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ATOMIC ABSORPTION 
AND MASS 
SPECTROSOPY 
G.Vanitha
ATOMIC ABSORPTION SPECTROSOPY
INTRODUTION 
Atomic Absorption Spectroscopy is a very 
common technique for detecting metals and 
metalloids 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 spectroscopy was built 
by CSIRO scientist Alan Walsh in 1954. 
The first commercial atomic absorption 
spectroscopy was introduced in 1959.
Elements detectable by atomic absorption are highlighted in pink 
in this periodic table.
PRINCIPLE 
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. 
Concentration measurements are usually determined from a 
working curve after calibrating the instrument with 
standards of known concentration.
INSTRUMENTATION
LIGHT SOURCE 
Hollow Cathode Lamp are the most common radiation 
source in AAS. 
It contains a tungsten anode and a hollow cylindrical 
cathode. 
These are sealed in a glass tube filled with an inert gas 
(neon or argon ) . 
Each element has its 
own unique lamp which 
must be used for that 
analysis .
Hollow Cathode Lamp for 
Aluminum (Al)
NEBULIZER 
Suck up liquid samples at controlled rate. 
Create a fine aerosol spray for introduction into 
flame. 
Mix the aerosol and fuel and oxidant thoroughly 
for introduction into flame.
ATOMIZER 
Elements to be analysed needs to in atomic state. 
Atomization is separation of particles into 
individual molecules and breaking molecules into 
atoms. This is done by exposing the analyte to high 
temperature in a flame or graphite furnace. 
Sample Atomization Technique 
Flame 
Atomization 
Electro thermal 
Atomization 
Hydride 
Atomization 
Cold-Vapor 
Atomization
Flame Atomization 
Nebulizer suck up liquid samples at controlled 
rate. 
Create a fine aerosol spray for introduction into 
flame. 
Mix the aerosol and oxidant thoroughly 
for introduction into flame. 
An aerosol is a colloid of fine solid particles or 
liquid droplets, in air or another gas.
Flame Atomization 
sample mist 
Solid/gas 
aerosol 
Gaseous 
molecules 
Atom 
s 
nebulization desolvation volatilization 
dissociation
Disadvantages of Flame 
Atomization 
Only 5-15% of the nebulized sample reaches the 
flame. 
A minimum sample volume of 0.5-1.0 ml is 
needed to give a reliable reading. 
Samples which are viscous require dilution with 
a solvent.
Electro Thermal Atomization 
Uses a graphite coated furnace to vaporize the 
sample. 
samples are deposited in a small graphite coated 
tube which can then heated to vaporize and 
atomize the analyte. 
The graphite tubes are heated using a high 
current power supply.
Advantages 
Small sample size 
Very little or no sample preparation is needed 
Sensitivity is enhanced 
Direct analysis of solid samples 
Disadvantages 
Analyte may be lost at the ashing stage 
The sample may not be completely atomized 
Analytical range is relatively low
MONOCHROMATOR 
This is very important part in an AAS. 
It is used to separate out all of the thousands of 
lines. 
A monochromator is used to select the specific 
wavelength of light which is absorbed by the 
sample, and to exclude other wavelengths. 
The selection of the specific light allows the 
determination of the selected element in the 
presence of others.
DETECTOR 
The light selected by the monochromator is 
directed onto a detector that is typically a 
photomultiplier tube, whose function is convert 
the light signal into an electrical signal 
proportional to the intensity. 
The processing of electrical signal is fulfilled by 
a signal amplifier. 
The signal could be displayed for readout, or 
further fed into a data station for printout by the 
requested format
Calibration Curve 
A calibration curve is used to determine the 
unknown concentration of an element in a 
solution. 
The instrument is calibrated using several 
solutions of known concentrations. 
The absorbance of each known solution is 
measured and then a calibration curve of 
concentration vs absorbance is plotted. 
The sample solution is fed into the instrument, and 
the absorbance of the element in this solution is 
measured. 
The unknown concentration of the element is then 
calculated from the calibration curve
Applications 
Determination of even small amounts of metals 
(lead, mercury, calcium, magnesium, etc.) 
