Laser Induced breakdown spectroscopy in Water for elemental analysis. PowerPoint PPT Presentation

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Title: Laser Induced breakdown spectroscopy in Water for elemental analysis.


1
Laser Induced breakdown spectroscopy in Water for
elemental analysis.
  • Satyanarayan Ray Pitambar Mohapatra
  • Project Guide Dr. R.K. Thareja

2
Advantages of LIBS technique
  • Can be used for rapid and remote analysis.
  • Real time analysis possible.
  • Complete elemental coverage can be achieved.
  • The analysis spot size is small.
  • Relatively low detection limit ( ppm/ppb).

3
Possible application
  • Detection of elements in nuclear reactors.
  • Detection of elements inside deep sea.
  • Space mission detection of elements in other
    planets.
  • Environmental monitoring (soil contamination,
    particulates) .
  • Materials analysis (metals, plastics).  
  • Forensics and biomedical studies (teeth, bones
    analysis).  
  • Military and safety needs (explosive particles,
    chemical and biological warfare agents e.g.
    Anthrax).  
  • Art restoration/conservation (pigments,
    precious/ancient metals).  

4
LIBS on Mars !
  • A 300 mJ laser pulse can detect from 25m away.
  • A 2 J laser pulse can detect from 100m away.
  • photo credit
    Chemistry Division , Los Alamos National
    Laboratory

5
Set up
6
Setup specification
  • Wavelength of laser radiation 355 nm
  • Energy of laser radiation 18 mJ
  • Focal length of Plano-convex quartz lens 10 cm
  • Pulse repetition rate 10 Hz
  • Gate width for time integrated spectra 2 micro
    second
  • Gate width for time- resolved spectra 500 ns
  • Gate delay with respect to laser pulse 300 ns

7
Advantages of water based test samples
  • Relatively low conc. Solution (ppm) can be
    prepared.
  • Solution in water are more homogeneous than solid
    ( so spatial variation of concentration is not
    there).

8
Why Na ?
  • Easily available element to start with.
  • To determine the concentration of Na in sea ice.
  • Na concentration in blood and cells.

9
Typical sodium lines time integrated
  • Na I 589 nm
  • ( 3s 2S-3p 2P0)( J 1)
  • D1 line
  • Na I 589.6 nm
  • ( 3s 2S-3p 2P0)( J 0)
  • D2 line

10
Time resolved data for concentration 38 ppm
11
Time resolved observation for concentration 102
ppm, gate delay 300 ns
12
Time resolved data of Sodium line for
Concentration 409 ppm, gate delay 300 ns
13
Calibration curve D2 line
  • Detection limit 3s /m
  • Detection limit observed (123 17) ppm

14
Calibration curve for D1 line
  • Detection limit 3s/m
  • Detection limit observed (11613) ppm

15
Calibration curve D2 line
  • Detection limit 3s/m
  • Detection limit observed (19 5) ppm

16
Calibration curve for D1 line
  • Detection limit 3s/m
  • Detection limit observed (7.83) ppm

17
Detection limit optimization
  • Two types of background noise plasma continuum
    detector noise.
  • Optimization
  • Optimum gating time optimum position
  • of detector.
  • Study of temporal and spatial expansion of plasma
    in air.

18
Problems to be fixed and future plans
  • An actual set up should have the capability to
    distinguish among several elements.
  • For that suitable wavelength of laser radiation
    to be decided.
  • Suitable energy of laser radiation to be
    determined.
  • Plasma parameters (plasma temperature, plasma
    density) to be determined for different
    elements.
  • The LIBS method should be compared with other
    standard authentic methods.
  • Salt solution of sodium and magnesium in the form
    of ice cubes to be analyzed.
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