Courses
Courses for Kids
Free study material
Offline Centres
More
Store Icon
Store

Emission Spectrum and Atomic Spectra in Chemistry

Reviewed by:
ffImage
hightlight icon
highlight icon
highlight icon
share icon
copy icon

What Is Emission Spectrum and Types of Atomic Spectra

The measurement of atoms (and ions) by their interaction with electromagnetic radiation in atomic spectra is an important topic. The coloured lines of light emitted by the excited atoms form the atomic spectra. We all know about light refraction. Light either bends toward the normal or away from the normal as it passes from one medium to another. The refraction effect is primarily due to the difference in the speed of light in different mediums. The speed of light depends upon the density of the medium it travels through.


Let us understand the phenomenon of white light dispersion through a prism, and about the continuum of emissions and the spectrum of absorption.


Emission Spectrum

Electrons shift from lower energy levels to higher energy levels as energy is consumed by an atom's electrons. To return to ground states from the excited state, which is unstable, these excited electrons have to radiate energy. The spectrum of pollution is formed by the frequency of the light emitted.

  • The electrons in these atoms will absorb energy as electromagnetic radiation interacts with atoms and molecules of matter, and leap to a higher energy state, losing their stability.

  • They need to switch from the higher energy state to the preceding lower energy state in order to recover their equilibrium.

  • These atoms and molecules emit radiation in different regions of the electromagnetic spectrum to accomplish this task.

  • This radiation spectrum emitted by electrons in the excited atoms or molecules is known as the spectrum of emissions.

Absorption Spectrum

On the other hand, as energy is absorbed by electrons in the ground state to enter higher energy states, the absorption range is constituted by the frequencies of light emitted by dark bands.

  • We observe that it experiences refraction twice when a beam of white light falls on a prism.

  • Once from a rare medium (air) to a denser medium (glass) and again from a denser medium (glass) to a rare medium (glass) (air).

  • Finally, we see a band of colors, called the continuum, which is built out of a white light beam. The color with a smaller wavelength deviates the most as we study this spectrum more closely and vice versa.

  • Thus red with the longest wavelength suffers the least variance, a continuum of colors ranging from red to violet is observed.

  • As violet merges into blue, blue into green and so on, this sort of spectrum is called a continuous spectrum.

However, in the gas phase, the emission spectrum of atoms does not display a constant spread of wavelengths from one color to another. Instead, the light emitted consists of a single wavelength with dark spaces occurring between them. These kinds of spectra are referred to as spectra of atoms or line spectra.


Emission Spectrum & Absorption Spectrum

In an atom, the electrons appear to be arranged in such a way that the atom's energy is as minimal as possible. The lowest energy state of the atom is the ground state of an atom. The electrons consume the energy and transfer to a higher energy level when those atoms are given energy. These electron energy levels in atoms are quantified, meaning again that the electron must travel in discrete steps rather than constantly from one energy level to another.


An atom's excited state is a state where its potential energy is greater than the state of the earth. An atom is not stable in a state of excitation. As it goes back to the ground state, in the form of electromagnetic radiation, it releases the energy it had previously accumulated.

  • An absorption spectrum is like a negative photograph of a spectrum of pollution.

  • Electromagnetic radiation is bombarded with a sample that absorbs radiation from certain wavelengths to observe the absorption spectrum.

Hydrogen Emission and Absorption Series

In astronomy, the spectrum of hydrogen is especially significant since much of the Universe is made of hydrogen. The processes of hydrogen emission or absorption give rise to series, which are sequences of lines corresponding to atomic transitions, each ending or starting with the same hydrogen atomic state. The Balmer Series, for example, includes transitions beginning (for absorption) or ending (for emission) with the first excited state of hydrogen, while the Lyman Series involves transitions beginning or ending with hydrogen's ground state; the adjacent picture shows the atomic transitions that create emissions from these two series.


The Balmer Series is in the visible spectrum and the Lyman Series is in the UV, owing to the specifics of hydrogen's atomic structure. Some of the transitions in the Balmer series are illustrated in the following illustration.


Molecular Spectra

Molecules can interact with electromagnetic radiation and give rise to characteristic spectra, in addition to spectra associated with atoms and ions. Because of the fundamental atomic and molecular structure, infrared wavelengths usually provide the spectra associated with molecules. Moreover, since molecules are typically fragile, molecular spectra are mainly essential in relatively cold objects, such as planetary atmospheres, very cool star surfaces, and different interstellar regions.

