Ch. 2 | Structure of Atom0/15

Atomic Spectra and the Hydrogen Spectrum

Why atoms emit only specific colours — the fingerprint that revealed quantised energy levels

Helium was discovered in the Sun — 27 years before it was found on Earth

During a solar eclipse in 1868, a French astronomer noticed a strange yellow line in the Sun's spectrum that matched no known element on Earth. Scientists named the mystery element helium after Helios, the Greek god of the Sun. It wasn't until 1895 that William Ramsay finally isolated helium from a uranium mineral in his London lab. A whole element, identified from 150 million kilometres away — purely by reading the light it emitted. That is the power of atomic spectra.

Introduction to Atomic Spectra
prism
Refraction of light through a prism

The speed of light depends upon the nature of the medium through which it passes. As a result, the beam of light is deviated or refracted from its original path as it passes from one medium to another.

It is observed that when a ray of white light is passed through a prism, the wave with shorter wavelength bends more than the one with a longer wavelength. Since ordinary white light consists of waves with all the wavelengths in the visible range, a ray of white light is spread out into a series of coloured bands called spectrum. The light of red colour which has longest wavelength is deviated the least while the violet light, which has shortest wavelength is deviated the most.

Line spectra of sodium_1
Line spectra of sodium.

Now heat sodium vapour until it glows. Instead of a rainbow, you see just two sharp yellow lines sitting in complete darkness. That is a line spectrum — and those two lines are sodium's identity card. Every element has its own unique set of lines, and no two elements share the same pattern.

Continuous spectra and line spectra

Listen to the audio explanation

0:002:32

Understanding why atoms produce line spectra — and not continuous rainbows — turned out to be one of the most important clues that led scientists to quantum mechanics.

Two Types of Spectra: Continuous and Line

When light from electrically excited gaseous atoms passes through a slit and is refracted by a prism, it does not create a continuous spectrum, or rainbow, as sunlight does. Instead, it creates a line spectrum, a series of fine lines at specific frequencies separated by black spaces. Figure below shows the apparatus and the line spectrum of atomic hydrogen and line spectrum of mercury and strontium.

The emission spectrum shows only a handful of sharp bright lines at specific wavelengths. The rest is dark. These are called line spectra or atomic spectra, because the emitted radiation appears as discrete bright lines — not a rainbow.

Absorption spectra work the opposite way: pass a beam of white light through a cool gas, and that gas absorbs exactly the same specific wavelengths it would otherwise emit. You see a rainbow with dark gaps — a photographic negative of the emission spectrum. The study of both kinds is called spectroscopy.

Diagram comparing emission and absorption spectra through a prism
📸 Fig (A) The line spectrum of atomic hydrogen (B) Unlike the continuous spectrum of white light, emission spectra of elements, such as mercury and strontium, appear as characteristic series of colored lines.

Emission Spectrum vs Absorption Spectrum

Emission Spectrum

  • Produced when excited atoms *release* energy as light
  • Appears as bright coloured lines on a dark background
  • Each line corresponds to a specific wavelength emitted
  • Atoms must be energised first (heat, electric discharge, UV)
  • Used to identify elements present in a glowing/hot sample
VS

Absorption Spectrum

  • Produced when atoms *absorb* specific wavelengths from white light
  • Appears as dark lines (gaps) on a continuous rainbow background
  • Dark lines occur at exactly the same wavelengths as emission lines
  • The cool gas sample absorbs what it would otherwise emit
  • Used to identify elements in cool interstellar clouds and stellar atmospheres

Line Spectra: Every Element's Unique Fingerprint

The key insight that made spectroscopy revolutionary: each element has a unique set of spectral lines — no two elements share the same pattern. Just as no two people share the same fingerprint, no two elements share the same spectrum.

This means you can identify an unknown element by matching its spectral lines against a reference table — even from across the galaxy. The German chemist Robert Bunsen (1811–1899) — famous for the burner he co-developed — was among the first to use this systematically for chemical analysis.

Elements discovered entirely through spectroscopy:

  • Rubidium (Rb) and Caesium (Cs) — Bunsen & Kirchhoff, 1860–61, from mineral spring residues
  • Thallium (Tl), Indium (In), Gallium (Ga), Scandium (Sc) — all found by spotting previously unknown lines in mineral spectra
  • Helium (He) — found in the Sun's spectrum in 1868, isolated on Earth in 1895

Spectroscopy remains one of the most powerful analytical tools in chemistry, astronomy, and forensic science today.

The Hydrogen Spectrum — Simplest, Yet Most Revealing

Hydrogen has only one electron, making its spectrum the simplest of all elements — and the easiest to analyse mathematically. When you pass an electric discharge through gaseous hydrogen, the HX2\ce{H2} molecules dissociate into individual atoms. The energetically excited hydrogen atoms then emit electromagnetic radiation, but only at discrete (specific) frequencies — not a continuous spread.