Environmental studies: drinking water, ocean 
water, soil. 
Food industry. 
Pharmaceutical industry. 
Presence of metals as an impurity or in alloys 
could be done easily 
Level of metals could be detected in tissue 
samples like Aluminum in blood and Copper in 
brain tissues
MASS SPECTROSOPY
Introduction 
Mass Spectroscopic method is one of the most popular 
molecular analysis methods today. 
Mass Spectroscopy is an analytical spectroscopic tool 
primarily concerned with the separation of molecular 
(and atomic) species according to their mass. 
It is a microanalytical technique requiring only a few 
nanomoles of the sample to obtain characteristic 
information pertaining to the structure and molecular 
weight of analyte. 
It is not concerned with non- destructive interaction 
between molecules and electromagnetic radiation.
Principle 
Mass spectroscopy is the most accurate method 
for determining the molecular mass of the 
compound and its elemental composition. 
In this technique, molecules are bombarded with 
a beam of energetic electrons. 
The molecules are ionised and broken up into 
many fragments, some of which are positive 
ions.
Mass spectra is used in two general ways: 
To prove the identity of two compounds. 
To establish the structure of a new a compound. 
The mass spectrum of a compound helps to 
establish the structure of a new compound in 
several different ways: 
It can give the exact molecular mass. 
It can give a molecular formula or it can reveal 
the presence of certain structural units in a 
molecule.
TYPICAL DIAGRAM OF MS
METHODOLOGY 
Gaseous or liquid substances that vaporize under 
vacuum are admitted to a mass spectroscopy. 
The gas is diluted by being partially pumped down to 
a low pressure (molecular flow range) in a vacuum 
chamber and ionized through electron bombardment. 
The ions thus generated are introduced to a mass 
filter and separated on the basis of their charge to 
mass ratio.
IONISATION 
The atom is ionised by knocking one or more 
electrons off to give a positive ion. (Mass 
spectrometers always work with positive ions). 
The particles in the sample (atoms or molecules) are 
bombarded with a stream of electrons to knock one or 
more electrons out of the sample particles to make 
positive ions.
ACCELERATION 
The ions are accelerated so that they all have the same 
kinetic energy.
The positive ions are repelled away from the 
positive ionization chamber and pass through three 
slits with voltage in the decreasing order. 
The middle slit carries some intermediate voltage 
and the final at ‘0’ volts. 
All the ions are accelerated into a finely focused 
beam.
DEFLECTION 
The ions are then deflected by a magnetic field 
according to their masses. The lighter they are, the more 
they are deflected. 
The amount of deflection also depends on the number 
of positive charges on the ion -The more the ion is 
charged, the more it gets deflected.
Different ions are deflected by the magnetic 
field by different amounts. The amount of 
deflection depends on: 
The mass of the ion: Lighter ions are deflected 
more than heavier ones. 
The charge on the ion: Ions with 2 (or more) 
positive charges are deflected more than ones 
with only 1 positive charge.
DETECTION 
The beam of ions passing through the machine is 
detected electrically. 
When an ion hits the metal box, its charge is 
neutralized by an electron jumping from the metal on 
to the ion.
That leaves a space among the electrons in the 
metal, and the electrons in the wire shuffle along 
to fill it. 
A flow of electrons in the wire is detected as an 
electric current which can be amplified and 
recorded. The more ions arriving, the greater the 
current.
APPLICATIONS 
Pharmaceutical analysis 
Bioavailability studies 
Drug metabolism studies, pharmacokinetics 
Characterization of potential drugs 
Drug degradation product analysis 
Screening of drug candidates 
Identifying drug targets 
Biomolecule characterization 
Proteins and peptides 
Oligonucleotides
Environmental analysis 
Pesticides on foods 
Soil and groundwater contamination 
Forensic analysis/clinical
Reference 
 Mass Spectroscopy Amruta S. Sambarekar 
 Mass Spectroscopy - An Overview Dr. M. Vairamani, 
IPFT 
 http://www.uga.edu/~sisbl/aaspec.html 
 http://www.clu-in.org/char/technologies/graphite.cfm 
 B. Welz, M. Sperling, Atomic Absorption 
Spectrometry, Wiley-VCH, Weinheim, Germany, ISBN 
3-527-28571-7. 
