6.2 The Bohr Model

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Vocabulary flashcards covering key Bohr model concepts from the lecture notes.

Last updated 6:05 AM on 8/20/25
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17 Terms

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Bohr model

Quantum model of the hydrogen atom with electrons in quantized circular orbits; photons are emitted or absorbed during transitions between orbits.

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Hydrogen atom

Simplest atom with one proton nucleus and one electron; the system Bohr used to develop his model.

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Stationary state hypothesis

Electron does not radiate while in a stationary orbit; radiation occurs only when transitioning between different orbits.

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Photon

Quantum of light energy emitted or absorbed during a transition between energy levels (energy = hν = hc/λ).

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Planck's constant (h)

Fundamental constant relating energy and frequency (E = hν); appears in Bohr’s and photon energy relations.

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Rydberg equation

Relation for hydrogen spectral lines: 1/λ = R(1/n1^2 − 1/n2^2); R is the Rydberg constant.

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Rydberg constant (R)

Constant used in the Rydberg equation; Bohr calculated a value that matched experimental results.

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Quantized energy levels

Energies of electrons in atoms occur in discrete values described by quantum numbers.

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Principal quantum number (n)

Integer label for electron energy levels (n = 1, 2, 3, …).

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Ground state

Lowest energy electronic state of an atom (n = 1 for hydrogen).

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Excited state

Any higher energy state (n > 1) reached by absorbing energy.

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Hydrogen-like atoms

One-electron ions such as He+, Li2+, Be3+; energy levels depend on the nuclear charge Z.

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Bohr radius (a0)

Distance scale of the hydrogen ground-state orbit; a0 ≈ 5.292×10^−11 m.

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Hydrogen-like energy formula

E_n = −k Z^2 / n^2, with k = 2.179×10^−18 J; describes energy of the nth orbit in a hydrogen-like atom.

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Ionization energy

Energy required to remove the electron completely (E → 0); for hydrogen ground state, ΔE = k = 2.179×10^−18 J.

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Ionization limit

Energy level E = 0 corresponding to n → ∞; electron is no longer bound to the nucleus.

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Limitations of Bohr model

Could not account for electron–electron interactions in multi-electron atoms; quantum mechanics later provided a better model.

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