The hydrogen spectrum is organised into several distinct series of lines, each appearing in a different region of the electromagnetic spectrum, and each named after the scientist who first studied it:

  • Lyman series — ultraviolet region
  • Balmer series — visible region (the only one you can see with your eyes)
  • Paschen series — infrared region
  • Brackett series — infrared region
  • Pfund series — infrared region
🖼 Image PendingEnergy level diagram showing electron transitions in hydrogen atom for Lyman, Balmer and Paschen series

AI Generation Prompt

Hydrogen atom energy level diagram showing electron transitions for spectral series. Vertical layout with energy increasing upward. Horizontal lines represent energy levels from n=1 (bottom, ground state, labelled n=1) up through n=2, n=3, n=4, n=5, n=6 and n=infinity (top, ionisation limit, dashed line at 0 eV). Draw downward-pointing arrows for electronic transitions grouped by series: Lyman series — many blue/indigo arrows terminating at n=1 (labelled 'Lyman series (ultraviolet)'); Balmer series — four arrows terminating at n=2, coloured Red, Green, Blue, Violet from longest to shortest wavelength (labelled 'Balmer series (visible)', with colour labels on each arrow); Paschen series — arrows terminating at n=3 (labelled 'Paschen series (infrared)'). Energy axis on the left with an upward arrow and label 'Energy'. Show n=infinity dashed line at top with label 'n = infinity'. Label all quantum number levels: n=1 through n=6. Dark background, orange accent labels, clean technical illustration style.

📸 Fig 2.11 — Electron transitions in the hydrogen atom. Arrows pointing downward represent photon emission. The Lyman series (UV) terminates at n=1, Balmer (visible) at n=2, Paschen (IR) at n=3.

Balmer's Formula — Finding the Pattern (1885)

In 1885, the Swiss mathematician Johann Balmer discovered that the four visible lines of the hydrogen spectrum obeyed a beautifully simple formula. He expressed the lines in terms of wavenumber νˉ\bar{\nu} — the number of waves per centimetre (unit: cm1\text{cm}^{-1}) — which is the reciprocal of wavelength:

νˉ=1λ\bar{\nu} = \frac{1}{\lambda}

The Balmer formula for the visible lines:

νˉ=109,677(1221n2) cm1\bar{\nu} = 109{,}677 \left(\frac{1}{2^2} - \frac{1}{n^2}\right) \text{ cm}^{-1}

Equation 2.8 — Balmer Series

where n is an integer ≥ 3 (i.e., n = 3, 4, 5, …). These lines lie in the visible region of the spectrum.

The Swedish spectroscopist Johannes Rydberg then showed that all the series of lines in the hydrogen spectrum — not just the visible Balmer series — could be described by a single generalised formula:

νˉ=109,677(1n121n22) cm1\bar{\nu} = 109{,}677 \left(\frac{1}{n_1^2} - \frac{1}{n_2^2}\right) \text{ cm}^{-1}

Equation 2.9 — Rydberg Formula

where n₁ = 1, 2, 3, … and n₂ = n₁ + 1, n₁ + 2, … The constant 109,677 cm⁻¹ is called the Rydberg constant (R∞). Each series corresponds to a fixed value of n₁ with n₂ taking successive higher integer values.

Table 2.3 — Spectral Line Series for Atomic Hydrogen

Seriesn₁ (lower level)n₂ (upper levels)Spectral Region
Lyman12, 3, 4, …Ultraviolet
Balmer23, 4, 5, …Visible
Paschen34, 5, 6, …Infrared
Brackett45, 6, 7, …Infrared
Pfund56, 7, 8, …Infrared

The Physical Meaning of n₁ and n₂

In the Rydberg formula, n1n_1 is the lower energy level (the shell the electron falls into) and n2n_2 is the higher energy level (where it starts). The photon is emitted because the electron loses energy dropping from n2n_2 down to n1n_1.

The series name tells you n1n_1:

  • Lyman: n1=1n_1 = 1 (electron lands in ground state)
  • Balmer: n1=2n_1 = 2 (visible — why we can see these)
  • Paschen: n1=3n_1 = 3, Brackett: n1=4n_1 = 4, Pfund: n1=5n_1 = 5

Why Does Hydrogen Emit Only Specific Lines?

NCERT poses this question directly at the end of the section: line spectra are unique to each element, and there is regularity in the pattern. Why? What does this tell us about electronic structure?

JEE / NEET Exam Insights — Atomic SpectraJEE / NEET
Rydberg constant value: R=109,677 cm1R_\infty = 109{,}677 \text{ cm}^{-1} — memorise this. JEE Mains often asks for the wavenumber of a specific line in a given series.
Which series is visible? Only the Balmer series lies in the visible region. All others (Lyman, Paschen, Brackett, Pfund) are UV or IR.
Lyman series: n1=1n_1 = 1, n22n_2 \geq 2, ultraviolet — the highest energy series.
Classic exam trap: 'The first line of the Balmer series' means n2=3n_2 = 3, n1=2n_1 = 2 (smallest possible transition into n=2n=2). The 'series limit' (convergence limit) is n2n_2 \to \infty, giving νˉ=109,677×1n12\bar{\nu} = 109{,}677 \times \frac{1}{n_1^2}.
Absorption spectra in stars: Fraunhofer lines in the solar spectrum are absorption lines — cool gases in the Sun's atmosphere absorb specific wavelengths. NEET sometimes asks whether solar spectra are emission or absorption.
Emission vs absorption spectra: Both show lines at identical wavelengths — one has bright lines on dark background (emission), the other has dark gaps on a rainbow (absorption). They are complementary.
Quick Check

Q1.Which series of the hydrogen spectrum falls in the visible region?