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ATOMIC
SPECROSCOPY (AS)
Atomic Absorption Spectroscopy
Flame Atomic Emission Spectroscopy
ICP Atomic Emission Spectroscopy
1
BASIC PRINCIPLE
ATOMIC ABSORPTION SPECTROSCOPY (AAS) is an
analytical technique that measures the concentrations of
elements. It makes use of the absorption of light
by these elements in order to measure their
concentration .
- 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.
- Atomic absorption is a very common technique for detecting
metals and metalloids in environmental samples.
Elements detectable by atomic absorption are highlighted in pink in this periodic table
The Atomic Absorption Spectrometer
• Atomic absorption spectrometers have 4 principal components
1 - A light source ( usually a hollow cathode lamp )
2 – An atom cell ( atomizer )
3 - A monochromator
4 - A detector , and read out device .
Schematic Diagram of an Atomic
Absorption Spectrometer
Light source
(hollow cathode Lamp )
atomizer
monochromator
Detector and
readout device
Atomic Absorption Spectrophotometer
1 – Light Source
•The light source is usually a hollow cathode lamp of
the element that is being measured . It contains a
tungsten anode and a hollow cylindrical cathode
made of the element to be determined. 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
cathode
Anode
Quartz window
Pyrex body
Anode
Cathode
How it works
Applying a potential difference between the anode
and the cathode leads to the ionization of some gas
atoms .
These gaseous ions bombard the cathode and eject
metal atoms from the cathode in a process called
sputtering. Some sputtered atoms are in excited
states and emit radiation characteristic of the metal
as they fall back to the ground state .
Scheme of a hollow cathode lamp
The shape of the cathode which is hollow
cylindrical concentrates the emitted radiation into a
beam which passes through a quartz window all the
way to the vaporized sample.
Since atoms of different elements absorb
characteristic wavelengths of light. Analyzing a
sample to see if it contains a particular element
means using light from that element .
For example with lead, a lamp containing lead
emits light from excited lead atoms that produce
the right mix of wavelengths to be absorbed by any
lead atoms from the sample .
A beam of the electromagnetic radiation emitted
from excited lead atoms is passed through the
vaporized sample. Some of the radiation is
absorbed by the lead atoms in the sample. The
greater the number of atoms there is in the vapor ,
the more radiation is absorbed .
2 – Atomizer
Elements to be analyzed needs to be in
atomic sate
Atomization is separation of particles into
individual molecules and breaking molecules
into atoms .This is done by exposing the
analyte to high temperatures in a flame or
graphite furnace .
The role of the atom cell is to primarily dissolvate a
liquid sample and then the solid particles are
vaporized into their free gaseous ground state form
. In this form atoms will be available to absorb
radiation emitted from the light source and thus
generate a measurable signal proportional to
concentration .
There are two types of atomization : Flame and
Graphite furnace atomization .
•
Flame
• Flame AA can only analyze solutions , where
it uses a slot type burner to increase the
path length, and therefore to increase the total
absorbance .
Sample solutions are usually
introduced into a nebuliser by being sucked up a
capillary tube .In the nebuliser the sample is
dispersed into tiny droplets , which can be
readily broken down in the flame.
FLAME ATOMIZERS
 Used in all Atomic Spectroscopic techniques
 Converts analyte into free atoms in the form of vapor phase
free atoms
 Heat is required
 Routes for sample introduction
Various flame atomization techniques
Types of Flames Used in Atomic Spectroscopy
Processes that take place in flame
Effect of flame temperature on excited state population
# atoms in
Ground state
# atoms in
Excited state
Energy
difference
Boltzmann
constant
Temperature
Statistical
factor
For Zn: N*/No = 10-15%
• Thus 99.998% of Na atoms are in the ground state
• Atomic emission uses Excited atoms
• Atomic absorption uses Ground state atoms
Effect of flame temperature on excited state population
ATOMIZATION DEVICES
ATOMIZATION :
A process of forming free atoms by heat
Atomizers are devices that carry out atomization:
Continuous
Non-continuous
Continuous: (Constant temperature with time)
Flame
Plasma
Non-Continuous: (temperature varies with time)
Electrothermal
Spark discharge
SAMPLE INTRODUCTION SYSTEMS
In continuous atomizers sample is constantly introduced in
form of droplets, dry aerosol, vapor
Nebulizer : A device for converting the solution into fine
spray or droplets
Continuous sample introduction is used with continuous
nebulizers in which a steady state atomic population is
produced. Sample is introduced in fixed or discrete amounts.
Discontinuous samplers are used with continuous atomizers
1- Discrete samples are introduced into atomizers in many
ways:
Electrothermal atomizers
a syringe is used
a transient signal is produced as temperature changes
with time and sample is consumed
2- Indirect insertion (Probe)
sample is introduced into a probe (carbon rod) and
mechanically moved into the atomization region
vapor cloud is transient because sample introduced is
limited
3-Flow Injection
The analyte is introduced into the carrier stream into a
nebulizer as mist
4-Hydride Generation
the volatile sample is stripped from the analyte
solution and carried out by a gas into the atomizer.
This strip is followed by chemically converting the
