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Presented By:-
Pallavi Sisodia
M.Sc I.C.A (3rd semester)
JIWAJI UNIVESITY
ï‚–
ï‚™ Introduction
ï‚™ Production of x-ray
ï‚™ X-ray absorption spectroscopy
ï‚™ X-ray fluorescence spectroscopy
ï‚™ Instrumentation
ï‚™ Detectors
ï‚™ Applications
ï‚™ References
CONTENTS
•X-rays are short-wavelength electromagnetic
radiation .
• X-rays have a wavelength in range of 0.01–10 nm.
Analytical range – 0.7-2 Angstrom
• X- Ray spectroscopy is based upon measurement of
emission, absorption, scattering, fluorescence and
diffraction of electromagnetic radiation.
Produced in three ways:
1. By bombardment of a metal target with a beam of high
energy electrons
2. By exposure to primary beam of X-rays to generate
secondary X-Rays
3. By employment of radioactive source whose decay
process results in X-Ray emission.
• An x-ray is absorbed by an atom
when the energy of the x-ray is
transferred to a core-level
electron (K, L, or M shell) which is
ejected from the atom.
• The atom is left in an excited state
with an empty electronic level (a
core hole). Any excess energy from
the x-ray is given to the ejected
photoelectron.
Principle of XAS is Lambert Beer’s law .
Transmission of X-rays are given
by formula :–
• It=Io exp(-μt)
Where , t is thickness of material
μ is linear absorption coefficient
It = intensity of transmitted radiation
Io= intensity of incident radiation
• X-Ray Fluorescence (XRF) can be considered in a
simple three step process occurring at the atomic
level:
1. An incoming X-Ray knocks out an electron
from one of the orbitals surrounding the
nucleus within an atom of the material.
2. A hole is produced in the orbital, resulting in a
high energy, unstable configuration for the
atom.
3. To restore equilibrium, an electron from a
higher energy, outer orbital falls into the hole.
Since this is a lower energy position, the excess
energy is emitted in the form of a fluorescent X-
Ray.
• Gas – Filled detector
• Scintillation detector
• Solid state detector
X-ray
Spectroscopy
Applications
Thickness
determination
Internal
Impurities
detection
Mining (e.g.,
measuring the
grade of ore)
Determination of
bond length and
bond angles
Ceramic and
glass
manufacturing
Detect broken
bones
• Organic spectroscopy, Willaim Kemp
• Instrumental method of chemical analysis
• Instrumental method of chemical analysis. Wilard
•https://www.slideshare.net/solairajananant/xray-spectroscopy-13887430
•http://sydney.edu.au/science/chemistry/facilities/xray/xray-
applications.shtml
Pallavi

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Pallavi

  • 1. Presented By:- Pallavi Sisodia M.Sc I.C.A (3rd semester) JIWAJI UNIVESITY
  • 2. ï‚– ï‚™ Introduction ï‚™ Production of x-ray ï‚™ X-ray absorption spectroscopy ï‚™ X-ray fluorescence spectroscopy ï‚™ Instrumentation ï‚™ Detectors ï‚™ Applications ï‚™ References CONTENTS
  • 3. •X-rays are short-wavelength electromagnetic radiation . • X-rays have a wavelength in range of 0.01–10 nm. Analytical range – 0.7-2 Angstrom • X- Ray spectroscopy is based upon measurement of emission, absorption, scattering, fluorescence and diffraction of electromagnetic radiation.
  • 4. Produced in three ways: 1. By bombardment of a metal target with a beam of high energy electrons 2. By exposure to primary beam of X-rays to generate secondary X-Rays 3. By employment of radioactive source whose decay process results in X-Ray emission.
  • 5. • An x-ray is absorbed by an atom when the energy of the x-ray is transferred to a core-level electron (K, L, or M shell) which is ejected from the atom. • The atom is left in an excited state with an empty electronic level (a core hole). Any excess energy from the x-ray is given to the ejected photoelectron.
  • 6. Principle of XAS is Lambert Beer’s law . Transmission of X-rays are given by formula :– • It=Io exp(-μt) Where , t is thickness of material μ is linear absorption coefficient It = intensity of transmitted radiation Io= intensity of incident radiation
  • 7. • X-Ray Fluorescence (XRF) can be considered in a simple three step process occurring at the atomic level: 1. An incoming X-Ray knocks out an electron from one of the orbitals surrounding the nucleus within an atom of the material. 2. A hole is produced in the orbital, resulting in a high energy, unstable configuration for the atom. 3. To restore equilibrium, an electron from a higher energy, outer orbital falls into the hole. Since this is a lower energy position, the excess energy is emitted in the form of a fluorescent X- Ray.
  • 8.
  • 9. • Gas – Filled detector • Scintillation detector • Solid state detector
  • 10. X-ray Spectroscopy Applications Thickness determination Internal Impurities detection Mining (e.g., measuring the grade of ore) Determination of bond length and bond angles Ceramic and glass manufacturing Detect broken bones
  • 11. • Organic spectroscopy, Willaim Kemp • Instrumental method of chemical analysis • Instrumental method of chemical analysis. Wilard •https://www.slideshare.net/solairajananant/xray-spectroscopy-13887430 •http://sydney.edu.au/science/chemistry/facilities/xray/xray- applications.shtml