The Rydberg equation calculates the wavelength of the light a hydrogen atom emits when its electron drops from a higher level n2 to a lower level n1 (or absorbs when it goes up). Enter the two levels; you get the wavelength in nanometres (in vacuum), the wavenumber and the photon energy in electronvolts.
Formula
1 ÷ λ = RH × (1 ÷ n12 − 1 ÷ n22); E = h × c ÷ λ.
- λ: wavelength in vacuum
- RH = 1.09677583 × 107 m−1, the Rydberg constant for hydrogen (the Rydberg constant R∞ = 1.0973731568 × 107 m−1 corrected for the electron-to-proton mass ratio)
- n1 < n2: whole-number energy levels (n1 = 1 Lyman, 2 Balmer, 3 Paschen series)
- h = 6.62607015 × 10−34 J·s, c = 299,792,458 m/s and e = 1.602176634 × 10−19 C, all exact; 1 eV = e × 1 V
Worked Example
The red Balmer-alpha line of hydrogen, n2 = 3 to n1 = 2.
- 1 ÷ 22 − 1 ÷ 32 = 0.25 − 0.111111 = 0.138889 (exactly 5 ÷ 36)
- 1 ÷ λ = 1.09677583 × 107 × 5 ÷ 36 = 1,523,299.76 m−1, a wavenumber of 15,233.0 cm−1
- λ = 1 ÷ 1,523,299.76 m−1 = 6.564696 × 10−7 m = 656.47 nm
- E = 6.62607015 × 10−34 × 299,792,458 × 1,523,299.76 = 3.02595 × 10−19 J; ÷ 1.602176634 × 10−19 = 1.8887 eV
Assumptions
- The atom is hydrogen (one electron, proton nucleus). For hydrogen-like ions multiply by Z2 and use the matching reduced-mass constant; for many-electron atoms the equation does not apply.
- The levels are whole numbers, chosen from the lists; n2 must be greater than n1, otherwise the calculator says so instead of giving a result.
- Fine structure and other small corrections are ignored; for Balmer-alpha they amount to about 0.01-0.02 nm.
How to read the result
The result is a vacuum wavelength. Tables of visible lines often list air wavelengths, which are slightly shorter: Balmer-alpha is about 656.47 nm in vacuum and 656.28 nm in air. Larger jumps give shorter wavelengths; all lines ending on n1 = 1 are ultraviolet.
Limits and common mistakes
- Using R∞ instead of RH shifts the wavelength by about 0.05% (0.36 nm for Balmer-alpha).
- Putting the larger level first gives a negative value; the lower level is n1.
Frequently Asked Questions
What does the Rydberg equation calculate?
The wavelength (or wavenumber) of light emitted or absorbed by a hydrogen atom when its electron moves between two energy levels.
What is the wavelength of the n = 3 to n = 2 transition?
About 656.47 nm in vacuum, the red Balmer-alpha line, with a photon energy of about 1.889 eV.
What is the Rydberg constant for hydrogen?
About 1.09678 × 10^7 m^−1, slightly smaller than R∞ because the proton is not infinitely heavy.
Formula used
sel n1 | Lower level n1 | 2 (Balmer series)=2, 1 (Lyman series)=1, 3 (Paschen series)=3, 4 (Brackett series)=4, 5 (Pfund series)=5, 6=6 sel n2 | Upper level n2 | 3=3, 4=4, 5=5, 6=6, 7=7, 8=8, 9=9, 10=10, 2=2 in r | Rydberg constant for hydrogen | m^-1 | 10967758.3 | 0 out lam | Wavelength (vacuum) | nm | 1e9 / (r * (1 / n1^2 - 1 / n2^2)) | 2 out wn | Wavenumber | cm^-1 | 10000000 / lam | 1 out ev | Photon energy | eV | 6.62607015e-34 * 299792458 * wn * 100 / 1.602176634e-19 | 4
Each line is one input (in, sel, list) or one result (out: label, unit, formula, decimals). How the calculators work
Method: the standard formula for this calculation with the constants and conversion factors written on the page, rounded as each result states. See method and constants, the disclaimer or report an error.
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