analyte to hydride vapor form.
5- With Arc Spark
Solids are employed
6- Laser Microbe Technique
A beam of laser is directed onto a small solid sample, gets
vaporized, atomized by relative heating. Either sample is
probed by encoding system or vapor produced is swept
into a second absorption or fluorescence
 Nebulization gas is always compressed, usually acts as the
oxidant; it is oxygen (O2) in flame and argon (Ar) in plasma
 Nebulization chambers produce smaller droplets and remove
or drain larger droplets called aerosol modifiers
 Aspiration rate is proportional to compressed gas pressure.
The pressure drops through capillary, here 1/4 capillary
diameters are recommended. This is inversely proportional to
viscocity of the solution
 Peristaltic and/or syringe pumps could be used
 Oxidant and fuel are usually brought into the nebulization
chamber through a separate port. They mix and pass the burner
head called premixed burner system.
 Add organic solvents to reduce the size of the drop
The Atomic Absorption Spectrometer
Sample Introduction System
Nebuliser
Capillary
Solution
• The fine mist of droplets is mixed with fuel ( acetylene ) , and
oxidant ( nitrous oxide) and burned.
The flame temperature is important because it influences the
distribution of atoms. It can be manipulated by oxidant and
fuel ratio.
Graphite Furnace
• The graphite furnace has several advantages over a flame. First it accept
solutions, slurries, or solid samples.
• Second it is a much more efficient atomizer than a flame and it can
directly accept very small absolute quantities of sample. It also provides
a reducing environment for easily oxidized elements. Samples are placed
directly in the graphite furnace and the furnace is electrically heated in
several steps to dry the sample, ash organic matter, and vaporize the
analyte atoms.
• It accommodates smaller samples but it’s a difficult operation, because
the high energy that is provided to atomize the sample particles into
ground state atoms might excite the atomized particles into a higher
energy level and thus lowering the precision .
3- Monochromators
This is a very important part in an AA spectrometer. It is
used to separate out all of the thousands of lines. Without a
good monochromator, detection limits are severely
compromised.
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.
4 - Detector and
Read out Device
The light selected by the monochromator is
directed onto a detector that is typically a
photomultiplier tube , whose function is to convert
the light signal into an electrical signal proportional
to the light 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
Calibration Curve
A 1.0 -
b 0.9 -
S 0.8 - .
o 0.7 - .
r 0.6 - .
b 0.5 - . .
a 0.4 - .
n 0.3 - .
c 0.2 -
e 0.1 -
10 20 30 40 50 60 70 80 90 100
Concentration ( g/ml )
Determining concentration from
Calibration Curve
A 1.0 - absorbance measured
b 0.9 -
S 0.8 - .
o 0.7 - .
r 0.6 - .
b 0.5 - . .
a 0.4 - .
n 0.3 - . concentration calculated
c 0.2 -
e 0.1 -
10 20 30 40 50 60 70 80 90 100
Concentration ( mg/l )
Interferences
The concentration of the analyte element is
considered to be proportional to the ground state
atom population in the flame ,any factor that
affects the ground state atom population can be
classified as an interference .
Factors that may affect the ability of the instrument
to read this parameter can also be classified as an
interference .
The different interferences that are encountered in atomic absorption
spectroscopy are :
- Absorption of Source Radiation : Element other than the one of
interest may absorb the wavelength being used.
- Ionization Interference : the formation of ions rather than atoms
causes lower absorption of radiation .This problem is overcome by
adding ionization suppressors.
- Self Absorption : the atoms of the same kind that are absorbing
radiation will absorb more at the center of the line than at the wings
,and thus resulting in the change of shape of the line as well as its
intensity .
- Back ground Absorption of Source Radiation :
This is caused by the presence of a particle from
incomplete atomization .This problem is overcome by
increasing the flame temperature .
- Transport Interference :
Rate of aspiration, nebulization, or transport of the
sample ( e g viscosity, surface tension, vapor
pressure , and density ) .
2
Atomic Emission
Spectroscopy
Atomic emission spectroscopy is also an analytical
technique that is used to measure the
concentrations of elements in samples .
It uses quantitative measurement of the emission
from excited atoms to determine analyte
concentration .
The analyte atoms are promoted to a higher energy level
by the sufficient energy that is provided by the high
temperature of the atomization sources .
The excited atoms decay back to lower levels by emitting
light . Emissions are passed through monochromators or
filters prior to detection by photomultiplier tubes.
The instrumentation of atomic emission spectroscopy is the same as
that of atomic absorption ,but without the presence of a radiation
source .
In atomic Emission the sample is atomized and the analyte atoms are
excited to higher energy levels all in the atomizer .
Schematic Diagram of an Atomic
Emission spectrometer
The source of energy in Atomic Emission could be a flame like
the one used in atomic absorption ,or an inductively coupled
plasma ( ICP ) .
- The flame ( 1700 – 3150 oC ) is most useful for
elements with relatively low excitation energies like
sodium potassium and calcium .
- The ICP ( 6000 – 8000 oC) has a very high
temperature and is useful for elements of high
excitation energies .
INDUCTIVELY COUPLED PLASMA
(ICP)

