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  3. /Physical Chemistry Calculators - Quantum Chemistry
  4. /Bohr Model Calculator

Bohr Model Calculator

Last updated: April 5, 2026

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.

Calculator

Results

Orbital Radius

5.2918e-11

m

Orbital Radius

0.5292

Å

Energy Level

-13.6

eV

Orbital Speed

2.1877e+6

m/s

Speed Fraction

0.007297

c

Orbital Period

1.5198e-16

s

Binding Energy Magnitude

2.1790e-18

J

Orbital Frequency

6.5797e+15

Hz

Results

Orbital Radius

5.2918e-11

m

Orbital Radius

0.5292

Å

Energy Level

-13.6

eV

Orbital Speed

2.1877e+6

m/s

Speed Fraction

0.007297

c

Orbital Period

1.5198e-16

s

Binding Energy Magnitude

2.1790e-18

J

Orbital Frequency

6.5797e+15

Hz

In This Guide

  1. 01Bohr Model Energy Level Formula
  2. 02The Hydrogen Spectral Series
  3. 03Bohr Radius: The Scale of Electron Orbits
  4. 04Limitations of the Bohr Model

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.

Bohr Model Energy Level Formula

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.

The Hydrogen Spectral Series

Named groups of hydrogen emission lines by the final quantum number (n₁):

  • Lyman series (n₁ = 1): transitions to ground state; UV light (91–122 nm)
  • Balmer series (n₁ = 2): transitions to n = 2; visible light (365–656 nm); the red Hα line (656 nm, n=3→2) is the most prominent hydrogen emission line in the universe
  • Paschen series (n₁ = 3): near-infrared (820 nm – 1875 nm)
  • Brackett series (n₁ = 4): mid-infrared (1460 nm – 4050 nm)
  • Pfund series (n₁ = 5): far-infrared

The Bohr radius calculator and atomic physics calculators provide complementary quantum chemistry tools.

Bohr Radius: The Scale of Electron Orbits

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.

Limitations of the Bohr Model

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.

Visual Analysis

How It Works

Enter initial quantum number n₂ (higher energy level) and final quantum number n₁ (lower level), and atomic number Z (1 for hydrogen). Energy levels: Eₙ = −13.6 × Z²/n² eV. Transition energy: ΔE = 13.6 × Z² × (1/n₁² − 1/n₂²) eV. Photon wavelength: λ = 1240/ΔE nm. Orbital radius: rₙ = 0.529 × n²/Z Å. Identifies the spectral series (Lyman, Balmer, Paschen, etc.).

Understanding Your Results

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.

Worked Examples

Hydrogen Ground State (n=1, Z=1)

Inputs

n1
Z1

Results

radius5.292e-11
radiusA0.5292
energy-13.6
velocity2188000
velocityC0.007297
period1.521e-16

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.

He⁺ Ion Second Orbit (n=2, Z=2)

Inputs

n2
Z2

Results

radius1.058e-10
radiusA1.0584
energy-13.6
velocity2188000
velocityC0.007297
period3.042e-16

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.

Frequently Asked Questions

The Bohr model (1913) describes the atom as a small positively charged nucleus surrounded by electrons that orbit at specific, fixed distances — like planets orbiting the sun. The key postulates: electrons occupy only certain allowed orbits (quantized energy states); electrons do not radiate energy while in these orbits; electrons emit or absorb light only when jumping between orbits, with the photon energy exactly equal to the energy difference between levels. The model successfully predicted hydrogen's emission spectrum to high precision and introduced the concept of quantized energy levels, a foundation of quantum mechanics. While superseded by quantum mechanical models for complex atoms, it remains exactly accurate for hydrogen and pedagogically essential for understanding atomic spectra.
Use the Rydberg formula: 1/λ = R_H × (1/n₁² − 1/n₂²), where R_H = 1.097 × 10⁷ m⁻¹ (Rydberg constant for hydrogen), n₁ is the lower energy level, and n₂ is the higher energy level. Or equivalently, using the Bohr energy formula: ΔE = 13.6 × (1/n₁² − 1/n₂²) eV; λ = 1240/ΔE nm. Example for the Balmer Hα line (n=3 to n=2): ΔE = 13.6 × (1/4 − 1/9) = 13.6 × 0.1389 = 1.89 eV; λ = 1240/1.89 = 656 nm (red light — the characteristic red color of hydrogen discharge tubes and nebulae).
The Balmer series consists of all hydrogen emission lines where electrons transition to the n = 2 energy level from higher levels. These transitions produce visible light, making them the most directly observable hydrogen emission lines: Hα (n=3→2): 656 nm — red; Hβ (n=4→2): 486 nm — blue-green; Hγ (n=5→2): 434 nm — violet; Hδ (n=6→2): 410 nm — violet; Balmer limit (n=∞→2): 365 nm — UV edge of the series. The Balmer series is visible in hydrogen discharge tubes, the spectra of stars (hydrogen absorption lines in stellar spectra are Balmer lines), and emission nebulae (the red glow of the Orion Nebula is Hα emission at 656 nm from ionized hydrogen).
The Bohr model is exact for hydrogen and hydrogen-like single-electron ions but fails in several important ways: it cannot handle multi-electron atoms (the electron-electron repulsion interactions cannot be incorporated); it cannot explain spectral line splitting in magnetic fields (Zeeman effect) or electric fields (Stark effect); it does not predict the relative intensities of emission lines; it cannot explain molecular bonding or chemistry. Most fundamentally, the model treats electrons as classical particles following defined orbits, contradicting the wave-particle duality established by quantum mechanics. The Schrödinger equation model (1926), which describes electrons as probability clouds (orbitals rather than orbits), corrects all these deficiencies but reduces to the Bohr result for hydrogen energy levels.
In the Bohr model, the principal quantum number n (n = 1, 2, 3, ...) specifies: the energy level of the electron (Eₙ = −13.6 eV/n²); the orbital radius (rₙ = 0.529 × n² Å for hydrogen); and the 'shell' of the electron (n=1 is the K shell, n=2 the L shell, etc.). Larger n means higher energy (less negative) and larger orbital. n = 1 is the ground state — the lowest energy, most stable configuration. Excited states (n > 1) are unstable; electrons in them spontaneously fall to lower levels, emitting photons. In full quantum mechanics, n remains the principal quantum number but is accompanied by l (angular momentum), mₗ (magnetic), and mₛ (spin) quantum numbers that together fully specify an electron's state.
When an atom absorbs energy (from heat, electrical discharge, or light), electrons jump to higher quantum states. These excited states are unstable — electrons spontaneously fall back toward the ground state, and when they do, the energy difference is released as a photon of light. Since electron energy levels are quantized (only specific energies are allowed), only specific photon energies — and therefore specific wavelengths — are emitted. Each element has a unique set of energy levels, producing a unique 'fingerprint' emission spectrum. This explains why hydrogen discharge tubes glow red (dominated by the Hα line at 656 nm), helium tubes glow yellow-white, neon tubes glow orange-red, and sodium street lights produce characteristic yellow (sodium D lines at 589 nm). Spectroscopy uses these atomic fingerprints to identify elements in stars, nebulae, and laboratory samples.

Sources & Methodology

Bohr, N. (1913). On the Constitution of Atoms and Molecules. Philosophical Magazine, 26, 1–25. Griffiths, D.J. (2018). Introduction to Quantum Mechanics, 3rd ed. Cambridge University Press. NIST (2023). Atomic Spectra Database. https://www.nist.gov/pml/atomic-spectra-database.

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