Hydrogen spectrum- Types of series, characterstics and it's application

 Hydrogen Spectrum: Details in simple explanation

Electrons of hydrogen atoms when absorb energy, get excited to the next higher shells. These excited electrons emit energy (in form of light), when they jump down to the lower energy levels. These energy (emitted light) are observed on a fluorescent screen which appear as group of lines. The number of lines observed on the screen indicates the number of possible transitions made by excited electrons.

By Rajettan - Own work, CC BY-SA 4.0, https://commons.wikimedia.org/w/index.php?curid=41466201
4. Actual obsevation of line spectrum

By OrangeDog, CC BY-SA 3.0, https://commons.wikimedia.org/w/index.php?curid=6278485

The hydrogen spectrum refers to the specific set of wavelengths of electromagnetic radiation emitted or absorbed by hydrogen atoms. When hydrogen atoms are excited, typically by heating or passing an electric current through a gas, they emit light of different wavelengths.

The hydrogen spectrum is well-known and has been extensively studied because hydrogen is the simplest and most abundant element in the universe. The spectrum consists of several series of spectral lines, which are grouped into different regions based on their wavelengths.

Types Of Series:There are mainly 5 types of Hydrogen spectrum series

  • Lyman series
  • Balmer series
  • Paschen series
  • Brackett series
  • Pfund series

Lyman series: 

  • This series lies in the ultraviolet (UV) region of the spectrum. It consists of lines resulting from transitions of electrons from higher energy levels to the n = 1 (ground) energy level.
  • The Lyman series of the hydrogen spectrum consists of spectral lines that are observed in the ultraviolet (UV) region of the electromagnetic spectrum. These lines are generated when electrons in excited states transition to the lowest energy level, which is the n = 1 or ground state.

The Ultraviolet Realm:

  • The Lyman series finds its home in the ultraviolet (UV) region of the electromagnetic spectrum. With wavelengths shorter than visible light, these lines are beyond the capability of human vision. Instead, specialized instruments and detectors are employed to study and analyze this intriguing UV spectrum emitted by excited hydrogen atoms.

Electron Transitions:

  • The Lyman series arises from transitions of electrons within hydrogen atoms. When an electron absorbs energy, either through heating or an electric current, it moves to a higher energy level, known as an excited state. Subsequently, as the electron returns to the n = 1 energy level, it emits electromagnetic radiation in the form of UV light. Each line in the Lyman series corresponds to a specific electron transition from a higher energy level (n > 1) to the ground state (n = 1).

The Lyman Formula:

  • The wavelengths of the Lyman series lines can be described by the Lyman formula, which captures the relationship between the wavelength (λ), the Rydberg constant (R_H), and the principal quantum number (n). The formula is given as:

        1/λ = R_H * (1 - 1/n^2)

  • This equation allows scientists to calculate the precise wavelengths associated with the Lyman series lines, aiding in the identification and characterization of these transitions.

Significance and Applications:

  • The Lyman series has immense scientific importance across various disciplines. Astrophysicists rely on the observation and analysis of Lyman series lines to study and understand celestial objects. By analyzing the absorption and emission spectra of hydrogen in stars, galaxies, and interstellar media, researchers gain insights into their composition, temperature, and density. The Lyman series also serves as a critical tool in the study of intergalactic hydrogen clouds and the early universe, shedding light on cosmic evolution.
  • Furthermore, the Lyman series played a pivotal role in the development of quantum mechanics. Its existence and the observed discrete energy levels provided evidence for the quantization of energy and the wave-particle duality of matter. The success in explaining the Lyman series with the Bohr model of the hydrogen atom eventually led to the formulation of more sophisticated quantum mechanical theories.

The Lyman series, residing in the ultraviolet portion of the electromagnetic spectrum, represents a crucial component of hydrogen's atomic spectrum. It showcases spectral lines resulting from electron transitions from higher energy levels to the ground state. Through its study, scientists have gained significant insights into the behavior and structure of hydrogen, making remarkable contributions to astrophysics and quantum mechanics. The Lyman series continues to inspire further exploration and understanding of the fundamental building blocks of the universe.

