
Rutherford's nucleus combined with quantum rules for electrons.
Bohr retained Rutherford's small positive nucleus but proposed that electrons may revolve only in certain permitted circular orbits. While in a stationary orbit an electron does not radiate energy.
Each orbit has a definite radius, speed and energy. Radiation is emitted or absorbed only when an electron jumps between two permitted states.
Electrons revolve only in selected orbits without radiating electromagnetic energy.
Permitted orbits satisfy mvr=nh/2π, where n=1,2,3...
A photon is emitted or absorbed when an electron changes state: hν=|E₂−E₁|.
The condition can be understood as a standing de Broglie wave: 2πr=nλ. Only an integral number of wavelengths can fit around a stable circular orbit.
The electrostatic force provides centripetal acceleration:
Together with angular-momentum quantisation, this selects discrete radii and energies. An electron in one of these stationary states does not continuously lose energy.
Radius increases as n² and decreases with nuclear charge Z. For hydrogen, r₁=a₀ and r₂=4a₀.
Combining Coulomb force with mvr=nh/2π gives:
rₙ = ε₀h²n²/(πmZe²)
For a fixed Z, electron speed decreases as 1/n. For the ground-state hydrogen atom, v₁≈2.18×10⁶ m s⁻¹.
Ionisation takes the electron from a bound state to n=∞, where E=0.
Ionisation potential of hydrogen in its ground state is 13.6 V.
A downward transition emits a photon; an upward transition requires absorption of exactly the energy difference.
Because energies are quantised, only selected photon wavelengths occur, producing a line spectrum.
Radius, velocity, energy, excitation, ionisation, wavelengths and series identification.
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Additional CBSE, NEET, JEE, IB, IGCSE, ICSE, A-Level, assertion-reason and case-study questions with answers.
Electrons revolve only in certain permitted stationary orbits without radiating energy.
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mvr = nh/2π, where n = 1, 2, 3, ...
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Because electrons can exist only in discrete energy levels and emit photons of definite energy during transitions.
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13.6 eV.
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Balmer series, because transitions terminate at n = 2.
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Energy required to raise an electron from lower energy level to a higher bound energy level.
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E_n = -13.6/n² eV.
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Helium has two electrons, so electron-electron interaction is present; Bohr model works exactly only for one-electron atoms.
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a0 = 5.29 × 10^-11 m.
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Lyman series, in ultraviolet region.
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E2 = -13.6/4 = -3.4 eV.
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ΔE = -3.4 - (-13.6) = 10.2 eV.
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r3 = 9a0 = 9 × 5.29 × 10^-11 m.
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Balmer series.
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13.6/4 = 3.4 eV.
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E1 = -13.6Z² = -13.6 × 4 = -54.4 eV.
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r1 = a0/Z = a0/3.
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v2 = 2.18×10^6/2 = 1.09×10^6 m/s.
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n = ∞ to n = 1.
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n = 3 to n = 2.
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2→1 gives maximum energy because energy gap is greatest among these.
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L = 3h/2π.
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It decreases as 1/Z.
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E3 = -13.6/9 = -1.51 eV.
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ΔE = 10.2 eV; wavelength = 1240/10.2 ≈ 121.6 nm.
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Infrared region.
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E_n ∝ -Z²/n².
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N = n(n-1)/2 = 4×3/2 = 6.
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Balmer series.
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n = ∞ to n = 2.
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ΔE = 13.6(1/2² - 1/3²)=1.889 eV, λ=1240/1.889≈656 nm.
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Energy at final state = -13.6+12.09=-1.51 eV = -13.6/n², so n=3.
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N = 5×4/2 = 10.
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Ionisation energy = 54.4 eV, so ionisation potential = 54.4 V.
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r(H,n=2)=4a0; r(He+,n=1)=a0/2; ratio=8.
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v ∝ Z/n. H:1/1=1, He+:2/2=1, ratio=1.
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ΔE=13.6(1/4-1/16)=2.55 eV.
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ΔE=10.2 eV=10.2×1.6×10^-19 J; ν=ΔE/h≈2.47×10^15 Hz.
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Transition 2→1; λ≈121.6 nm.
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n=3 to n=2.
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ΔE=13.6×4(1-1/4)=40.8 eV.
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L=4h/2π=2h/π.
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v/4.
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r=4a0/2=2a0.
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E=-13.6×9/9=-13.6 eV.
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It can ionise the atom, electron just escapes with zero kinetic energy.
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15 - 13.6 = 1.4 eV.
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ΔE=13.6 eV; λ=1240/13.6≈91.2 nm.
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ΔE=13.6/4=3.4 eV; λ=1240/3.4≈365 nm.
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(-13.6/16)/(-13.6/4)=1/4.
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For a stable orbit, electron wave must join smoothly after one round: 2πr=nλ. With λ=h/mv, this gives mvr=nh/2π.
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It ignores electron-electron repulsion and cannot solve coupled motion exactly.
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Zero energy is chosen at infinite separation; bound electron has less energy than a free electron at infinity.
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Transition energy increases as Z².
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Energy levels vary as -1/n², so separation decreases as n becomes large.
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No. Bound-bound absorption requires exactly matching energy gap; larger sufficient photon may ionise.
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Transitions to n=2 have smaller energy than transitions to n=1, so longer wavelengths lie in visible region.
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From n=3 it is 13.6/9 eV, much smaller than 13.6 eV from ground state.
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It corresponds to transition from n=∞ to a fixed lower level, giving maximum photon energy in that series.
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To avoid classical collapse of the Rutherford atom and explain discrete spectra.
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Electrons emit photons only during transitions between quantised levels; each transition gives a definite wavelength.
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E=1240/656≈1.89 eV.
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Lowest energy state of an atom.
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A state with energy higher than ground state but still bound.
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Atoms emit photons of specific wavelengths due to transitions between discrete energy levels.
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It moves to a higher allowed energy level.
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It is not absorbed for that transition.
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Ionisation raises electron to E=0 level, corresponding to complete removal from atom.
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1/λ = R(1/n1² - 1/n2²).
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Spectral lines identify hydrogen and reveal physical properties and motion of stars.
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Both true; Reason correctly explains Assertion.
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Both true; Reason correctly explains Assertion.
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Both true; Reason correctly explains Assertion.
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Both true; Reason correctly explains Assertion.
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Assertion false; Reason false.
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Maximum lines = n(n-1)/2 = 6.
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n=2.
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He+ energy is Z²=4 times hydrogen, so 40.8 eV.
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From ground state, final state is n=2.
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Lyman-alpha transition, n=2 to n=1.
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