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Atomic Absorption
Spectroscopy
MISS AYESHA SHAFI
Contents
 Introduction
 Principle
 Theory
 Instrumentation
 Applications
Introduction
 Atomic Absorption Spectroscopy is a very common technique for detecting
metals and a few non-metal in samples
 It is very reliable and simple to use.
 It can analyze over 62 elements.
 It also measures the concentration of metals in the sample.
HISTORY:
The first atomic absorption spectrometer was built by CSIRO
scientist Alan Walsh in 1954. Shown in the picture Alan
Walsh(left), with a spectrometer.
Elements detectable by atomic absorption are highlighted in pink in this
periodic table
TYPES OF ATOMIC
SPECTRA
1) ATOMIC EMISSION SPECTRA:
2) ATOMIC ABSORPTION SPECTRA:
3) ATOMIC FLUORESCENCE SPECTRA
COMPARISON
ATOMIC EMISSION
SPECTROSCOPY
• Examines the wavelengths of photons
emitted by atoms or molecules during
their transition from an excited state
to a lower energy state.
• Each element emits a characteristic set
of discrete wavelengths.
• By observing these wavelengths the
elemental composition of the sample
can be determined.
ATOMIC ABSORPTION
SPECTROSCPY
• Measures the loss of
electromagnetic energy after
it illuminates the sample
under study.
• The energy in certain amount
is absorbed during transition
to the higher level.
• The amount of energy
absorbed gives estimate of
the concentration of the
analyte in the sample.
 The technique uses basically the principle that free atoms (gas) generated in an
atomizer can absorb radiation at specific frequency.
 Atomic-absorption spectroscopy quantifies the absorption of ground state atoms
in the gaseous state .
 The atoms absorb ultraviolet or visible light and make transitions to higher
electronic energy levels. The analyte concentration is determined from the amount
of absorption.
THEORY OF ATOMIC ABSORPTION
SPECTROSCOPY
 Atomic absorption spectroscopy is a method of elemental analysis.
 When a solution containing the metallic species is introduced into a flame, the vapours of metallic species
will be obtained. Some of the metal atoms may be raised to an energy level sufficiently high to emit the
characteristic radiation of the metal during their return but a large percentage of metal will remain in the
non-emitting ground state. These ground state elements are receptive of light radiation of their own
specific wavelength. Thus when a light of this wavelength is allowed to pass through a flame having atoms
of metallic species, part of light is absorbed and the absorption is directly propotional to the density in the
flame.
 It is particularly useful for determining trace metal in liquids and is almost independent of molecular form
of the metal in the sample.
 The method is very sensitive and can detect the different metals in concentration as low as and one
frequently lower than 1 ppm.
 A disadvantage of the method is that only one element can be determined at a time.
 This method has limited use in quantitative analysis.
THEORY OF ATOMIC ABSORPTION
SPECTROSCOPY
 .
 The total amount of light absorbed may be given mathematically by the following expressions:
Total number of light absorbed = πe2/mc Nf
Where,
e= is the charge on the electron of mass
m= mass of electron
c= is the speed of light
N= is the total number of atoms that can absorb at frequency in the light path
v= frequency
f= is the oscillator strength or ability of each atom to absorb at frequency
π= is constant
The above equation can be written as:
Total amount of light absorbed= Constant x N x f
THEORY OF ATOMIC ABSORPTION SPECTROSCOPY
INSTRUMENTATIONOF ATOMIC ABSORPTION
SPECTROSCOPY
Atomic absorption spectroscopy lec
Atomic absorption spectroscopy lec
Atomic absorption spectroscopy lec
Atomic absorption spectroscopy lec
Atomic absorption spectroscopy lec
Instrumentation
Atomic absorption spectrophotometer based on the following components.
 Source
 Atomizer
 Monochromator
 Detector
 Read out devise
Radiation Source
 The main radiation sources are used for the atomic absorption are following.
 Hollow cathode lamp (HCL)
 Electrode less discharge lamp (EDL)
 Hollow cathode lamp :
 It consist of tungsten anode and a cylindrical cathode sealed in a glass tube filled
with neon or Argon at a pressure of 1-5 torr.
 When a potential of 300V is applied, ionization of inert gas occur and a current of
5-20mA is generated as ions.
Hollow Cathode lamp:
 A portion of the sputtered metal atoms is in excited states and thus emit their
characteristics radiation as they returns to the ground state.
Electrode less Discharge Lamp
 A typical lamp is constructed from a sealed quartz tube containing a few torr of
an inert gas such as argon and a small quantity of the metal whose spectrum is of
interest.
