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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.
Raman Spectroscopy Instrumentation: Overview01:26

Raman Spectroscopy Instrumentation: Overview

A conventional Raman spectrophotometer includes a laser source, a sample holding system, a wavelength selector, and a detector.
The monochromatic laser source, typically using visible or near-infrared radiation, generates a highly focused beam of light. This light interacts with the molecules of the sample, scattering some of the light. Liquid and gaseous samples are usually tested in ordinary glass capillaries, while solids can be analyzed as powders packed in capillaries or as potassium...
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.
Atomic Absorption Spectroscopy: Instrumentation01:22

Atomic Absorption Spectroscopy: Instrumentation

An atomic absorption spectrophotometer (AAS) comprises several components: a radiation source, an atomizer, a monochromator, and a detector. The radiation source can be a hollow-cathode lamp (HCL) or an electrodeless-discharge lamp (EDL), both of which provide a narrow emission line of the required wavelength. However, some instruments use continuum sources and high-resolution monochromators to achieve a narrow range of radiation.
The atomizer used in AAS can be either a flame atomizer or an...
Mass Analyzers: Overview01:13

Mass Analyzers: Overview

The mass analyzer is a crucial component of the mass spectrometer. In the ionization chamber, the vaporized sample is bombarded with a high-energy electron beam to generate a radical cation and further fragment into neutral molecules, radicals, and cations. A series of negatively charged accelerator plates accelerate the cations into the mass analyzer. The mass analyzer separates ions according to their mass-to-charge (m/z) ratios and then directs them to the detector. The common types of mass...
Mass Analyzers: Common Types01:19

Mass Analyzers: Common Types

The quadrupole mass analyzer consists of four cylindrical metal rods arranged in a diamond carrying a DC voltage and a radio-frequency AC voltage. The motion of ions through the quadrupole depends on the field strength, causing only ions of a certain m/z to resonate successfully and strike the detector at a given field strength. Though the transmission rate for these analyzers is high, the exact elemental composition of the sample is not determined because of low resolution; however, they are...

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Related Experiment Video

Updated: Jun 17, 2026

Measurement of Ultrafast Vibrational Coherences in Polyatomic Radical Cations with Strong-Field Adiabatic Ionization
08:22

Measurement of Ultrafast Vibrational Coherences in Polyatomic Radical Cations with Strong-Field Adiabatic Ionization

Published on: August 6, 2018

A time-resolving spectrograph for free-flight ballistic range application.

I D Liu1

  • 1AC Electronics Defense Research Laboratories,General Motors Corporation, Santa Barbara, California 93017, USA.

Applied Optics
|January 12, 2010
PubMed
Summary
This summary is machine-generated.

This study analyzed hypervelocity object emissions using spectroscopy. Researchers observed molecular species in the near wake of ablating models, suggesting potential for further wake studies.

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Last Updated: Jun 17, 2026

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Area of Science:

  • Fluid Dynamics
  • Spectroscopy
  • Aerophysics

Background:

  • Understanding hypervelocity object dynamics is crucial for aerospace applications.
  • Spectroscopic analysis provides insights into the physical and chemical processes occurring during high-speed flight.
  • Previous studies have limited detailed spectral analysis of the near-wake region.

Purpose of the Study:

  • To obtain time-resolved spectra of hypervelocity spheres and cones.
  • To identify molecular species present in the near-wake region of ablating models.
  • To assess the feasibility of using advanced imaging for far-wake emission studies.

Main Methods:

  • Utilized a free-flight ballistic range.
  • Employed a large aperture, slitless spectrograph coupled with an image converter camera.
  • Analyzed spectral data from nonablating and ablating models at hypervelocities.

Main Results:

  • Observed emission primarily from the shock cap for nonablating spheres.
  • Identified molecular species like C(2), CH, CN, Cu(2), CuF, CuO, BeO, and AlO in the near wake of ablating models.
  • Detected distinct spectral signatures for hydrocarbon and metallic models.

Conclusions:

  • The study successfully characterized near-wake emissions from hypervelocity models.
  • Spectroscopic methods reveal the presence of specific molecular species under hypervelocity conditions.
  • Further investigation into far-wake emission using image intensifiers is warranted.