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MOLECULAR ABSORPTION SPECTROSCOPY; THEORY,
INSTRUMENTATION AND APPLICATION
2.1 Terms employed in Absorption Spectroscopy
Term & Symbol Definition Alternative Name & Symbol
Incident radiant power, Po
Radiant power in watts in incident on sample
Incident intensity, Io
Transmitted radiant Power, P
Radiant power transmitted by sample
Transmitted intensity, I
Absorbance, A Log (Po/P) Optical density, D; extinction, E
Transmittance, T P/Po Transmission, T
Path length of sample, b
Length over which attenuation occurs
l,d
Absorptivity, a A/(bc) Extinction coefficient, k
Molar absorptivity, ε A/bc Molar extinction coefficient
2.1.1 Transmittance T
2.1.1 Transmittance T
2.1.2 Absorbance A
• The logarithm of the ratio between the initial power of a beam of radiation Po and its power after it has traversed an absorbing medium:
• When Absorbance of a solution increases, transmittance decreases
2.1.2 Absorbance A
2.1.3 Measuring Transmittance & Absorbance
• Losses in measuring: Reflection losses and scattering losses in solution
• To compensate these effects, the power of the beam transmitted through a cell containing the analyte solution is compared with one that traverses either in identical cell containing only the solvent/reagent blank
2.1.4 Sample Containers
2.2 Beer’s Law
2.2 Beer’s Law
Exercise:
A 7.25 x 10-5 M solution of potassium permanganate has a transmittance of 44.1% when measured in a 2.10 cm cell at a wavelength of 525 nm. Calculate (a) the absorbance of this solution; (b) the molar absorptivity of KMnO4
2.2.1 Application of Beer’s Law to Mixtures
• Beer’s Law also applies to solutions containing more than one kind of absorbance substance
• Provided that there is no interaction among the various species, the total absorbance of multicomponent system at a single wavelength is the sum of the individual absorbances:
2.2.2 Limitation to the applicability of Beer’s Law
• There are few exceptions to the linear relationship between absorbance and path length at a fixed concentration due to deviation:– Real deviation (fundamental)– Method:
• Instrumental• Chemical
2.2.2 Limitation to the applicability of Beer’s Law
2.2.2 Limitation to the applicability of Beer’s Law
2.2.2 Limitation to the applicability of Beer’s Law
2.2.2 Limitation to the applicability of Beer’s Law
2.2.2 Limitation to the applicability of Beer’s Law
2.2.3 Absorption Spectra
• Line spectra – Occur when the radiating species are individual atomic particles
that are well separated in gas– The individual particles in a gases medium behave
independently of one another, and spectrum consists of a series of sharp lines
• Band spectra– Are often produced in spectral source because of the presence
of gases radicals or small molecules– This spectra is not fully resolved by the instruments
2.2.3 Absorption Spectra
• Continuum Spectra
2.2.3 Absorption Spectra
2.3 Instruments for Optical Absorption Instruments
• Ultraviolet/Visible Spectrophotometers– Single beam instruments– Double beam instruments– Multichannel instruments
• Infrared Spectrophotometer– Dispersive Instruments– Fourier Transform Instruments
2.3.1.1 Single Beam Instruments
2.3.1.2 Double Beam Instruments
2.3.1.2 Double Beam Instruments
2.3.1.3 Multichannel Instruments
2.3.2.IR Spectrophotometers – Dispersive Instruments
2.3.2.IR Spectrophotometers – Fourier Transform
• Characteristics:– Great speed– High resolution– High sensitivity– Excellent wavelength precision and accuracy
• FTIR have been reduced to benchtop size which is reliable and easy to maintain, less price
• Contain no dispersive elements, all wavelengths are detected and measured simultaneously
• Interferometer is used to produce interference patterns that contain the IR spectral information
• Types of sources are the same as dispersive instruments
• Transducers: pyro-electric transducer, photoconductive transducer
• Most FTIR are of the single beam type
2.3.2.IR Spectrophotometers – Fourier Transform
• Advantages:– Better speed and sensivity– Simpler mechanical design– Better light-gathering power– More accurate wavelength calibration– Elimination of stray light and IR emission