 The lamp contain no electrode but instead is energized by an intense field of
radiofrequency or microwave radiation.
SOURCE MODULATION
 Used to eliminate the interferences caused by
emission of radiation by the flame. For these,
output of the radiation source is modulated so
that the intensity fluctuates at a constant
frequency .
 An easy way to eliminate the emission from the
source is to interpose a circular metal disk or
chopper in the beam between the source and
the flame.
Atomizers
 The process of converting an analyte in solid, liquid or solution form to a free
gaseous atom is called as the atomization and the instrument used for this
purpose is called as the atomizers.
 Two types of the atomizers are used.
 A) flame atomizer
 B) Electrothermal atomizer
Flame atomizer
 In flame atomizer, the sample is first converted into a fine mist consisting of small
droplets of solution.
 It is accomplished by using a nebulizer assembly.
 The sample is aspirated into a spray chamber by passing a high pressure stream
consisting of one or more combustion gases, part the end of a capillary tube
immersed in the sample.
 The impact of the sample with the glass impact head produces an aerosol mist.
 The aerosol mist mixes with the combustion gases in the spray chamber before
passing to flame which desolvates the aerosol mist to a dry aerosol of small solid
particles.
 Subsequently, flame thermal energy volatilizes the particles, producing a vapors
consisting of molecular species, ionic species and free atoms.
 Thermal energy in flame atomization is provided by the combustion of a fuel –
oxidant mixture.
FLAME ATOMIZER:
• Flame is used to atomize the sample
• Sample when heated is broken into its atoms
PRINCIPLE:
• High temperature of flame causes excitation
• Electrons of the atomized sample are promoted to higher orbitals, by absorbing
certain amount of energy
QUANTITATIVE ANALYSIS:
• The amount of energy absorbed is specific for a particular element (for electronic
transition).
SAMPLE NEBULIZER
ASSEMBLY
CONVERSION
INTO FINE
MIST & SMALL
DROPLETS OF
SOLUTION
ASPIRATED
INTO SPRAY
CHAMBER
(MIXING
CHAMBER)
AEROSOL
MIXES WITH
COMBUSTIO
N GASES
FLAME
(ATOMIZATIO
N OCCURS)
Sample to
be nebulized
is taken
(aspirated)
via a
capillary
tube
Nebulizer:
sample+fuel
+
oxidant
fine mist or
aerosol
Natural Gas Air 1700-1900 39-43
Natural Gas Oxygen 2700-2800 370-390
Hydrogen Air 2000-2100 300-440
Hydrogen Oxygen 2550-2700 900-1400
Acetylene Air 2100-2400 158-266
Acetylene Oxygen 3050-3150 1100-2480
Acetylene Nitrous Oxide 2600-2800 285
Flame Structure
Flame atomizers
 Flame atomizers are of two types
 Continuous
 Discrete
 Continuous: the sample is fed into atomizer at a constant rate. The spectral line is
then constant with time.
 Discrete: A measured quantity of the sample is introduced as a plug of liquid or
solid. The spectral line is rises to a maximum and then decreases to zero.
Electro thermal Atomizers
 A typical electro thermal atomizer also known as graphite furnace, consisting of a
cylindrical graphite tube approximately 1-3 cm in length and 3-8 mm in diameter.
 The graphite tube is housed in an assembly that seals the end of the tube with
optically transparent windows. The assembly also allows for the passage of
continuous stream of inert gas, protecting the graphite tube from oxidation and
removing the gaseous products produced during atomization. A power supply is
used to pass a current through the graphite tube, resulting in resistive heating.
Construction of electro thermal atomizers
 .
Graphite tube
Enclosed water cooled
housing
Transparent windows
Inert purge gas
control
Electrical contact
Electro thermal Atomizers
 Samples between 5 and 50 micro liter are injected into the graphite tube through
a small diameter hole located at the top of the tube.
 Atomization takes place in three stages:
Atomization
of sample
1.Drying
2. Ashing
3.Atomizatio
Electro thermal Atomizers
 In the first stage sample is dried by using a current that raises the temperature of
the graphite tube to about 110◦C and desolvation leaves the sample as a solid
residue.
 In the second stage, which is called as the ashing, the temperature is increased to
about 350-1200 ◦C. At this temperature the sample is converted into the carbon
dioxide and water and volatile inorganic material are vaporized. These gases are
removed by the inert gas flow.
 In the final stage, the sample is atomized by rapidly increasing the temperature to
2000-3000 ◦C.
 Three stages are completed in 45-90 sec.
