Jove
Visualize
Contact Us
JoVE
x logofacebook logolinkedin logoyoutube logo
ABOUT JoVE
OverviewLeadershipBlogJoVE Help Center
AUTHORS
Publishing ProcessEditorial BoardScope & PoliciesPeer ReviewFAQSubmit
LIBRARIANS
TestimonialsSubscriptionsAccessResourcesLibrary Advisory BoardFAQ
RESEARCH
JoVE JournalMethods CollectionsJoVE Encyclopedia of ExperimentsArchive
EDUCATION
JoVE CoreJoVE BusinessJoVE Science EducationJoVE Lab ManualFaculty Resource CenterFaculty Site
Terms & Conditions of Use
Privacy Policy
Policies

Related Concept Videos

Inductively Coupled Plasma Atomic Emission Spectroscopy: Principle01:19

Inductively Coupled Plasma Atomic Emission Spectroscopy: Principle

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...
Inductively Coupled Plasma–Mass Spectrometry (ICP–MS): Overview01:19

Inductively Coupled Plasma–Mass Spectrometry (ICP–MS): Overview

In inductively coupled plasma–mass spectrometry (ICP–MS), an inductively coupled plasma (ICP) torch is used as an atomizer and ionizer. Solid samples are dissolved and volatilized before being introduced into the high-temperature argon plasma, while solution samples are nebulized and passed through the high-temperature argon plasma. Plasma dissociates the analytes and ionizes their component atoms to form a mixture of positive ions and molecular species. The positive ions are then passed on to...
Atomic Emission Spectroscopy: Instrumentation01:22

Atomic Emission Spectroscopy: Instrumentation

The instrumentation of atomic emission spectrometry (AES) involves various components, including atomization devices that convert samples into gas-phase atoms and ions. There are two main types of atomization devices: continuous and discrete atomizers.  Continuous atomizers, like plasmas and flames, introduce samples in a constant stream, while discrete atomizers inject individual samples using syringes or autosamplers. The most common discrete atomizer is the electrothermal atomizer.
Inductively Coupled Plasma Atomic Emission Spectroscopy: Instrumentation01:26

Inductively Coupled Plasma Atomic Emission Spectroscopy: Instrumentation

Inductively coupled plasma (ICP) is the common plasma source used in atomic emission spectroscopy (AES), a technique that detects and analyzes various elements in a sample. This method is often called inductively coupled plasma atomic emission spectroscopy (ICP-AES).
There are three main types of inductively coupled plasma atomic emission spectroscopy  (ICP-AES) instruments: sequential, simultaneous multichannel, and Fourier transform instruments, with the latter being less commonly used.
Gas Chromatography: Types of Detectors-II01:19

Gas Chromatography: Types of Detectors-II

In gas chromatography, different detectors are employed to meet specific analytical needs. These detectors are often categorized based on their detection mechanisms and the types of compounds they are best suited to analyze. Thermal Conductivity Detectors (TCD), Flame Ionization Detectors (FID), and Electron Capture Detectors (ECD) represent common categories, each with unique operating principles and applications. However, beyond these, several other detectors are designed for more specialized...
Van de Graaff Generator01:15

Van de Graaff Generator

Van de Graaff generators (or Van de Graaffs) are devices used to demonstrate high voltage due to static electricity that can also be used for research. Robert Van de Graaff first built one in 1931 (based on original suggestions by Lord Kelvin) for use in nuclear physics research.
Van de Graaff uses both smooth and pointed surfaces, conductors, and insulators to generate large static charges and, hence, large voltages. A substantial excess charge can be deposited on the sphere because it moves...

You might also read

Related Articles

Articles linked to this work by shared authors, journal, and citation graph.

Sort by
Same author

Hygiene of the Teeth.

The Dental register·2021
Same author

Improved mount and alignment procedures for a rapid-scan fabry-perot interferometer.

Applied optics·2010
Same author

Gas discharge ion source III. Modified Berkeley multifilament ion source.

The Review of scientific instruments·1978
Same author

Gas discharge ion source. II. Duopigatron.

The Review of scientific instruments·1978

Related Experiment Video

Updated: Jul 2, 2026

An Atmospheric Pressure Plasma Setup to Investigate the Reactive Species Formation
08:36

An Atmospheric Pressure Plasma Setup to Investigate the Reactive Species Formation

Published on: November 3, 2016

Gas discharge ion source. I. Duoplasmatron.

F M Bacon1

  • 1Sandia Laboratories, Albuquerque, NM 87185, USA.

The Review of Scientific Instruments
|April 1, 1978
PubMed
Summary

Investigating plasma expansion cups in duoplasmatron ion sources revealed that a modified steel and boron nitride design significantly improved ion beam current and stability. This optimized cup enhances performance for scientific applications.

Area of Science:

  • Plasma Physics
  • Ion Source Technology
  • Materials Science

Background:

  • Duoplasmatron ion sources are critical for generating ion beams.
  • The plasma expansion cup influences ion beam characteristics.
  • Previous designs had limitations in performance and durability.

Purpose of the Study:

  • To investigate the effect of different plasma expansion cup materials and potentials on duoplasmatron ion source operation.
  • To optimize the plasma expansion cup design for improved ion beam current, energy, mass, and current density distributions.
  • To enhance the durability of the anode insert.

Main Methods:

  • Experimental investigation of copper and mild steel plasma expansion cups.
  • Measurement of total ion current, ion energy distribution, ion mass distribution, and current density distribution.

More Related Videos

Photoelectron Imaging of Anions Illustrated by 310 Nm Detachment of F−
06:53

Photoelectron Imaging of Anions Illustrated by 310 Nm Detachment of F−

Published on: July 27, 2018

Non-equilibrium Microwave Plasma for Efficient High Temperature Chemistry
07:17

Non-equilibrium Microwave Plasma for Efficient High Temperature Chemistry

Published on: August 1, 2017

Related Experiment Videos

Last Updated: Jul 2, 2026

An Atmospheric Pressure Plasma Setup to Investigate the Reactive Species Formation
08:36

An Atmospheric Pressure Plasma Setup to Investigate the Reactive Species Formation

Published on: November 3, 2016

Photoelectron Imaging of Anions Illustrated by 310 Nm Detachment of F−
06:53

Photoelectron Imaging of Anions Illustrated by 310 Nm Detachment of F−

Published on: July 27, 2018

Non-equilibrium Microwave Plasma for Efficient High Temperature Chemistry
07:17

Non-equilibrium Microwave Plasma for Efficient High Temperature Chemistry

Published on: August 1, 2017

  • Testing of cups at anode potential and floating potential.
  • Design and testing of a modified cup with tapered steel walls and a boron nitride insert, using a molybdenum anode insert.
  • Main Results:

    • Copper cup resulted in a sharply peaked current density; steel cup at anode potential yielded flatter distributions but lower total current.
    • Steel cup at floating potential improved total current and current density flatness compared to the copper cup.
    • The modified tapered steel cup with boron nitride insert and molybdenum anode showed superior performance, achieving 200 mA total beam current at 24 A arc current.
    • Molybdenum anode insert demonstrated superior erosion resistance over copper.

    Conclusions:

    • Plasma expansion cup material and electrical potential significantly impact duoplasmatron ion source performance.
    • A modified design combining tapered steel walls, boron nitride lining, and a molybdenum anode insert offers superior ion beam generation and durability.
    • The optimized design represents a significant advancement in duoplasmatron ion source technology.