The Hydrogen Spectrum
Sharp lines that classical physics couldn't explain.
Lesson at a glanceShow the key points
- Hydrogen emits sharp lines in series: Lyman (UV), Balmer (visible), Paschen (IR)…
- 1/λ = R(1/n² − 1/m²) (43.1), R = 1.097 × 10⁷ m⁻¹.
- Classically an orbiting electron radiates and spirals in: atoms should collapse.
A hot solid glows with every colour. Hot hydrogen glows with just a few sharp ones, the same everywhere in the universe. Those lines were a fingerprint no classical theory could explain.
Line spectra
A lamp filament, sent through a prism, gives a continuous spectrum. Hydrogen heated in a sealed tube gives a line spectrum: only certain sharp wavelengths, such as 656.3 nm and 486.1 nm, with nothing in between. Hydrogen also emits lines in the ultraviolet and infrared.
The lines fall into series. Within each series the gaps shrink toward shorter wavelengths, approaching a series limit: the Lyman series (ultraviolet), the Balmer series (visible), the Paschen series (infrared), and so on. All the wavelengths fit one formula:
Find the wavelengths of the 3 → 2 and 4 → 2 Balmer lines, and the Lyman series limit.
Why Rutherford’s atom can’t be right
Hydrogen is one electron and one proton. In Rutherford’s picture the electron circles the proton, the Coulomb force supplying the centripetal force. Mechanically fine, but Maxwell’s equations say an accelerating charge must radiate continuously. So the electron should lose energy, spiral inward, and crash into the proton, emitting a smoothly changing range of wavelengths on the way.
Reality: hydrogen at room temperature is perfectly stable and emits nothing. When excited by heat or a discharge it emits only those sharp wavelengths, always the same, from a lab in Delhi to the Sun. Classical physics had no explanation: something new was needed.
- 1Hydrogen emits sharp lines in series (Lyman UV, Balmer visible, Paschen IR…) with series limits.
- 21/λ = R(1/n² − 1/m²) (43.1).
- 3Classically an orbiting electron should radiate and spiral in: atoms would collapse and give continuous spectra.
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Keep exploring
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