 The analyte concentration in the resulting vapor phase may be as much as 1000
times greater than that produced by flame atomization.
Instrumentation (continues)
 Monochromators:
 Monochromators are used to isolate the narrow band width of wavelength that
are absorbed by the metals.
 Detectors:
 the photomultiplier is used to detect the light absorbed by the analyte. It is same
as described in UV/ mass spectrometer.
Working of atomic absorption spectrophotometer
 Single beam atomic absorption spectrophotometer:
Single beam measurements are depended upon the varying intensity of a single
single beam of light having a single optical path. That is why called as single beam
AA spectrophotometer. It consist of hollow cathode lamp, a chopper, atomizer
and a simple grating spectrophotometer with photomultiplier detector.
Double beam atomic absorption spectrophotometer:
the beam from the hollow cathode source is split by mirror chopper so that one half
passed through the flame and the other half around it. The two beams are then
recombined by a half silver mirror and passed into grating monochromator. The
photomultiplier tube serves as the detector
Atomic absorption spectroscopy lec
Single / double beam spectrophotometer
4343
Atomic absorption spectrophotometer
I nstrumentationI nstrumentation
SAMPLE PREPARATION T
the preparation of the sample solution for a solid
material is most time consuming step of process
of analysis in an atomic absorption spectroscopy.
It involves following steps;
Weighing of sample
Dissolution in appropriate solvent or
digestion using different techniques
Dilution of sample if necessary
 Pharmaceutical
 Biological
 Biochemical
For detection of purity and
consistency of these trace
metals
Also for quantitative
determination of metals mainly
in solid sample as mineral, ores
and alloys
Apllication of atomic absorption spectroscopy
• Magnesium in cast iron
• Silver, Zinc, Copper and Lead in
Cadmium metal
• Method of multiple standard addition
• A plot of absorbance against the
amount of standard can be used to
determine the amount of copper in a
sample.
 Determination of trace metal in a silicon foam cavity wound
dressing
 Zinc in Zinc insulin suspension and tetracosactrin
Zinc injection
 Copper and Iron in ascorbic acid
 Aluminum in albumin solution and Ca, Mg,
Mercury
 Zinc in water used for diluting haemodialysis solution
•For the analysis of pharmaceutically or
therapeutically essential component of formulation,
such as Zinc in Zinc-insulin, minerals in multivitamin-
mineral preparation and Ca, Mg, Al in antacids.
•To establish concentration limits where the metal is
regarded as an impurity.
•Mining industries
•Petroleum industries
•Determination of metallic elements in
food industry like Copper, Zinc and Nickel
in vegetable oil and copper in beer.

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Atomic absorption spectroscopy lec

  • 2. Contents  Introduction  Principle  Theory  Instrumentation  Applications
  • 3. Introduction  Atomic Absorption Spectroscopy is a very common technique for detecting metals and a few non-metal in samples  It is very reliable and simple to use.  It can analyze over 62 elements.  It also measures the concentration of metals in the sample.
  • 4. HISTORY: The first atomic absorption spectrometer was built by CSIRO scientist Alan Walsh in 1954. Shown in the picture Alan Walsh(left), with a spectrometer.
  • 5. Elements detectable by atomic absorption are highlighted in pink in this periodic table
  • 6. TYPES OF ATOMIC SPECTRA 1) ATOMIC EMISSION SPECTRA:
  • 9. COMPARISON ATOMIC EMISSION SPECTROSCOPY • Examines the wavelengths of photons emitted by atoms or molecules during their transition from an excited state to a lower energy state. • Each element emits a characteristic set of discrete wavelengths. • By observing these wavelengths the elemental composition of the sample can be determined. ATOMIC ABSORPTION SPECTROSCPY • Measures the loss of electromagnetic energy after it illuminates the sample under study. • The energy in certain amount is absorbed during transition to the higher level. • The amount of energy absorbed gives estimate of the concentration of the analyte in the sample.
  • 10.  The technique uses basically the principle that free atoms (gas) generated in an atomizer can absorb radiation at specific frequency.  Atomic-absorption spectroscopy quantifies the absorption of ground state atoms in the gaseous state .  The atoms absorb ultraviolet or visible light and make transitions to higher electronic energy levels. The analyte concentration is determined from the amount of absorption.
