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Fourier Transform InfraRed
Spectroscopy ; FT-IR
Jintara Padchasri
04/06/58 1FT-IR
Outline
Basic Ideas Wavelength and Wavenumber What is the FT-IR ? Why Infrared Spectroscopy? Older Technology Theory and Instrumentation Mathematics Applications Advantages and Disadvantages
04/06/58 2FT-IR
Basic Ideas Wavelength and Wavenumber What is the FT-IR ? Why Infrared Spectroscopy? Older Technology Theory and Instrumentation Mathematics Applications Advantages and Disadvantages
Basic Ideas; Energy Level
04/06/58 FT-IR 3
About 15 micron radiationBasic Global Warming:The C02 dance
Wavelength and Wavenumber Wavelength = 1 / Wavenumber
For the IR, wavelength is in microns.
Wavenumber is typically in 1/cm, or cm-1.
5 microns corresponds to 2000 cm-1.
20 microns corresponds to 500 cm-1.
15 microns corresponds to 667 cm-1. Much‘terrestrial’ IR energy at the wavenumber.
04/06/58 FT-IR 4
Wavelength = 1 / Wavenumber
For the IR, wavelength is in microns.
Wavenumber is typically in 1/cm, or cm-1.
5 microns corresponds to 2000 cm-1.
20 microns corresponds to 500 cm-1.
15 microns corresponds to 667 cm-1. Much‘terrestrial’ IR energy at the wavenumber.
What is FT-IR?
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What is FT-IR?what information can FT-IR provide? It can identify unknown materials It can determine the quality or consistencyof a sample It can determine the amount of componentsin a mixture
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what information can FT-IR provide? It can identify unknown materials It can determine the quality or consistencyof a sample It can determine the amount of componentsin a mixture
Why Infrared Spectroscopy?
IR spectrum ;fingerprint of a sample withabsp. peaks which correspond to the f ofvibrations between the bonds of the atomsmaking up the material. Because each different material is a uniquecombination of atoms, no two compounds producethe exact same IR spectrum IR can result in a positive identification ofevery different kind of material. Size of peaks in the spectrum is a directindication of amount of material.
04/06/58 7FT-IR
IR spectrum ;fingerprint of a sample withabsp. peaks which correspond to the f ofvibrations between the bonds of the atomsmaking up the material. Because each different material is a uniquecombination of atoms, no two compounds producethe exact same IR spectrum IR can result in a positive identification ofevery different kind of material. Size of peaks in the spectrum is a directindication of amount of material.
Older TechnologyFT-IR spectroscopy is preferred over dispersive orfilter methods of infrared spectral analysis forseveral reasons:
It is a non-destructive technique It provides a precise measurement method whichrequires no external calibration It can increase speed, collecting a scan every second It can increase sensitivity – one second scans can be co-added together to ratio out random noise It has greater optical throughput It is mechanically simple with only one moving part
It is a non-destructive technique It provides a precise measurement method whichrequires no external calibration It can increase speed, collecting a scan every second It can increase sensitivity – one second scans can be co-added together to ratio out random noise It has greater optical throughput It is mechanically simple with only one moving part
Theory and InstrumentationThe Michelson interferometer principle1. Monochromatic light
Movable mirror δ = Optical Path Difference
04/06/58 9FT-IR
Detector
Stationary MirrorBeamsplitter
Interference
δ = (n + ½) λ
δ = n λ
2. Dichromatic source
II
Theory and Instrumentation
04/06/58 FT-IR
10
vδ
- l -l/2 0 l/2 l
Moveable mirror
3. Broadband source
I I
Theory and Instrumentation
04/06/58 FT-IR 11
v
Continuous IR spectrum Interferogram
δ0
FT
Mathematics
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Time domain: I vs. δ Frequency domain: I vs. v
δ
I
v
I
Mathematics
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Optical path difference is
Intensity of the detector has maxima at
and minima at
)(I 2,1,0, nn )2/1( n
MathematicsThe resulting interferogram is described as an infinitely long
cosine wave
where =intensity as F(v)
For non-monochromatic source treat each frequency as if itresulted in a separate cosine train.
)2cos()(B )(B
04/06/58 FT-IR 14
The resulting interferogram is described as an infinitely longcosine wave
where =intensity as F(v)
For non-monochromatic source treat each frequency as if itresulted in a separate cosine train.
ApplicationsApplications are vast and diverse.Some of them are
Compositional analysis of organic, inorganic and polymers
Biological and biomedical fields like detection of water inbiological membranes
Analysis of Aircraft exhausts
Measurement of toxic gas in fuels
Combustion
Gas analysis
and lots more
04/06/58 FT-IR 15
Compositional analysis of organic, inorganic and polymers
Biological and biomedical fields like detection of water inbiological membranes
Analysis of Aircraft exhausts
Measurement of toxic gas in fuels
Combustion
Gas analysis
and lots more
Advantages and Disadvantages FT – IR can take wavelength readings across the whole IRregion simultaneously and smoothly, making this a very rapidtechnique.
The technique is non-invasive and non-destructive. Its willnot give the same detailed structural information that NMR,MS, or X-ray crystallography.
Spec. in the freq. domain can never be eyeballedconclusively. They are always subject to some sort ofmanipulation, leading some to believe that the data can saywhatever the experimenter wants it to say depending on how itis manipulated.
Greater wavenumber accuracy. Most FT instruments havean accuracy of +/- 0.01 cm-1
04/06/58 FT-IR 16
FT – IR can take wavelength readings across the whole IRregion simultaneously and smoothly, making this a very rapidtechnique.
The technique is non-invasive and non-destructive. Its willnot give the same detailed structural information that NMR,MS, or X-ray crystallography.
Spec. in the freq. domain can never be eyeballedconclusively. They are always subject to some sort ofmanipulation, leading some to believe that the data can saywhatever the experimenter wants it to say depending on how itis manipulated.
Greater wavenumber accuracy. Most FT instruments havean accuracy of +/- 0.01 cm-1
04/06/58 17FT-IR