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“INFRARED ABSORPTION
SPECTROSCOPY”
“IntroductionTo
IR Spectroscopy”
Spectroscopy
Absorption
spectroscopy
UV
spectroscopy
IR
spectroscopy
NMR
spectroscopy
Emission
spectroscopy
Fluorimetry
Flame
photometery
 Infrared
spectroscopy (IR
spectroscopy) is
the spectroscopy that deals
with the infrared region of
the electromagnetic
spectrum, that is light with a
longer wavelength and
lower frequency than visible
light
 Infrared Spectroscopy is the
analysis of infrared light
interacting with a molecule.
 It is based on absorption
spectroscopy
INFRARED REGIONS RANGE
Near infrared region 0.8-2.5 µ(12,500-4000 cm-1)
Main infrared region 2.5-15 µ(4000-667cm-1)
Far infrared region 15-200 m µ(667-100 cm-1)
 When infrared 'light' or radiation hits a molecule, the bonds in
the molecule absorb the energy of the infrared and respond by
vibrating.
IR
radiation
vanllin
Molecular vibrations
“Molecular Vibrations”
MOLECULAR
VIBRATIONS
Fundamental
Vibrations
Stretching
Vibration
Symmetri
c
Asymmetric
Bending
Vibration
In-plane
Bending
Scissoring Rocking
Out Of Plane
Bending
Wagging Twisting
Non-
fundamental
Vibrations
OverTones,
Combination
Tones,
Fermi
Resonance
What is a vibration in a molecule?
“Any change in shape of the molecule- stretching of bonds,
bending of bonds, or internal rotation around single bonds”.
Why we study the molecular vibration?
Because whenever the interaction b/w electromagnetic waves
& matter occur so change appears in these vibrations.
FUNDAMENTAL
VIBRATIONS
• Vibrations which appear as band in
the spectra.
NON-
FUNDAMENTAL
VIBRATIONS
• Vibrations which appears as a
result of fundamental vib.
Mol. vibration divided into 2 main types:
1.Streching vibration
Involves a continuous
change in the inter
atomic distance along
the axis of the bond
b/w 2 atoms.
2.It requires more
energy so appear at
shorter wavelength.
STRETCHING
VIB.
1.Bending vibrations
are characterized by a
change in the angle
b/w two bonds.
2.It requires less energy
so appear at longer
wavelength.
BENDING
VIB.
Fundamental vibration is also divided into types:
SYMMETRIC VIB.
• Inter atomic
distance b/w 2
atoms
increases/decreases.
ASYMMETRIC
VIB.
• Inter atomic
distance b/w 2
atoms is
alternate/opposite.
• If all the atoms are
on same plane.
IN PLANE
BENDING
• If 2 atoms are on
same plane while the
1 atom is on
opposite plane.
OUT OF
PLANE
BENDING
SCISSORING:
When 2 atoms
move away or
close towards
each other.
ROCKING:
Change in angle
b/w a group of
atoms.
• Change in angle
b/w the plane of
a group of atom
WAGGING
• Change in angle
b/w the plane of
2 groups of
atoms.
TWISTING
NON-
FUNDAMENTAL
OVERTONES:
These are
observed at twice
the frequency of
strong band.
Ex:
carbonyl group.
COMBINATION
TONES:
Weak bands that
appear occasionally
at frequencies that
are sum/difference of
2 or more
fundamental bands.
FERMI
RESONANCE:
Interaction b/w
fundamental
vibration &
overtones or
combination
tones.
Ex:CO2
“Coupled Interactions And
Factors”
Interactions between vibrations can occur (Coupling) if the
vibrating bonds are joined to a single, central atom.
This is because there is mechanical coupling interaction
between the oscillators.
Example:
C=O (both symmetric and asymmetric stretching
vibrations)
• Coupling is greatest when the coupled groups have
approximately equal energies
• Coupling between a stretching vibration and a bending
vibration occurs if the stretching bond is one side of
an angle varied by bending vibration.
• No coupling is seen between groups separated by two
or more bonds
c
C c cLess coupling
no coupling
Greater
coupling
THE RELATIVE MASS OFTHE
ATOMS: heavier the atoms lower is
the vibration frequency of the bond
between them.
THE FORCE CONSTANT OF
THE BONDS: Stronger the bond
higher is the vibration frequency.
Stronger bonds O-H, N-H & C-H
weaker bonds C-C & C-O bond.
EFFECTS OF BONDS: C=C stretching
is expected to absorb at a higher
frequency than C-C stretching.