  • 11. THEORY OF ATOMIC ABSORPTION SPECTROSCOPY  Atomic absorption spectroscopy is a method of elemental analysis.  When a solution containing the metallic species is introduced into a flame, the vapours of metallic species will be obtained. Some of the metal atoms may be raised to an energy level sufficiently high to emit the characteristic radiation of the metal during their return but a large percentage of metal will remain in the non-emitting ground state. These ground state elements are receptive of light radiation of their own specific wavelength. Thus when a light of this wavelength is allowed to pass through a flame having atoms of metallic species, part of light is absorbed and the absorption is directly propotional to the density in the flame.  It is particularly useful for determining trace metal in liquids and is almost independent of molecular form of the metal in the sample.  The method is very sensitive and can detect the different metals in concentration as low as and one frequently lower than 1 ppm.  A disadvantage of the method is that only one element can be determined at a time.  This method has limited use in quantitative analysis.
  • 12. THEORY OF ATOMIC ABSORPTION SPECTROSCOPY  .
  • 13.  The total amount of light absorbed may be given mathematically by the following expressions: Total number of light absorbed = πe2/mc Nf Where, e= is the charge on the electron of mass m= mass of electron c= is the speed of light N= is the total number of atoms that can absorb at frequency in the light path v= frequency f= is the oscillator strength or ability of each atom to absorb at frequency π= is constant The above equation can be written as: Total amount of light absorbed= Constant x N x f THEORY OF ATOMIC ABSORPTION SPECTROSCOPY
  • 20. Instrumentation Atomic absorption spectrophotometer based on the following components.  Source  Atomizer  Monochromator  Detector  Read out devise
  • 21. Radiation Source  The main radiation sources are used for the atomic absorption are following.  Hollow cathode lamp (HCL)  Electrode less discharge lamp (EDL)  Hollow cathode lamp :  It consist of tungsten anode and a cylindrical cathode sealed in a glass tube filled with neon or Argon at a pressure of 1-5 torr.  When a potential of 300V is applied, ionization of inert gas occur and a current of 5-20mA is generated as ions.
  • 22. Hollow Cathode lamp:  A portion of the sputtered metal atoms is in excited states and thus emit their characteristics radiation as they returns to the ground state.
  • 23. Electrode less Discharge Lamp  A typical lamp is constructed from a sealed quartz tube containing a few torr of an inert gas such as argon and a small quantity of the metal whose spectrum is of interest.  The lamp contain no electrode but instead is energized by an intense field of radiofrequency or microwave radiation.
  • 24. SOURCE MODULATION  Used to eliminate the interferences caused by emission of radiation by the flame. For these, output of the radiation source is modulated so that the intensity fluctuates at a constant frequency .  An easy way to eliminate the emission from the source is to interpose a circular metal disk or chopper in the beam between the source and the flame.
  • 25. Atomizers  The process of converting an analyte in solid, liquid or solution form to a free gaseous atom is called as the atomization and the instrument used for this purpose is called as the atomizers.  Two types of the atomizers are used.  A) flame atomizer  B) Electrothermal atomizer
  • 26. Flame atomizer  In flame atomizer, the sample is first converted into a fine mist consisting of small droplets of solution.  It is accomplished by using a nebulizer assembly.  The sample is aspirated into a spray chamber by passing a high pressure stream consisting of one or more combustion gases, part the end of a capillary tube immersed in the sample.  The impact of the sample with the glass impact head produces an aerosol mist.  The aerosol mist mixes with the combustion gases in the spray chamber before passing to flame which desolvates the aerosol mist to a dry aerosol of small solid particles.
  • 27.  Subsequently, flame thermal energy volatilizes the particles, producing a vapors consisting of molecular species, ionic species and free atoms.  Thermal energy in flame atomization is provided by the combustion of a fuel – oxidant mixture. FLAME ATOMIZER: • Flame is used to atomize the sample • Sample when heated is broken into its atoms PRINCIPLE: • High temperature of flame causes excitation • Electrons of the atomized sample are promoted to higher orbitals, by absorbing certain amount of energy QUANTITATIVE ANALYSIS: • The amount of energy absorbed is specific for a particular element (for electronic transition).
  • 28. SAMPLE NEBULIZER ASSEMBLY CONVERSION INTO FINE MIST & SMALL DROPLETS OF SOLUTION ASPIRATED INTO SPRAY CHAMBER (MIXING CHAMBER) AEROSOL MIXES WITH COMBUSTIO N GASES FLAME (ATOMIZATIO N OCCURS)
  • 29. Sample to be nebulized is taken (aspirated) via a capillary tube Nebulizer: sample+fuel + oxidant fine mist or aerosol
  • 30. Natural Gas Air 1700-1900 39-43 Natural Gas Oxygen 2700-2800 370-390 Hydrogen Air 2000-2100 300-440 Hydrogen Oxygen 2550-2700 900-1400 Acetylene Air 2100-2400 158-266 Acetylene Oxygen 3050-3150 1100-2480 Acetylene Nitrous Oxide 2600-2800 285
  • 32. Flame atomizers  Flame atomizers are of two types  Continuous  Discrete  Continuous: the sample is fed into atomizer at a constant rate. The spectral line is then constant with time.  Discrete: A measured quantity of the sample is introduced as a plug of liquid or solid. The spectral line is rises to a maximum and then decreases to zero.
