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Hydrogen spectrum

Intermediate

Lyman, Balmer and Paschen series.

Key relation1/λ = R(1/n₁²−1/n₂²)

Photons emitted when electrons fall: 1/λ = R(1/n_f² − 1/n_i²). Series: Lyman (to n = 1, UV), Balmer (n = 2, visible), Paschen (n = 3, IR).

Worked example

Balmer Hα (3→2): 656 nm red.

Common mistake

Each series ends at a series limit.

In more detail

The hydrogen spectrum consists of discrete lines grouped into series, such as the Lyman, Balmer and Paschen series. Each line corresponds to a transition between two energy levels.

Real-world uses

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Frequently asked questions

What is the Balmer series?

Transitions that end at n equal to two, producing visible lines.

Why are the lines discrete?

Because electrons can only occupy specific energy levels.

What is the difference between the Lyman and Balmer series?

Lyman lines end in the ground state and are ultraviolet, while Balmer lines end in the second level and include visible red light.

Related topics in Atomic & Nuclear Physics

Bohr's postulates · Radius of Bohr orbit · Energy of hydrogen levels · Rydberg constant · Absorption and emission spectra · Ionisation energy

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