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

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.
UV–Vis Spectrometers01:14

UV–Vis Spectrometers

The absorbance of UV and visible (UV–visible) radiations is measured using a UV–visible spectrophotometer. Deuterium lamps, which emit UV radiation, and tungsten lamps, which produce radiation in the visible region, are used as light sources in UV–visible spectrophotometers. A monochromator or prism is used for diffraction grating, i.e., to split the incoming radiation into different wavelengths. A system of slits is used to focus the desired wavelength on the sample cell. Samples for...
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...
IR Spectrum Peak Intensity: Dipole Moment01:20

IR Spectrum Peak Intensity: Dipole Moment

The dipole moment of a bond is the product of the partial charge on either atom and the distance between them. Dipole moments influence the efficiency of IR absorption and the peak intensity. When a bond with a dipole moment is placed in an electric field, the direction of the field determines if the bond is compressed or stretched. Electromagnetic radiation consists of an electric field component that rapidly reverses direction. It follows that polar bonds are alternately stretched and...
IR Spectrometers01:25

IR Spectrometers

There are two main infrared (IR) spectrophotometers: dispersive IR spectrometers and Fourier transform infrared (FTIR) spectrometers. In a dispersive IR spectrometer, a beam of infrared radiation produced by a hot wire is divided into two parallel equal-intensity beams using mirrors. One beam passes through the sample, while another is a reference beam. The beams then move through the monochromator, which separates the radiations into a continuous spectrum of different frequencies. The...
Atomic Emission Spectroscopy: Lab01:29

Atomic Emission Spectroscopy: Lab

AES is a powerful analytical technique, especially effective when used with plasma sources, producing abundant spectra in characteristic emission lines. The Inductively Coupled Plasma (ICP), in particular, yields superior quantitative analytical data due to its high stability, low noise, low background, and minimal interferences under optimal experimental conditions. However, newer air-operated microwave sources are emerging as promising alternatives that could be more cost-effective than...

You might also read

Related Articles

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

Sort by
Same author

Evaluation of immunogenicity of enterobactin conjugate vaccine for the control of Escherichia coli mastitis in dairy cows.

Journal of dairy science·2023
Same author

The cross-reactive idiotype of A-strain mice Serological and structural analyses.

Immunology today·2014
Same author

Bayesian estimation of the diagnostic accuracy of a multiplex real-time PCR assay and bacteriological culture for 4 common bovine intramammary pathogens.

Journal of dairy science·2012
Same author

Human exposure from dioxins in soil.

Environmental science & technology·2011
Same author

Study of 100 cases of abdominal pain in service women.

United States naval medical bulletin·2010
Same author

Solar magnetograph employing integrated diode arrays.

Applied optics·2010

Related Experiment Video

Updated: Jun 16, 2026

Studying Soft-matter and Biological Systems over a Wide Length-scale from Nanometer and Micrometer Sizes at the Small-angle Neutron Diffractometer KWS-2
11:27

Studying Soft-matter and Biological Systems over a Wide Length-scale from Nanometer and Micrometer Sizes at the Small-angle Neutron Diffractometer KWS-2

Published on: December 8, 2016

Kitt Peak 60-cm vacuum telescope.

W C Livingston, J Harvey, A K Pierce

    Applied Optics
    |February 16, 2010
    PubMed
    Summary

    A new solar research tool was developed affordably, aiming to observe magnetic and velocity fields. Initial tests show potential but require improvements in optical quality and efficiency for better performance.

    Area of Science:

    • Solar Physics
    • Astronomy
    • Astrophysics

    Background:

    • Budget constraints necessitated innovative approaches in solar research instrumentation.
    • Observing solar magnetic and velocity fields requires high-resolution, synoptic observational tools.

    Purpose of the Study:

    • To describe a newly developed, cost-effective instrument for solar research.
    • To achieve diffraction-limited resolution for observing solar magnetic and velocity field structures.
    • To assess the initial performance and identify areas for improvement.

    Main Methods:

    • Utilized oversize mirrors and windows to mitigate thermal edge effects.
    • Positioned the coelostat feed outside the vacuum for economic reasons.
    • Selected a site with prevailing winds to minimize thermal interference.

    More Related Videos

    High Speed Sub-GHz Spectrometer for Brillouin Scattering Analysis
    13:31

    High Speed Sub-GHz Spectrometer for Brillouin Scattering Analysis

    Published on: December 22, 2015

    Related Experiment Videos

    Last Updated: Jun 16, 2026

    Studying Soft-matter and Biological Systems over a Wide Length-scale from Nanometer and Micrometer Sizes at the Small-angle Neutron Diffractometer KWS-2
    11:27

    Studying Soft-matter and Biological Systems over a Wide Length-scale from Nanometer and Micrometer Sizes at the Small-angle Neutron Diffractometer KWS-2

    Published on: December 8, 2016

    High Speed Sub-GHz Spectrometer for Brillouin Scattering Analysis
    13:31

    High Speed Sub-GHz Spectrometer for Brillouin Scattering Analysis

    Published on: December 22, 2015

  • Conducted tests including Modulation Transfer Function (MTF) and optical transmission measurements.
  • Acquired full disk magnetograms and photoheliograms for performance evaluation.
  • Main Results:

    • Measured MTF indicates a response of 0.2 at 1 arcsecond, below the diffraction-limited target of ~0.8.
    • System optical transmission, including the spectrograph, is limited to 2-3% across the observed wavelengths.
    • Initial magnetograms and photoheliograms demonstrate the system's capability to capture solar features.

    Conclusions:

    • The new solar research tool demonstrates feasibility despite budget limitations.
    • Significant improvements in optical quality and system efficiency are needed to reach diffraction-limited performance.
    • Further development is required to optimize the instrument for advanced solar magnetic and velocity field studies.