Plasma is a type of electrical discharge

Plasma is any type of matter that contains an appreciable
amount of less than 1% of electrons and +ve ions in equal
numbers + atoms + neutral molecules
 Plasma has 2 characteristics:
i- can conduct electricity
II- affected by magnetic fields
 Plasma is highly energetic ionized gases usually inert,
recently reactive oxygen is used.
 ICP is the state-of-the-art plasma
 Other plasmas include direct current plasma (DCP) and
microwave induced plasma (MIP)
ADVANTAGES OF THE ICP

High degree of selectivity

Ability to overcome depressive interference effects

Capable of exciting several elements not excitable by
ordinary flames

Higher sensitive than Flame Photometry

Simpler to operate than Arc Spark methods

Higher degree of sensitivity than Arc Spark

Lacks electrodes which gives freedom from contamination
and extremely low background.
GENERAL CHARACTERISTICS OF THE ICP
Up to 70 elements can be analyzed at concentrations below 1
ppm
(Fig 1))
THE ICP DISCHARGE
(Fig 2)

The argon gas is directed through a torch consists of 3
concentric tubes made of quartz

A copper coil called the Load Coil surrounds the top
end of the torch and connected to a Radio Frequency
Generator (RF)

When RF power (700 – 1500 Watts) is applied to the
load coil, an alternating current moves back and forth
within the coil or oscillates at a rate corresponding to the
frequency of the generator (27 – 40 MHz). This RF
oscillation causes the RF electric and magnetic fields to
be set up in the area at the top of the torch.

With Argon gas being swirled through the torch, a spark is
applied to the gas causing some electrons to strip out from their
Argon atoms

These electrons are then caught up in the magnetic field and
accelerated by them.

Adding energy to the electrons by the use of the coil in this
manner is called “Inductively Coupling”

These high-energy electrons in turn collide with other Argon
atoms, stripping off still more electrons

This collisional ionization of Argon continues in a chain
reaction thus breaking down the gas into a Plasma consisting of
Argon atoms, electrons, and Argon ions know as “ICP”
discharge

This ICP discharge is sustained

This ICP discharge appears as intense, brilliant, white and
tear-drop shaped (Fig 3)

(Fig 4)
Explains what happens to aerosol samples introduced into the
plasma
(Fig 5)
Explains advantage of the plasma with repect to stability,
high temperature suurounding the sample for long time
(2 milliseconds) thus resulting into lack of matrix
interferences.
General Information

Used for Qualitative Analysis

Used for Quantitative Analysis

Detection limit is in ppb range

Not possible to determine: H, N, O, C or Ar in trace levels
as they are used in solvents and plasma

Not possible to determine F, Cl and noble gases at trace
levels as they require high excitation energy