 Skoog, Douglas (2007). Principles of Instrumental 
Analysis (6th ed.). Canada: Thomson Brooks/Cole. 
ISBN 0-495-01201-7.
thank you

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atomic absorption spectroscopy and mass spectroscopy

  • 1. ATOMIC ABSORPTION AND MASS SPECTROSOPY G.Vanitha
  • 3. INTRODUTION Atomic Absorption Spectroscopy is a very common technique for detecting metals and metalloids 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 spectroscopy was built by CSIRO scientist Alan Walsh in 1954. The first commercial atomic absorption spectroscopy was introduced in 1959.
  • 5. Elements detectable by atomic absorption are highlighted in pink in this periodic table.
  • 6. PRINCIPLE 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. Concentration measurements are usually determined from a working curve after calibrating the instrument with standards of known concentration.
  • 8.
  • 9. LIGHT SOURCE Hollow Cathode Lamp are the most common radiation source in AAS. It contains a tungsten anode and a hollow cylindrical cathode. These are sealed in a glass tube filled with an inert gas (neon or argon ) . Each element has its own unique lamp which must be used for that analysis .
  • 10. Hollow Cathode Lamp for Aluminum (Al)
  • 11. NEBULIZER Suck up liquid samples at controlled rate. Create a fine aerosol spray for introduction into flame. Mix the aerosol and fuel and oxidant thoroughly for introduction into flame.
  • 12. ATOMIZER Elements to be analysed needs to in atomic state. Atomization is separation of particles into individual molecules and breaking molecules into atoms. This is done by exposing the analyte to high temperature in a flame or graphite furnace. Sample Atomization Technique Flame Atomization Electro thermal Atomization Hydride Atomization Cold-Vapor Atomization
  • 13. Flame Atomization Nebulizer suck up liquid samples at controlled rate. Create a fine aerosol spray for introduction into flame. Mix the aerosol and oxidant thoroughly for introduction into flame. An aerosol is a colloid of fine solid particles or liquid droplets, in air or another gas.
  • 14. Flame Atomization sample mist Solid/gas aerosol Gaseous molecules Atom s nebulization desolvation volatilization dissociation
  • 15. Disadvantages of Flame Atomization Only 5-15% of the nebulized sample reaches the flame. A minimum sample volume of 0.5-1.0 ml is needed to give a reliable reading. Samples which are viscous require dilution with a solvent.
  • 16. Electro Thermal Atomization Uses a graphite coated furnace to vaporize the sample. samples are deposited in a small graphite coated tube which can then heated to vaporize and atomize the analyte. The graphite tubes are heated using a high current power supply.
  • 17. Advantages Small sample size Very little or no sample preparation is needed Sensitivity is enhanced Direct analysis of solid samples Disadvantages Analyte may be lost at the ashing stage The sample may not be completely atomized Analytical range is relatively low
  • 18. MONOCHROMATOR This is very important part in an AAS. It is used to separate out all of the thousands of lines. A monochromator is used to select the specific wavelength of light which is absorbed by the sample, and to exclude other wavelengths. The selection of the specific light allows the determination of the selected element in the presence of others.
  • 19. DETECTOR The light selected by the monochromator is directed onto a detector that is typically a photomultiplier tube, whose function is convert the light signal into an electrical signal proportional to the intensity. The processing of electrical signal is fulfilled by a signal amplifier. The signal could be displayed for readout, or further fed into a data station for printout by the requested format
  • 20. Calibration Curve A calibration curve is used to determine the unknown concentration of an element in a solution. The instrument is calibrated using several solutions of known concentrations. The absorbance of each known solution is measured and then a calibration curve of concentration vs absorbance is plotted. The sample solution is fed into the instrument, and the absorbance of the element in this solution is measured. The unknown concentration of the element is then calculated from the calibration curve
  • 21.
