Atomic Absorption spectroscopy
Objectives
After this session students will be able to
• Explain
the principle and instrumentation of atomic absorption
spectrophotometry
• Distinguish
between the atomic absorption spectroscopy and flame photometry
Atomic Absorption
Spectroscopy
Atomic Absorption spectroscopy involves the study of the
absorption of radiant energy by neutral (ground state) atoms in the gaseous
state.
Hollow
Cathode Lamp
Emission is form elements in cathode that have been
sputtered off into gas phase
Electrodless
Discharge Lamps, EDL
For easily evaporized elements as Hg or As
Used for AAS and AES
Give much greater radiation intensities than hollow cathode
There is no electrode, but instead , the inert carrier gas
is energized by an intense field of radiofrequency or microwave radiation →
plasma formation which cause excitation of the metal inside
Degree of
absorption:
Total amount of light absorbed = (πe2/mc2)Nf
Where:
e = electronic charge,
m = mass of electron
c = speed of light,
N = total No. of atoms that
can absorb light
f = Ability of each atom to absorb light
π, e, m,
and c are constants, therefore
Total amount of light absorbed = constant x Nf
Since f is also constant for the same substance
A & C
Interferences
Spectral
Interferences
1. They arise when the absorption line of an interfering
species either overlaps or lies so close to the analyte absorption line that
resolution by the monochromator becomes impossible. Ex. Mg in presence of Ca.
2. They occur from band or continuous spectra which are due
to absorption of molecules or complex ions remaining in the flame
3. They arise from flame background spectrum.
Correction:
1. It may be useful to shift to another spectral line
2. Two line correction method: (Instrumental correction)
It employs a line
from the source as a reference. The line
should lie as close as possible to the analyte line but must not be absorbed by
the analyte. If the conditions are met,
any decrease in the reference line from that observed during calibration arises
from absorption by the matrix of the sample.
Chemical
Interferences
occurs during atomization that prevent the gaseous atoms
production of the analyte. They are more
common than spectral ones.
Types of chemical
interferences
- Formation
of stable compounds: → incomplete dissociation of the sample in flame - Formation
of refractory oxides: → which fail to dissociate into the constituent
atoms
Examples
- Detn.
of Ca in presence of sulphate or phosphate - Formation
of stable refractory oxides of TiO2, V2O5
or Al2O3 by reaction with O2 and OH
species in the flame
Overcome
1. Increase in the flame temp. → Formation of free gaseous
atoms
e.g. Al2O3
is readily dissociated in acetylene-nitrous oxide flame
2. Use of releasing agents:
M-X + R → RX +
M ex. Detn of Ca in presence of phosphate
(Ca – phosphate +
SrCl2 → Sr-phosphate + Ca atoms) or (Ca – phosphate + EDTA → Ca-EDTA
easily dissociated complex).
3. Solvent extraction of the sample or of the interferring
elements
Ionization
Interferences
Ionization of atoms in the flame → decrease the absorption
or emission
Overcome : 1. Use of lowest possible temp which is
satisfactory for the sample ex. Acetylene –air must not be used for easily
ionised elements as Na, K, Ca, Ba
2. Addition of an ionisation supressant ( soln of cation has
a lower ionisation potential than that of the sample, e.g. addition of K-soln
to Ca or Ba soln. Ca → Ca2+ +
2e K → K+ + e
Physical
Interferences
- Variation
in gas flow rate - Variation
in sample viscosity - Change
in flame temp.
Overcome: 1. by continuous calibration
2. Use of internal standard
Advantages of AAS:
Very sensitive.
Fast.
Disadvantages of
AAS: Hollow cathode lamp for
each element.
Expensive element.
Relationship
between Atomic Absorption and Flame Emission Spectroscopy
Atomic Absorption | Flame Emission |
1. Measures the | 1. Measures the |
2. Depends only | 2. Depends only |
3. Absorption | 3. Emission |
Summary
• Atomic
Absorption spectroscopy involves the study of the absorption of radiant energy
by neutral (ground state) atoms in the gaseous state.
• Hollow
cathode lamp is the radiation source.
• Total
amount of light absorbed = (πe2/mc2)Nf
Where:
e = electronic charge,
m = mass of electron
c = speed of light,
N = total No. of atoms that can absorb light
f = Ability of each atom to absorb light
π, e, m,
and c are constants,