Bohr's Model of an Atom (original) (raw)

Last Updated : 8 May, 2026

Bohr's model is an atomic model proposed by Danish physicist Niels Bohr in 1913. In an atom, the electrons revolve around the nucleus in definite energy levels called orbits/shells. This model provides a basic understanding of the concept of the atom and its constituents. According to this model, the electron revolving near the nucleus has less energy, whereas the electron revolving away from the nucleus has higher energy.

bohr_model

**Postulates of Bohr's Model

To describe how electrons move in fixed paths around the nucleus, Bohr suggested certain important statements known as postulates of the Bohr model, which explain the arrangement and energy of electrons in an atom.

atoms

Therefore the angular momentum "L" of the revolving electron is,

L = \frac{nh}{2\pi}

where,
n is integer 1,2,3..... known as a principal quantum number
h is Planck's constant

hv = Ei- Ef

Limitations of Bohr's Model of Atom

The Bohr model successfully explained the structure and spectrum of the hydrogen atom. However, it could not explain many observations related to more complex atoms, such as the spectra of multi-electron atoms and the fine structure of spectral lines.

**1. Does Not Follow Heisenberg’s Uncertainty Principle
Bohr's model states that electrons revolve in fixed circular orbits with definite radius and velocity. However, according to Werner Heisenberg’s Uncertainty Principle, it is impossible to determine both the exact position and exact momentum of an electron at the same time. Thus, the idea of fixed electron orbits is inconsistent with the Heisenberg Uncertainty Principle.

**2. Cannot Explain the Zeeman Effect
Bohr's model fails to explain the splitting of spectral lines when an atom is placed in a magnetic field. This phenomenon is known as the Zeeman effect.

**3. Cannot Explain the Stark Effect
It also cannot explain the splitting of spectral lines in the presence of an electric field. This phenomenon is called the Stark effect.

**4. Not Applicable to Multi-Electron Atoms
Bohr's model works well only for hydrogen or hydrogen-like atoms (single-electron systems). It does not explain the electronic spectra of larger atoms having more than one electron.

**5. Cannot Explain Intensity of Spectral Lines
The model explains the position of spectral lines but does not explain why some spectral lines are brighter (more intense) than others.

**6. Ignores Wave Nature of Electrons
Later, Louis de Broglie showed that electrons have a wave nature. Bohr's model treats electrons only as particles and does not consider their wave behavior.

Applications of Bohr's Model of an Atom

Its applications are important in understanding atomic structure, spectral lines, and the behavior of electrons in atoms, especially in simple systems like hydrogen.

Distribution of Electrons in Orbits or Shells

In an atom, electrons are arranged around the nucleus in different energy levels called orbits or shells. According to the Bohr model, the distribution of electrons in these shells helps us understand the structure of atoms and the chemical properties of elements.

**K Shell (1st Orbit)

**L Shell (2nd Orbit)

**M Shell (3rd Orbit)

**N Shell (4th Orbit)

Solved Examples

**Example 1: If the velocity of an electron's first orbit in Bohr's atomic model of a hydrogen atom is 2.19 × 10 6 m/s. Find the velocity of electrons in the second orbit.

**Solution:

Velocity of an electron in orbit n is given by vn = v1/n

Given,
v1 = 2.19 × 106 m/s
n = 2

So, v2 = 2.19 × 106 /2

= 1.095 × 106 m/s.

**Example 2: Find the distance between the 2 nd **and 3 rd orbits of Bohr's Hydrogen atom.

**Solution:

Radius of 3rd orbit r3 = 0.529 × n2 × 10-10 / z

= 0.529 × 9 × 10-10

Radius of 2nd orbit r2 = 0.529 × 4 × 10-10

r3 - r2 = 0.529 × (5 × 10 -10)m

= 2.645 Å

**Example 3: Find the distance between the 2 nd **and 1 st orbits of Bohr's atom.

**Solution:

Radius of 2nd orbit r2 = 0.529 × n2 × 10-10 / z

= 0.529 × 4 × 10-10

Radius of 1st orbit r1 = 0.529 × 1 × 10-10

r2 - r1 = 0.529 × ( 3 × 10-10) m

= 1.587 Å