JoVE Logo

Sign In

Inductively coupled plasma (ICP) is the most widely used plasma source in atomic emission spectroscopy (AES), also known as Inductively Coupled Plasma Optical Emission Spectroscopy (ICP-OES). The ICP source, or torch, consists of three concentric quartz tubes with argon gas flowing through them. A spark from a Tesla coil initiates the ionization of argon, generating a high-temperature plasma.

The ions and electrons produced interact with the fluctuating magnetic field created by a water-cooled induction coil powered by a radio-frequency generator. This interaction leads to ohmic heating, forming a high-temperature plasma and providing an optimal environment for elemental analysis. Sample introduction in ICP-AES can be achieved using different methods, such as a concentric glass nebulizer or electrothermal vaporization. In the former, the sample is transported by the Bernoulli effect with the help of high-velocity argon gas, forming fine droplets that enter the plasma. In the latter, the sample is vaporized in a furnace before being introduced into the plasma via a stream of argon.

Configurations for ICP spectrometers include radial or axial viewing. Horizontally oriented, axially viewed plasma is ideal for high-sensitivity analyses. It features a unique cooled cone interface (CCI) that prevents the optics from considering the cooler plasma tail, reducing interferences and improving the system's tolerance to high dissolved solids. Vertically oriented, radially viewed plasma is suitable for challenging applications, such as the analysis of oils, organic solvents, geological/metal digests, and high total dissolved solids (TDS) solutions.

Isothermal contours depict the range of temperatures experienced by sample atoms in the plasma during their residence time before reaching the observation point. This results in more complete atomization and fewer chemical interferences. The ICP source in AES offers numerous advantages, including chemically inert atomization, uniform temperature distribution, linear calibration curves over a wide range of concentrations, and significant ionization, making it an excellent choice for ICP-MS applications.

From Chapter 14:

article

Now Playing

14.12 : Inductively Coupled Plasma Atomic Emission Spectroscopy: Principle

Atomic Spectroscopy

205 Views

article

14.1 : Atomic Spectroscopy: Absorption, Emission, and Fluorescence

Atomic Spectroscopy

205 Views

article

14.2 : Atomic Spectroscopy: Effects of Temperature

Atomic Spectroscopy

83 Views

article

14.3 : Atomic Absorption Spectroscopy: Overview

Atomic Spectroscopy

162 Views

article

14.4 : Atomic Absorption Spectroscopy: Instrumentation

Atomic Spectroscopy

115 Views

article

14.5 : Atomic Absorption Spectroscopy: Radiation and Light Sources

Atomic Spectroscopy

104 Views

article

14.6 : Atomic Absorption Spectroscopy: Atomization Methods

Atomic Spectroscopy

79 Views

article

14.7 : Atomic Absorption Spectroscopy: Interference

Atomic Spectroscopy

135 Views

article

14.8 : Atomic Absorption Spectroscopy: Lab

Atomic Spectroscopy

61 Views

article

14.9 : Atomic Emission Spectroscopy: Overview

Atomic Spectroscopy

170 Views

article

14.10 : Atomic Emission Spectroscopy: Instrumentation

Atomic Spectroscopy

63 Views

article

14.11 : Atomic Emission Spectroscopy: Interference

Atomic Spectroscopy

26 Views

article

14.13 : Inductively Coupled Plasma Atomic Emission Spectroscopy: Instrumentation

Atomic Spectroscopy

60 Views

article

14.14 : Atomic Emission Spectroscopy: Lab

Atomic Spectroscopy

43 Views

article

14.15 : Atomic Fluorescence Spectroscopy

Atomic Spectroscopy

37 Views

See More

JoVE Logo

Privacy

Terms of Use

Policies

Research

Education

ABOUT JoVE

Copyright © 2025 MyJoVE Corporation. All rights reserved