Balmer series: 

  • This series lies in the visible region of the spectrum and is the most well-known. It consists of lines resulting from transitions of electrons from higher energy levels to the n = 2 energy level. The Balmer series includes the famous four visible lines: H-alpha (656.3 nm, red), H-beta (486.1 nm, blue-green), H-gamma (434.0 nm, violet), and H-delta (410.2 nm, violet).
  • The Balmer series is indeed a set of spectral lines that are observed in the visible region of the electromagnetic spectrum. These lines are generated when electrons in excited states transition to the n = 2 energy level in hydrogen atoms.
  • The Balmer series is named after Johann Balmer, a Swiss mathematician who discovered an empirical formula to describe the wavelengths of these spectral lines in 1885. The formula, known as the Balmer formula, is given by:

         1/λ = R_H [(1/2²) - (1/n²)]

  • where λ is the wavelength of the emitted or absorbed light, R_H is the Rydberg constant for hydrogen (approximately 1.097 × 10^7 m¹), and n is the principal quantum number indicating the energy level of the electron (n = 3, 4, 5, and so on).

The Balmer series includes several spectral lines, but the most well-known and prominent lines are:

  • H-alpha (656.3 nm): This line appears in the red part of the spectrum. It corresponds to the transition from the n = 3 energy level to the n = 2 energy level.
  • H-beta (486.1 nm): This line appears in the blue-green part of the spectrum. It corresponds to the transition from the n = 4 energy level to the n = 2 energy level.
  • H-gamma (434.0 nm): This line appears in the violet part of the spectrum. It corresponds to the transition from the n = 5 energy level to the n = 2 energy level.
  • H-delta (410.2 nm): This line also appears in the violet part of the spectrum. It corresponds to the transition from the n = 6 energy level to the n = 2 energy level.

These four lines of the Balmer series are particularly famous and are often used in spectroscopy and astrophysics. They have been instrumental in studying and understanding the properties of hydrogen and are frequently observed in various astronomical objects, including stars and nebulae.

Paschen series: 

  • This series lies in the infrared (IR) region of the spectrum. It consists of lines resulting from transitions of electrons from higher energy levels to the n = 3 energy level.
  • The Paschen series is a set of spectral lines observed in the infrared (IR) region of the electromagnetic spectrum. The lines in this series are generated when electrons transition from higher energy levels to the n = 3 energy level in hydrogen atoms.
  • The Paschen series is named after Friedrich Paschen, a German physicist who studied atomic spectra in the late 19th and early 20th centuries. The wavelengths of the lines in the Paschen series can be described using the following formula, known as the Paschen formula:

         1/λ = R_H [(1/3²) - (1/n²)]

  • where λ is the wavelength of the emitted or absorbed light, R_H is the Rydberg constant for hydrogen (approximately 1.097 × 10^7 m¹), and n is the principal quantum number indicating the energy level of the electron (n = 4, 5, 6, and so on).
  • The Paschen series includes several spectral lines, but since they lie in the infrared region, they are not visible to the human eye. These lines are significant for studying hydrogen and its presence in various astronomical objects, especially in the field of astrophysics.

While the exact wavelengths of the lines vary, here are a few examples of the Paschen series lines and their approximate wavelengths:

  • Paschen-alpha (1875.1 nm): Transition from the n = 4 energy level to the n = 3 energy level.
  • Paschen-beta (1281.8 nm): Transition from the n = 5 energy level to the n = 3 energy level.
  • Paschen-gamma (1093.1 nm): Transition from the n = 6 energy level to the n = 3 energy level.

These lines are commonly observed and studied in infrared spectroscopy, as they provide valuable information about the energy levels and transitions in hydrogen atoms.

Brackett series:

  • This series also lies in the IR region of the spectrum. It consists of lines resulting from transitions of electrons from higher energy levels to the n = 4 energy level.
  • The Paschen series is a set of spectral lines observed in the infrared (IR) region of the electromagnetic spectrum. The lines in this series are generated when electrons transition from higher energy levels to the n = 3 energy level in hydrogen atoms.
  • The Paschen series is named after Friedrich Paschen, a German physicist who studied atomic spectra in the late 19th and early 20th centuries. The wavelengths of the lines in the Paschen series can be described using the following formula, known as the Paschen formula:

1/λ = R_H [(1/3²) - (1/n²)]

  • where λ is the wavelength of the emitted or absorbed light, R_H is the Rydberg constant for hydrogen (approximately 1.097 × 10^7 m¹), and n is the principal quantum number indicating the energy level of the electron (n = 4, 5, 6, and so on).
  • The Paschen series includes several spectral lines, but since they lie in the infrared region, they are not visible to the human eye. These lines are significant for studying hydrogen and its presence in various astronomical objects, especially in the field of astrophysics.

