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Hydrogen spectral series — transitions to n = 1 (UV region)
Rydberg Formula
1/λ = RH × (1/1² − 1/n²)
RH = 1.09737 × 10⁷ m⁻¹
E = hc/λ | ν = c/λ
| Transition | n = 2 → n = 1 |
| Wavelength (λ) | 121.502 nm |
| Frequency (ν) | 2.4674 PHz (2.4674e+15 Hz) |
| Photon energy (eV) | 10.2043 eV |
| Photon energy (J) | 1.6349e-18 J |
| Region | Ultraviolet (UV) |
| n | Name | λ (nm) | Energy (eV) | Frequency (PHz) | Region |
|---|---|---|---|---|---|
| 2 | Lyman α | 121.502 | 10.2043 | 2.4674 | Ultraviolet (UV) |
| 3 | Lyman β | 102.518 | 12.0939 | 2.9243 | Ultraviolet (UV) |
| 4 | Lyman γ | 97.202 | 12.7553 | 3.0842 | Ultraviolet (UV) |
| 5 | Lyman δ | 94.924 | 13.0615 | 3.1582 | Ultraviolet (UV) |
| 6 | Lyman ε | 93.730 | 13.2278 | 3.1985 | Ultraviolet (UV) |
| 7 | Lyman ζ | 93.025 | 13.3280 | 3.2227 | Ultraviolet (UV) |
| ∞ | Series limit (ionization) | 91.127 | 13.6057 | 3.2898 | Ultraviolet (UV) |
Click any row to select that line.
Note
All Lyman series lines fall in the ultraviolet region (λ < 400 nm). They were discovered by Theodore Lyman in 1906–1914.
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Bohr model, Rydberg formula, photon energy, wavelength, and spectral series
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