  • 22. Applications Determination of even small amounts of metals (lead, mercury, calcium, magnesium, etc.) Environmental studies: drinking water, ocean water, soil. Food industry. Pharmaceutical industry. Presence of metals as an impurity or in alloys could be done easily Level of metals could be detected in tissue samples like Aluminum in blood and Copper in brain tissues
  • 24. Introduction Mass Spectroscopic method is one of the most popular molecular analysis methods today. Mass Spectroscopy is an analytical spectroscopic tool primarily concerned with the separation of molecular (and atomic) species according to their mass. It is a microanalytical technique requiring only a few nanomoles of the sample to obtain characteristic information pertaining to the structure and molecular weight of analyte. It is not concerned with non- destructive interaction between molecules and electromagnetic radiation.
  • 25. Principle Mass spectroscopy is the most accurate method for determining the molecular mass of the compound and its elemental composition. In this technique, molecules are bombarded with a beam of energetic electrons. The molecules are ionised and broken up into many fragments, some of which are positive ions.
  • 26. Mass spectra is used in two general ways: To prove the identity of two compounds. To establish the structure of a new a compound. The mass spectrum of a compound helps to establish the structure of a new compound in several different ways: It can give the exact molecular mass. It can give a molecular formula or it can reveal the presence of certain structural units in a molecule.
  • 27.
  • 29. METHODOLOGY Gaseous or liquid substances that vaporize under vacuum are admitted to a mass spectroscopy. The gas is diluted by being partially pumped down to a low pressure (molecular flow range) in a vacuum chamber and ionized through electron bombardment. The ions thus generated are introduced to a mass filter and separated on the basis of their charge to mass ratio.
  • 30. IONISATION The atom is ionised by knocking one or more electrons off to give a positive ion. (Mass spectrometers always work with positive ions). The particles in the sample (atoms or molecules) are bombarded with a stream of electrons to knock one or more electrons out of the sample particles to make positive ions.
  • 31. ACCELERATION The ions are accelerated so that they all have the same kinetic energy.
  • 32. The positive ions are repelled away from the positive ionization chamber and pass through three slits with voltage in the decreasing order. The middle slit carries some intermediate voltage and the final at ‘0’ volts. All the ions are accelerated into a finely focused beam.
  • 33. DEFLECTION The ions are then deflected by a magnetic field according to their masses. The lighter they are, the more they are deflected. The amount of deflection also depends on the number of positive charges on the ion -The more the ion is charged, the more it gets deflected.
  • 34. Different ions are deflected by the magnetic field by different amounts. The amount of deflection depends on: The mass of the ion: Lighter ions are deflected more than heavier ones. The charge on the ion: Ions with 2 (or more) positive charges are deflected more than ones with only 1 positive charge.
  • 35. DETECTION The beam of ions passing through the machine is detected electrically. When an ion hits the metal box, its charge is neutralized by an electron jumping from the metal on to the ion.
  • 36. That leaves a space among the electrons in the metal, and the electrons in the wire shuffle along to fill it. A flow of electrons in the wire is detected as an electric current which can be amplified and recorded. The more ions arriving, the greater the current.
  • 37.
  • 38. APPLICATIONS Pharmaceutical analysis Bioavailability studies Drug metabolism studies, pharmacokinetics Characterization of potential drugs Drug degradation product analysis Screening of drug candidates Identifying drug targets Biomolecule characterization Proteins and peptides Oligonucleotides
  • 39. Environmental analysis Pesticides on foods Soil and groundwater contamination Forensic analysis/clinical
  • 40. Reference  Mass Spectroscopy Amruta S. Sambarekar  Mass Spectroscopy - An Overview Dr. M. Vairamani, IPFT  http://www.uga.edu/~sisbl/aaspec.html  http://www.clu-in.org/char/technologies/graphite.cfm  B. Welz, M. Sperling, Atomic Absorption Spectrometry, Wiley-VCH, Weinheim, Germany, ISBN 3-527-28571-7.  Skoog, Douglas (2007). Principles of Instrumental Analysis (6th ed.). Canada: Thomson Brooks/Cole. ISBN 0-495-01201-7.