While the exact wavelengths of the lines vary, here are a few examples of the Paschen series lines and their approximate wavelengths:

  • Paschen-alpha (1875.1 nm): Transition from the n = 4 energy level to the n = 3 energy level.
  • Paschen-beta (1281.8 nm): Transition from the n = 5 energy level to the n = 3 energy level.
  • Paschen-gamma (1093.1 nm): Transition from the n = 6 energy level to the n = 3 energy level.

These lines are commonly observed and studied in infrared spectroscopy, as they provide valuable information about the energy levels and transitions in hydrogen atoms.

Pfund series: 

  • This series lies in the IR region and represents transitions to the n = 5 energy level.
  • The Pfund series is a set of spectral lines that lie in the infrared (IR) region of the electromagnetic spectrum. These lines represent transitions of electrons in hydrogen atoms from higher energy levels to the n = 5 energy level. The Pfund series is named after August Herman Pfund, an American physicist who studied atomic spectra in the early 20th century.
  • The wavelengths of the lines in the Pfund series can be described by the following formula, known as the Pfund formula:

         1/λ = R_H [(1/5²) - (1/n²)]

  • where λ is the wavelength of the emitted or absorbed light, R_H is the Rydberg constant for hydrogen (approximately 1.097 × 10^7 m¹), and n is the principal quantum number indicating the energy level of the electron (n = 6, 7, 8, and so on).
  • Since the Pfund series lines lie in the infrared region of the spectrum, they are not visible to the human eye. However, they are of significant importance in spectroscopy, astrophysics, and the study of hydrogen.

Here are a few examples of the Pfund series lines and their approximate wavelengths:

  • Pfund-alpha (7457 nm): Transition from the n = 6 energy level to the n = 5 energy level.
  • Pfund-beta (4657 nm): Transition from the n = 7 energy level to the n = 5 energy level.
  • Pfund-gamma (4101 nm): Transition from the n = 8 energy level to the n = 5 energy level.

These lines are commonly observed and studied in infrared spectroscopy and astrophysical research, as they provide valuable information about the energy levels and transitions in hydrogen atoms.

The Pfund series, along with the Lyman, Balmer, Paschen, and Brackett series, completes the set of major hydrogen spectral series. Each series represents transitions to a specific energy level, with the Pfund series corresponding to transitions to the n = 5 energy level.

The study of these series played a crucial role in the development of quantum mechanics, as they provided evidence for the existence of discrete energy levels in atoms and the quantized nature of electrons. The observation and analysis of these spectral lines have deepened our understanding of the atomic structure and behavior of hydrogen, which is the simplest and most abundant element in the universe.

The Pfund series is a series of infrared spectral lines resulting from transitions of electrons in hydrogen atoms to the n = 5 energy level. Although these lines are not visible to the human eye, they are essential for the study of hydrogen and are used in various fields such as spectroscopy, astrophysics, and quantum mechanics.

Each series can have an infinite number of lines, but as the energy levels get closer together, the lines become denser and start to merge into a continuum. The Lyman series has the highest energy transitions and shortest wavelengths, while the Pfund series has the lowest energy transitions and longest wavelengths.

The hydrogen spectrum has played a crucial role in the development of quantum mechanics, as it provided evidence for the existence of discrete energy levels in atoms and the quantized nature of electrons.

 Image Credit:

3. Energy level diagram as straight lines
By Rajettan - Own work, CC BY-SA 4.0, https://commons.wikimedia.org/w/index.php?curid=41466201
4. Actual obsevation of line spectrum

By OrangeDog, CC BY-SA 3.0, https://commons.wikimedia.org/w/index.php?curid=6278485