Not used for determining radioactive elements

Upper limit for linear calibration is 10000 – 1000000 times
the detection limits for a particular emission line

Only 2 standard solutions are required for the calibration
plot as linearity is infinite

ICP has a multi-elemental capability for analysis
INSTRUMENTATION
Similar to an atomic absorption spectrometer ,the
monochromator is simply a wavelength selector
that separates all different wave lengths and select
the desired one .
The selected wave length is passed on to a detector
that converts the light signal into an electrical signal
.
Comparison Between Atomic Absorption
and Emission Spectroscopy
Absorption
- Measure trace metal
concentrations in
complex matrices .
- Atomic absorption
depends upon the
number of ground state
atoms .
Emission
- Measure trace metal
concentrations in
complex matrices .
- Atomic emission depends
upon the number of
excited atoms .
- It measures the
radiation absorbed by
the ground state atoms.
- Presence of a light
source ( HCL ) .
- The temperature in
the atomizer is adjusted to
atomize the analyte
atoms in the ground
state only.
- It measures the
radiation emitted by the
excited atoms .
- Absence of the light
source .
- The temperature in the
atomizer is big enough to
atomize the analyte
atoms and excite them to
a higher energy level.
3
AAS APPLICATIONS
The are many applications for atomic absorption:
- Clinical analysis : Analyzing metals in biological fluids such as blood
and urine.
- Environmental analysis : Monitoring our
environment – e g finding out the levels of various elements in rivers,
seawater, drinking water, air, and petrol.
- Pharmaceuticals. In some pharmaceutical
manufacturing processes, minute quantities of a
catalyst used in the process (usually a metal) are
sometimes present in the final product. By using
AAS the amount of catalyst present can be
determined.
- Industry : Many raw materials are examined and
AAS is widely used to check that the major elements
are present and that toxic impurities are lower than
specified – e g in concrete, where calcium is a major
constituent, the lead level should be low because it is
toxic.
- Mining: By using AAS the amount of metals such as gold in rocks can
be determined to see whether it is worth mining the rocks to extract
the gold .
- Trace elements in food analysis
- Trace element analysis of cosmetics
- Trace element analysis of hair

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1606732404-atomic-absorption-emission-2.ppt

