The Bohr Model Calculator computes electron energy levels, orbital radii, and photon emission and absorption wavelengths for hydrogen and hydrogen-like atoms. Enter the principal quantum numbers of two energy levels to calculate the transition energy and the wavelength of light emitted or absorbed.
5.2918e-11
m
0.5292
Å
-13.6
eV
2.1877e+6
m/s
0.007297
c
1.5198e-16
s
2.1790e-18
J
6.5797e+15
Hz
5.2918e-11
m
0.5292
Å
-13.6
eV
2.1877e+6
m/s
0.007297
c
1.5198e-16
s
2.1790e-18
J
6.5797e+15
Hz
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.
The orbital radius increases as n² and decreases with Z, meaning highly charged ions are much more compact. For hydrogen ground state, r₁ = 0.529 Å. For He⁺ (Z=2), r₁ = 0.265 Å—half the hydrogen value. The energy becomes more negative (more tightly bound) with increasing Z² and decreasing n². The ground state of He⁺ is −54.4 eV—four times deeper than hydrogen. The velocity at the ground state of hydrogen is about 2.19 × 10⁶ m/s (0.73% of c). For heavy hydrogen-like ions, v can approach c, making the Bohr model inaccurate and requiring relativistic quantum mechanics (Dirac equation). The orbital period for hydrogen ground state is ~1.5 × 10⁻¹⁶ s, corresponding to a frequency of ~6.6 × 10¹⁵ Hz.
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Results
The hydrogen ground state has the Bohr radius a₀ = 0.529 Å, energy −13.6 eV, and orbital velocity about 0.73% of the speed of light.
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Results
The n=2 orbit of He⁺ has the same radius and energy as the hydrogen ground state (coincidence of n²/Z scaling), with velocity αcZ/n = αc.
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