Atomic absorption spectroscopy (AAS) is defined as the measurement and interpretation of the absorbed radiation in atomic level. This method is widely used for the determination of the elements. Robert Wilhelm Bunsen and Gustav Robert Kirchoff first proposed the AAS theory. Alan Walsh first introduced the principle of AAS.
The atoms present in the ground state absorb the radiation produced by the flame and excited to the excited state and which is measured by the AAS spectrometer. Atomic absorption measures the amount of light at the wavelength which is absorbed by the atoms. Atoms present in the sample are directly proportional to the absorption intensity.
Schematic diagrams for the atomic absorption
Steps involved in the AAS:
There are mainly three steps involved in the AAS:
AAS is used to determine the absorbed light which directly gives the concentration of the element present in the sample. The absorption is directly proportional to the concentration which is derived from the Beer–Lambert's law.
The total amount of absorbed light is given by
where e is the charge; m is the mass of the electron; c is the speed of the light; N is the total number of atoms; f is the oscillator strength; Π, e and m are constants hence the equation becomes
The AAS contains the following components:
Schematic diagram for the atomic absorption spectrometer
The radiation source of AAS should posses the following characters:
There are two types of radiation sources used in the AAS.
Hallow cathode lamp: This is the most frequently used radiation source in AAS. This consists of a sealed glass tube which in turn consists of tungsten anode and cylindrical cathode with quartz window and the rest of the glass tube is filled with argon gas at low pressure.
Diagram for the hallow cathode lamp
Electrode less discharge lamp: This is rarely used because of its high cost and less sensitivity. It consists of quartz tube containing inert gas and metal. This metal is excited with the radio frequency coil.
Diagram for the electrode less discharge lamp
Steps involved in the atomic absorption spectroscopy
There are two main types of atomisers used in the AAS.
Schematic diagram for the atomiser
Schematic diagram for the electro thermal atomiser
Generally prism and grating monochromators are used. The main use of monochromator is to convert the polychromatic light to monochromatic light.
The detector commonly employed in the AAS is the photomultiplier tube. Electrons from the photocathode are attracted to anode 1 and liberate more electrons which trowel towards anode 2 and continue till the last anode. The final current of 106–108 times is greater than that of primary current.
From the detector, the electric current produced is amplified with AC amplifier and DC ampli-fer amplifies and the difference in the frequency is summarised and recorded with the help of recorder.
There are mainly three types of interferences:
Single-beam atomic absorption spectrometer: In this, the radiation source is connected to chopper and then to atomiser which is connected to the monochromator. The signal is detected by the detector and recorded by the recorder.
Double-beam atomic absorption spectrometer: The radiation source is connected to the chopper then it splits the incident beam into two paths one is to the sample and another to the reference. These two are connected by the monochromator which measures the difference in the intensity of the sample with that of the reference. Then the signals are detected by the detector and recorded by the recorder.
Schematic diagram for the double beam AA spectrometer
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