  • 1. ATOMIC SPECROSCOPY (AS) Atomic Absorption Spectroscopy Flame Atomic Emission Spectroscopy ICP Atomic Emission Spectroscopy
  • 2. 1 BASIC PRINCIPLE ATOMIC ABSORPTION SPECTROSCOPY (AAS) is an analytical technique that measures the concentrations of elements. It makes use of the absorption of light by these elements in order to measure their concentration .
  • 3. - 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.
  • 4. - Concentration measurements are usually determined from a working curve after calibrating the instrument with standards of known concentration. - Atomic absorption is a very common technique for detecting metals and metalloids in environmental samples.
  • 5. Elements detectable by atomic absorption are highlighted in pink in this periodic table
  • 6. The Atomic Absorption Spectrometer • Atomic absorption spectrometers have 4 principal components 1 - A light source ( usually a hollow cathode lamp ) 2 – An atom cell ( atomizer ) 3 - A monochromator 4 - A detector , and read out device .
  • 7. Schematic Diagram of an Atomic Absorption Spectrometer Light source (hollow cathode Lamp ) atomizer monochromator Detector and readout device
  • 9. 1 – Light Source •The light source is usually a hollow cathode lamp of the element that is being measured . It contains a tungsten anode and a hollow cylindrical cathode made of the element to be determined. 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 cathode Anode Quartz window Pyrex body Anode Cathode
  • 11. How it works Applying a potential difference between the anode and the cathode leads to the ionization of some gas atoms . These gaseous ions bombard the cathode and eject metal atoms from the cathode in a process called sputtering. Some sputtered atoms are in excited states and emit radiation characteristic of the metal as they fall back to the ground state .
  • 12. Scheme of a hollow cathode lamp
  • 13. The shape of the cathode which is hollow cylindrical concentrates the emitted radiation into a beam which passes through a quartz window all the way to the vaporized sample. Since atoms of different elements absorb characteristic wavelengths of light. Analyzing a sample to see if it contains a particular element means using light from that element .
  • 14. For example with lead, a lamp containing lead emits light from excited lead atoms that produce the right mix of wavelengths to be absorbed by any lead atoms from the sample . A beam of the electromagnetic radiation emitted from excited lead atoms is passed through the vaporized sample. Some of the radiation is absorbed by the lead atoms in the sample. The greater the number of atoms there is in the vapor , the more radiation is absorbed .
  • 15. 2 – Atomizer Elements to be analyzed needs to be in atomic sate Atomization is separation of particles into individual molecules and breaking molecules into atoms .This is done by exposing the analyte to high temperatures in a flame or graphite furnace .
  • 16. The role of the atom cell is to primarily dissolvate a liquid sample and then the solid particles are vaporized into their free gaseous ground state form . In this form atoms will be available to absorb radiation emitted from the light source and thus generate a measurable signal proportional to concentration . There are two types of atomization : Flame and Graphite furnace atomization .
  • 17.
  • 18. Flame • Flame AA can only analyze solutions , where it uses a slot type burner to increase the path length, and therefore to increase the total absorbance . Sample solutions are usually introduced into a nebuliser by being sucked up a capillary tube .In the nebuliser the sample is dispersed into tiny droplets , which can be readily broken down in the flame.
  • 19. FLAME ATOMIZERS  Used in all Atomic Spectroscopic techniques  Converts analyte into free atoms in the form of vapor phase free atoms  Heat is required  Routes for sample introduction
  • 21. Types of Flames Used in Atomic Spectroscopy
  • 22. Processes that take place in flame
  • 23. Effect of flame temperature on excited state population # atoms in Ground state # atoms in Excited state Energy difference Boltzmann constant Temperature Statistical factor
  • 24. For Zn: N*/No = 10-15%
  • 25. • Thus 99.998% of Na atoms are in the ground state • Atomic emission uses Excited atoms • Atomic absorption uses Ground state atoms
  • 26. Effect of flame temperature on excited state population
  • 27.
  • 28. ATOMIZATION DEVICES ATOMIZATION : A process of forming free atoms by heat Atomizers are devices that carry out atomization: Continuous Non-continuous Continuous: (Constant temperature with time) Flame Plasma Non-Continuous: (temperature varies with time) Electrothermal Spark discharge
  • 29. SAMPLE INTRODUCTION SYSTEMS In continuous atomizers sample is constantly introduced in form of droplets, dry aerosol, vapor Nebulizer : A device for converting the solution into fine spray or droplets Continuous sample introduction is used with continuous nebulizers in which a steady state atomic population is produced. Sample is introduced in fixed or discrete amounts. Discontinuous samplers are used with continuous atomizers
  • 30. 1- Discrete samples are introduced into atomizers in many ways: Electrothermal atomizers a syringe is used a transient signal is produced as temperature changes with time and sample is consumed 2- Indirect insertion (Probe) sample is introduced into a probe (carbon rod) and mechanically moved into the atomization region vapor cloud is transient because sample introduced is limited
