The Bohr Model Calculator computes energy levels, orbital radii, and photon wavelengths for hydrogen using Bohr's 1913 equations. Enter two principal quantum numbers to get the transition energy and the exact wavelength of light emitted or absorbed — Lyman, Balmer, or Paschen series.
-3.4
eV
-13.6
eV
10.2
eV
121.553136
nm
2.116708
angstrom
0.529177
angstrom
1,093,845.65
m/s
2,187,691.3
m/s
82,302.986775
cm^-1
-3.4
eV
-13.6
eV
10.2
eV
121.553136
nm
2.116708
angstrom
0.529177
angstrom
1,093,845.65
m/s
2,187,691.3
m/s
82,302.986775
cm^-1
When Niels Bohr proposed his atomic model in 1913, he solved a problem that had stumped classical physics for decades: why do excited hydrogen atoms emit light at specific discrete wavelengths rather than a continuous spectrum? His answer — electrons orbit the nucleus only at specific allowed energy levels, and emit or absorb photons when jumping between them — was a revolutionary step toward quantum mechanics. The Bohr model calculator applies his equations to any hydrogen-like transition.
The energy of electron level n in a hydrogen-like atom:
Eₙ = −13.6 eV × Z² / n²
where Z = atomic number (Z = 1 for hydrogen), n = principal quantum number (1, 2, 3, ...). The energy is negative because electrons are bound — n = 1 (ground state) has the lowest (most negative) energy; higher n means higher (less negative) energy and larger orbital.
Transition energy: ΔE = 13.6 eV × Z² × (1/n₁² − 1/n₂²)
If ΔE > 0: photon is emitted (emission); if ΔE < 0: photon is absorbed. Photon wavelength: λ = hc/ΔE = 1240 eV·nm / ΔE. Use this online calculator to compute any hydrogen transition wavelength.
Named groups of hydrogen emission lines by the final quantum number (n₁):
The Bohr radius calculator and atomic physics calculators provide complementary quantum chemistry tools.
The Bohr radius (a₀ = 5.29 × 10⁻¹¹ m = 0.529 Å) is the most probable distance between the proton and electron in ground-state hydrogen. Orbital radius at level n: rₙ = a₀ × n² / Z. At n = 1: r₁ = 0.529 Å (for hydrogen). At n = 2: r₂ = 4 × 0.529 = 2.116 Å — four times larger. At n = 3: r₃ = 9 × 0.529 = 4.76 Å. The orbital radius scales as n² — electron orbits expand quadratically with quantum number.
The Bohr model works exactly for hydrogen and hydrogen-like ions (He⁺, Li²⁺) but fails for multi-electron atoms. It cannot explain: fine structure (spin-orbit coupling); the Zeeman effect (splitting in magnetic fields); the relative intensities of spectral lines; or molecular bonding. The quantum mechanical model (Schrödinger equation, electron probability clouds) supersedes Bohr for accuracy, but Bohr's energy level formula remains exact for hydrogen and is foundational for understanding spectroscopy, atomic structure, and quantum mechanics pedagogy.
Energy is always negative (bound state); more negative = more tightly bound. E_1 = -13.6 eV (ground state), E_2 = -3.4 eV, E_3 = -1.51 eV. Ionization energy = |E_1| = 13.6 eV. Lyman series (to n=1) lies in UV (91-122 nm). Balmer series (to n=2) lies in visible (365-656 nm). Paschen series (to n=3) lies in near-IR (820-1875 nm).
Inputs
Results
The H-alpha line at 656 nm (red) is the most prominent hydrogen emission line and the dominant feature in emission nebulae.
Inputs
Results
He+ (Z=2) has 4x more binding energy than hydrogen (54.4 eV). Its ionization energy matches observed helium spectrum. The transition photon is deep UV.
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