Bohr model
Summary
The Bohr model pictures the hydrogen electron in circular orbits with fixed, quantized energies. Light is absorbed or emitted when the electron jumps between levels, and the photon energy equals the energy gap. It fits one-electron species well but was replaced by the quantum mechanical model.
Detail
Meaning: Bohr pictured the electron in hydrogen moving in circular orbits of fixed energy, labeled by the principal quantum number n = 1, 2, 3 … The electron does not radiate while in an orbit. It changes level by absorbing or emitting a photon whose energy equals the gap between the two levels. Energies are negative (bound) and rise toward zero as n → ∞, where the electron is free. This explains why hydrogen shows a discrete line spectrum.
Equation: En = −2.18 × 10⁻¹⁸ J × Z²/n² and ΔE = hf = hc/λ. En is the level energy (J), Z is nuclear charge (unitless), n is the principal quantum number (unitless), h is 6.63 × 10⁻³⁴ J·s, f is frequency (Hz), c is 3.00 × 10⁸ m/s, and λ is wavelength (m).
On the MCAT: A passage gives a transition such as n = 3 → 2 and asks for photon energy or wavelength, or whether light is absorbed or emitted. A larger ΔE means higher frequency and shorter wavelength. Transitions down to n = 1 give ultraviolet light; those down to n = 2 include visible light.
Common confusion: Bohr's orbits are not the modern picture. The quantum mechanical model describes orbitals as probability distributions, and the Bohr energy formula works quantitatively only for one-electron species (H, He⁺, Li²⁺). Also, levels crowd together as n rises, so 2 → 1 releases much more energy than 4 → 3.
Sources
- Chemistry: The Central Science
- Chemistry (Zumdahl)
- General Chemistry (Ebbing and Gammon)
Written for the MCAT and checked before it was published. For study reference only. Spotted an error? Let us know.