  • 31. 3-Flow Injection The analyte is introduced into the carrier stream into a nebulizer as mist 4-Hydride Generation the volatile sample is stripped from the analyte solution and carried out by a gas into the atomizer. This strip is followed by chemically converting the analyte to hydride vapor form.
  • 32. 5- With Arc Spark Solids are employed 6- Laser Microbe Technique A beam of laser is directed onto a small solid sample, gets vaporized, atomized by relative heating. Either sample is probed by encoding system or vapor produced is swept into a second absorption or fluorescence
  • 33.  Nebulization gas is always compressed, usually acts as the oxidant; it is oxygen (O2) in flame and argon (Ar) in plasma  Nebulization chambers produce smaller droplets and remove or drain larger droplets called aerosol modifiers  Aspiration rate is proportional to compressed gas pressure. The pressure drops through capillary, here 1/4 capillary diameters are recommended. This is inversely proportional to viscocity of the solution  Peristaltic and/or syringe pumps could be used
  • 34.  Oxidant and fuel are usually brought into the nebulization chamber through a separate port. They mix and pass the burner head called premixed burner system.  Add organic solvents to reduce the size of the drop
  • 35. The Atomic Absorption Spectrometer Sample Introduction System Nebuliser Capillary Solution
  • 36. • The fine mist of droplets is mixed with fuel ( acetylene ) , and oxidant ( nitrous oxide) and burned. The flame temperature is important because it influences the distribution of atoms. It can be manipulated by oxidant and fuel ratio.
  • 37. Graphite Furnace • The graphite furnace has several advantages over a flame. First it accept solutions, slurries, or solid samples. • Second it is a much more efficient atomizer than a flame and it can directly accept very small absolute quantities of sample. It also provides a reducing environment for easily oxidized elements. Samples are placed directly in the graphite furnace and the furnace is electrically heated in several steps to dry the sample, ash organic matter, and vaporize the analyte atoms. • It accommodates smaller samples but it’s a difficult operation, because the high energy that is provided to atomize the sample particles into ground state atoms might excite the atomized particles into a higher energy level and thus lowering the precision .
  • 38. 3- Monochromators This is a very important part in an AA spectrometer. It is used to separate out all of the thousands of lines. Without a good monochromator, detection limits are severely compromised. 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.
  • 39. 4 - Detector and Read out Device The light selected by the monochromator is directed onto a detector that is typically a photomultiplier tube , whose function is to convert the light signal into an electrical signal proportional to the light 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.
  • 40. 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
  • 41. Calibration Curve A 1.0 - b 0.9 - S 0.8 - . o 0.7 - . r 0.6 - . b 0.5 - . . a 0.4 - . n 0.3 - . c 0.2 - e 0.1 - 10 20 30 40 50 60 70 80 90 100 Concentration ( g/ml )
  • 42. Determining concentration from Calibration Curve A 1.0 - absorbance measured b 0.9 - S 0.8 - . o 0.7 - . r 0.6 - . b 0.5 - . . a 0.4 - . n 0.3 - . concentration calculated c 0.2 - e 0.1 - 10 20 30 40 50 60 70 80 90 100 Concentration ( mg/l )
  • 43. Interferences The concentration of the analyte element is considered to be proportional to the ground state atom population in the flame ,any factor that affects the ground state atom population can be classified as an interference . Factors that may affect the ability of the instrument to read this parameter can also be classified as an interference .
  • 44. The different interferences that are encountered in atomic absorption spectroscopy are : - Absorption of Source Radiation : Element other than the one of interest may absorb the wavelength being used. - Ionization Interference : the formation of ions rather than atoms causes lower absorption of radiation .This problem is overcome by adding ionization suppressors. - Self Absorption : the atoms of the same kind that are absorbing radiation will absorb more at the center of the line than at the wings ,and thus resulting in the change of shape of the line as well as its intensity .
  • 45. - Back ground Absorption of Source Radiation : This is caused by the presence of a particle from incomplete atomization .This problem is overcome by increasing the flame temperature . - Transport Interference : Rate of aspiration, nebulization, or transport of the sample ( e g viscosity, surface tension, vapor pressure , and density ) .
  • 46. 2 Atomic Emission Spectroscopy Atomic emission spectroscopy is also an analytical technique that is used to measure the concentrations of elements in samples . It uses quantitative measurement of the emission from excited atoms to determine analyte concentration .
  • 47. The analyte atoms are promoted to a higher energy level by the sufficient energy that is provided by the high temperature of the atomization sources . The excited atoms decay back to lower levels by emitting light . Emissions are passed through monochromators or filters prior to detection by photomultiplier tubes.
  • 48. The instrumentation of atomic emission spectroscopy is the same as that of atomic absorption ,but without the presence of a radiation source . In atomic Emission the sample is atomized and the analyte atoms are excited to higher energy levels all in the atomizer .
  • 49. Schematic Diagram of an Atomic Emission spectrometer