  • 33. Electro thermal Atomizers  A typical electro thermal atomizer also known as graphite furnace, consisting of a cylindrical graphite tube approximately 1-3 cm in length and 3-8 mm in diameter.  The graphite tube is housed in an assembly that seals the end of the tube with optically transparent windows. The assembly also allows for the passage of continuous stream of inert gas, protecting the graphite tube from oxidation and removing the gaseous products produced during atomization. A power supply is used to pass a current through the graphite tube, resulting in resistive heating.
  • 34. Construction of electro thermal atomizers  . Graphite tube Enclosed water cooled housing Transparent windows Inert purge gas control Electrical contact
  • 35. Electro thermal Atomizers  Samples between 5 and 50 micro liter are injected into the graphite tube through a small diameter hole located at the top of the tube.  Atomization takes place in three stages: Atomization of sample 1.Drying 2. Ashing 3.Atomizatio
  • 36. Electro thermal Atomizers  In the first stage sample is dried by using a current that raises the temperature of the graphite tube to about 110◦C and desolvation leaves the sample as a solid residue.  In the second stage, which is called as the ashing, the temperature is increased to about 350-1200 ◦C. At this temperature the sample is converted into the carbon dioxide and water and volatile inorganic material are vaporized. These gases are removed by the inert gas flow.  In the final stage, the sample is atomized by rapidly increasing the temperature to 2000-3000 ◦C.  Three stages are completed in 45-90 sec.  The analyte concentration in the resulting vapor phase may be as much as 1000 times greater than that produced by flame atomization.
  • 37. Instrumentation (continues)  Monochromators:  Monochromators are used to isolate the narrow band width of wavelength that are absorbed by the metals.  Detectors:  the photomultiplier is used to detect the light absorbed by the analyte. It is same as described in UV/ mass spectrometer.
  • 38. Working of atomic absorption spectrophotometer  Single beam atomic absorption spectrophotometer: Single beam measurements are depended upon the varying intensity of a single single beam of light having a single optical path. That is why called as single beam AA spectrophotometer. It consist of hollow cathode lamp, a chopper, atomizer and a simple grating spectrophotometer with photomultiplier detector. Double beam atomic absorption spectrophotometer: the beam from the hollow cathode source is split by mirror chopper so that one half passed through the flame and the other half around it. The two beams are then recombined by a half silver mirror and passed into grating monochromator. The photomultiplier tube serves as the detector
  • 40. Single / double beam spectrophotometer 4343 Atomic absorption spectrophotometer I nstrumentationI nstrumentation
  • 41. SAMPLE PREPARATION T the preparation of the sample solution for a solid material is most time consuming step of process of analysis in an atomic absorption spectroscopy. It involves following steps; Weighing of sample Dissolution in appropriate solvent or digestion using different techniques Dilution of sample if necessary
  • 42.  Pharmaceutical  Biological  Biochemical For detection of purity and consistency of these trace metals Also for quantitative determination of metals mainly in solid sample as mineral, ores and alloys Apllication of atomic absorption spectroscopy
  • 43. • Magnesium in cast iron • Silver, Zinc, Copper and Lead in Cadmium metal • Method of multiple standard addition • A plot of absorbance against the amount of standard can be used to determine the amount of copper in a sample.
  • 44.  Determination of trace metal in a silicon foam cavity wound dressing  Zinc in Zinc insulin suspension and tetracosactrin Zinc injection  Copper and Iron in ascorbic acid  Aluminum in albumin solution and Ca, Mg, Mercury  Zinc in water used for diluting haemodialysis solution
  • 45. •For the analysis of pharmaceutically or therapeutically essential component of formulation, such as Zinc in Zinc-insulin, minerals in multivitamin- mineral preparation and Ca, Mg, Al in antacids. •To establish concentration limits where the metal is regarded as an impurity.
  • 46. •Mining industries •Petroleum industries •Determination of metallic elements in food industry like Copper, Zinc and Nickel in vegetable oil and copper in beer.