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  4. /Bohr Model Calculator

Bohr Model Calculator

Last updated: April 5, 2026

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.

Calculator

Results

Initial Level Energy

-3.4

eV

Final Level Energy

-13.6

eV

Photon Energy

10.2

eV

Photon Wavelength

121.553136

nm

Initial Orbit Radius

2.116708

angstrom

Final Orbit Radius

0.529177

angstrom

Electron Speed at Initial Level

1,093,845.65

m/s

Electron Speed at Final Level

2,187,691.3

m/s

Spectral Wavenumber

82,302.986775

cm^-1

Results

Initial Level Energy

-3.4

eV

Final Level Energy

-13.6

eV

Photon Energy

10.2

eV

Photon Wavelength

121.553136

nm

Initial Orbit Radius

2.116708

angstrom

Final Orbit Radius

0.529177

angstrom

Electron Speed at Initial Level

1,093,845.65

m/s

Electron Speed at Final Level

2,187,691.3

m/s

Spectral Wavenumber

82,302.986775

cm^-1

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

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).

Worked Examples

Hydrogen Balmer-Alpha (n=3 to n=2)

Inputs

Z1
n3
n final2

Results

energy eV-1.51111
radius angstrom4.761
velocity ms729230
transition energy eV1.88889
wavelength nm656.47

The H-alpha line at 656 nm (red) is the most prominent hydrogen emission line and the dominant feature in emission nebulae.

Helium-Like Ion He+ Ground State

Inputs

Z2
n1
n final2

Results

energy eV-54.4
radius angstrom0.2645
velocity ms4375382
transition energy eV40.8
wavelength nm30.38

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.

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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