FAQs on Emission Spectrum and Atomic Spectra in Chemistry

1. What is an emission spectrum in chemistry?

An emission spectrum is the pattern of wavelengths of light emitted by an excited atom when its electrons return to lower energy levels. It appears as bright colored lines on a dark background and is unique for each element.

  • Electrons absorb energy and jump to higher energy levels.
  • When they fall back to lower levels, they release energy as light.
  • The emitted light has specific wavelengths, forming a line emission spectrum.
This unique pattern acts as a fingerprint for identifying elements in atomic spectroscopy.

2. What causes the emission spectrum of an atom?

An emission spectrum is caused by electronic transitions from higher to lower energy levels within an atom. When energy is supplied (heat, electricity, or radiation), electrons become excited.

  • Excited electrons move to higher energy states.
  • They are unstable in excited states.
  • They return to lower levels, emitting photons of specific energy.
The energy of the emitted light is given by E = hν, where h is Planck’s constant and ν is frequency.

3. Why is the emission spectrum of each element unique?

The emission spectrum of each element is unique because every element has a distinct set of quantized energy levels. The arrangement of electrons differs for each atom.

  • Energy gaps between levels vary from element to element.
  • Therefore, emitted photon energies are different.
  • This produces a unique set of spectral lines.
For example, hydrogen shows specific lines known as the Balmer series in the visible region.

4. What is the difference between emission spectrum and absorption spectrum?

An emission spectrum shows bright lines produced by emitted light, whereas an absorption spectrum shows dark lines where light has been absorbed.

  • Emission spectrum: Bright lines on a dark background.
  • Absorption spectrum: Dark lines on a continuous spectrum.
  • Emission occurs when electrons fall to lower levels.
  • Absorption occurs when electrons absorb energy and move to higher levels.
Both spectra correspond to the same energy differences in atomic spectra.

5. What is the atomic emission spectrum of hydrogen?

The atomic emission spectrum of hydrogen consists of discrete lines grouped into spectral series such as Lyman, Balmer, and Paschen.

  • Lyman series: Transitions to n = 1 (ultraviolet region).
  • Balmer series: Transitions to n = 2 (visible region).
  • Paschen series: Transitions to n = 3 (infrared region).
The wavelength of hydrogen spectral lines is calculated using the Rydberg equation:
1/λ = RH(1/n12 − 1/n22), where RH = 1.097 × 107 m-1.

6. How do you calculate the wavelength of a spectral line?

The wavelength of a spectral line is calculated using the Rydberg formula for hydrogen or E = hc/λ for general cases.

  • For hydrogen: 1/λ = RH(1/n12 − 1/n22).
  • For energy transitions: E = hν and ν = c/λ.
  • Combine to get λ = hc/E.
Here, h = 6.626 × 10-34 J·s and c = 3.00 × 108 m/s.

7. What are the types of atomic spectra?

The three main types of atomic spectra are emission spectra, absorption spectra, and continuous spectra.

  • Emission spectrum: Bright lines from excited atoms.
  • Absorption spectrum: Dark lines due to absorbed wavelengths.
  • Continuous spectrum: Unbroken range of wavelengths (e.g., hot solids).
Atomic spectra are mainly line spectra because atomic energy levels are quantized.

8. Why do emission spectra consist of lines instead of a continuous spectrum?

Emission spectra consist of lines because electrons can only occupy specific quantized energy levels in atoms.

  • Energy levels are discrete, not continuous.
  • Only specific energy differences are allowed.
  • Each transition emits light of a fixed wavelength.
This quantum behavior explains the line spectrum observed in atomic emission spectroscopy.

9. How is emission spectroscopy used to identify elements?

Emission spectroscopy identifies elements by matching their unique spectral lines to known reference spectra.

  • A sample is heated or electrically excited.
  • It emits characteristic wavelengths of light.
  • The observed lines are compared with standard atomic spectra.
This technique is widely used in chemical analysis, flame tests, and astronomical studies.

10. What is the relationship between energy levels and spectral lines?

Spectral lines correspond to the energy difference between two quantized energy levels in an atom.

  • When an electron moves from E2 to E1, energy is emitted.
  • The photon energy equals ΔE = E2 − E1.
  • This energy determines the wavelength using E = hν.
Thus, each spectral line directly reflects a specific electronic transition in the atomic structure.