  • 50. The source of energy in Atomic Emission could be a flame like the one used in atomic absorption ,or an inductively coupled plasma ( ICP ) . - The flame ( 1700 – 3150 oC ) is most useful for elements with relatively low excitation energies like sodium potassium and calcium . - The ICP ( 6000 – 8000 oC) has a very high temperature and is useful for elements of high excitation energies .
  • 51. INDUCTIVELY COUPLED PLASMA (ICP)  Plasma is a type of electrical discharge  Plasma is any type of matter that contains an appreciable amount of less than 1% of electrons and +ve ions in equal numbers + atoms + neutral molecules
  • 52.  Plasma has 2 characteristics: i- can conduct electricity II- affected by magnetic fields  Plasma is highly energetic ionized gases usually inert, recently reactive oxygen is used.  ICP is the state-of-the-art plasma  Other plasmas include direct current plasma (DCP) and microwave induced plasma (MIP)
  • 53. ADVANTAGES OF THE ICP  High degree of selectivity  Ability to overcome depressive interference effects  Capable of exciting several elements not excitable by ordinary flames  Higher sensitive than Flame Photometry  Simpler to operate than Arc Spark methods  Higher degree of sensitivity than Arc Spark  Lacks electrodes which gives freedom from contamination and extremely low background.
  • 54. GENERAL CHARACTERISTICS OF THE ICP Up to 70 elements can be analyzed at concentrations below 1 ppm (Fig 1))
  • 55.
  • 56. THE ICP DISCHARGE (Fig 2)  The argon gas is directed through a torch consists of 3 concentric tubes made of quartz  A copper coil called the Load Coil surrounds the top end of the torch and connected to a Radio Frequency Generator (RF)  When RF power (700 – 1500 Watts) is applied to the load coil, an alternating current moves back and forth within the coil or oscillates at a rate corresponding to the frequency of the generator (27 – 40 MHz). This RF oscillation causes the RF electric and magnetic fields to be set up in the area at the top of the torch.
  • 57.
  • 58.  With Argon gas being swirled through the torch, a spark is applied to the gas causing some electrons to strip out from their Argon atoms  These electrons are then caught up in the magnetic field and accelerated by them.  Adding energy to the electrons by the use of the coil in this manner is called “Inductively Coupling”  These high-energy electrons in turn collide with other Argon atoms, stripping off still more electrons
  • 59.  This collisional ionization of Argon continues in a chain reaction thus breaking down the gas into a Plasma consisting of Argon atoms, electrons, and Argon ions know as “ICP” discharge  This ICP discharge is sustained  This ICP discharge appears as intense, brilliant, white and tear-drop shaped (Fig 3)
  • 60.
  • 61.  (Fig 4) Explains what happens to aerosol samples introduced into the plasma
  • 62.
  • 63. (Fig 5) Explains advantage of the plasma with repect to stability, high temperature suurounding the sample for long time (2 milliseconds) thus resulting into lack of matrix interferences.
  • 64.
  • 65. General Information  Used for Qualitative Analysis  Used for Quantitative Analysis  Detection limit is in ppb range  Not possible to determine: H, N, O, C or Ar in trace levels as they are used in solvents and plasma  Not possible to determine F, Cl and noble gases at trace levels as they require high excitation energy  Not used for determining radioactive elements
  • 66.  Upper limit for linear calibration is 10000 – 1000000 times the detection limits for a particular emission line  Only 2 standard solutions are required for the calibration plot as linearity is infinite  ICP has a multi-elemental capability for analysis
  • 68.
  • 69. Similar to an atomic absorption spectrometer ,the monochromator is simply a wavelength selector that separates all different wave lengths and select the desired one . The selected wave length is passed on to a detector that converts the light signal into an electrical signal .
  • 70. Comparison Between Atomic Absorption and Emission Spectroscopy Absorption - Measure trace metal concentrations in complex matrices . - Atomic absorption depends upon the number of ground state atoms . Emission - Measure trace metal concentrations in complex matrices . - Atomic emission depends upon the number of excited atoms .
  • 71. - It measures the radiation absorbed by the ground state atoms. - Presence of a light source ( HCL ) . - The temperature in the atomizer is adjusted to atomize the analyte atoms in the ground state only. - It measures the radiation emitted by the excited atoms . - Absence of the light source . - The temperature in the atomizer is big enough to atomize the analyte atoms and excite them to a higher energy level.
  • 72. 3 AAS APPLICATIONS The are many applications for atomic absorption: - Clinical analysis : Analyzing metals in biological fluids such as blood and urine. - Environmental analysis : Monitoring our environment – e g finding out the levels of various elements in rivers, seawater, drinking water, air, and petrol.
  • 73. - Pharmaceuticals. In some pharmaceutical manufacturing processes, minute quantities of a catalyst used in the process (usually a metal) are sometimes present in the final product. By using AAS the amount of catalyst present can be determined.
  • 74. - Industry : Many raw materials are examined and AAS is widely used to check that the major elements are present and that toxic impurities are lower than specified – e g in concrete, where calcium is a major constituent, the lead level should be low because it is toxic.
  • 75. - Mining: By using AAS the amount of metals such as gold in rocks can be determined to see whether it is worth mining the rocks to extract the gold . - Trace elements in food analysis - Trace element analysis of cosmetics - Trace element analysis of hair