Example: C≡C 2200cm-1
C=C 1650cm-1
C-C 1200cm-1
“Degree Of Freedom”
For linear (3n-5)degree of freedom represent fundamental vibrations
For non linear (3n-6)degree of freedom represent fundamental vibrations
For a molecule containing n number of atom s has 3n degree of freedom
Each atom has 3 degree of freedom depend on x , y ,z
Fundamental vibration of molecule depend on degree of freedom
For non linear molecule 3 degree of freedom represent rotational &
transational motion
Only those vibrational changes that result in change in
dipole movement appear as band
All vibrational changes don’t appear as band
 It gives the relation between frequency of oscillation ,
atomic mass , force constant of the bond .
 Thus vibrational frequency is
 C = velocity of light
 F = force constant
 Mx= mass of atom x
 My = mass of atom y
 Since force constant measures the strength of bond,
value of f is
• 5×10⁵ dynes/cmFOR SINGLE
BOND
• 10×10⁵ dynes /cmFOR DOUBLE
BOND
• 15×10⁵ dynes/cmFOR TRIPLE
BOND
Factors OnWhichVibrational Frequency
Depends:
ATOMIC
MASS
BOND
STRENGTH
“Hydrogen Bonding”
Proton Donor Group (S-Orbital )
Proton Acceptor Group (P-Orbital)
Hydrogen Bonding
Proton Donor Group
Carboxyl, Hydroxyl,Amine Or Amide Group
Proton Acceptor Group
Oxygen, Nitrogen, Halogens And Unsaturated Group
1-Intermolecular Hydrogen Bonding
2-Intramolecular Hydrogen Bonding
Collinear Non-linear
P-Hydroxyacetophenone o-Hydroxyacetophenone
Stretching bands move towards longer wavelength or lower
frequencies And Bending vibrations shift towards Shorter
wavelength or Higher frequencies.
Bending vibrations Stretching vibrations
Temperature
Concentration
Molecular Geometry
Relative Acidity
Basicity
“Instrumentation”
The main parts of IR spectrometer are as follows:
 radiation source
 sample cells and sampling of substances
 monochromators
 detectors
 recorder
IR instruments require a source of radiant energy which
emit IR radiation which must be:
Sufficient
intensity
Continuous Stable
Sources of IR radiations are as follows:
GLOBAR:
Rod of silicon
carbide
Heated up to
1300 degree
centigrade
Produce radiant
energy from 1-
40 micron
 NERNST GLOWER:
Rod of
zirconium and
yittrium
Heated up to
1500 degree
centigrade
Emits radiation
between 0.4-
20 micron.
 For gas samples:
The spectrum of a gas can be obtained by
permitting the sample to expand into an evacuated
cell, also called a cuvette.
 For solution sample:
Infrared solution cells consists of two windows
of pressed salt sealed. Samples that are liquid at
room temperature are usually analyzed in pure
form or in solution.The most common solvents are
Carbon Tetrachloride (CCl4) and Carbon Disulfide
(CS2).
 For solid sample:
Solids reduced to small particles (less than 2 micron) can be
examined as a thin paste or mull.The mull is formed by grinding
a 2-5 milligrams of the sample in the presence of one or two
drops of a hydrocarbon oil (nujol oil).The resulting mull is then
examined as a film between flat salt plates.
Another technique is to ground a
milligram or less of the sample with
about 100 milligram potassium
bromide.The mixture is then pressed
in an evaluable die to produce a
transparent disk.
“Detectors”
Detector
Thermal Non-thermal
There are four types of thermal detector.
Bolometers
Thermocouple and thermopile
Pyro electric detector
Golay cell
Bolometer is derived from a Greek word
(bolometron)
Bolo = for something thrown
Metron = measure
Construction
 A bolometer consists of an absorptive element, such as a
thin layer of metal.
 Most bolometers use semiconductor or superconductor
absorptive elements rather than metals.
Working
Thin layer of metal
connected to a
reservoir
Any radiation on the
absorptive element
raises its temperature
above that of the
reservoir.
The temperature
change can be
measured directly
with an attached
thermometer.
Temperature changes Potential difference changes
Thermocouples consist of a pair of junctions of different metals; for
example, two pieces of bismuth fused to either end of a piece of antimony.
Thermopile detectors are voltage-generating devices,
which can be thought of as miniature arrays of
thermocouple junctions.
Construction:
• Single crystalline wafer of
a pyro electric material,
such as triglycerine
sulphate.
• Pyro electric Infrared
Detectors (PIR) convert
the changes in incoming
infrared light to electric
signals.
Below curie temperature
Pyro electric materials exhibit electrical polarization.
Temperature is altered, the polarization changes.
Observed as an electrical signal
(if electrodes are placed on opposite faces of a thin slice of the material
to form a capacitor)
Construction:
 Small metal cylinder
 Flexible silvered diaphragm
 Whole chamber is filled with xenon gas.
Metal cylinder and flexible diaphragm
Temperature increases
Gas is expended and diaphragm deforms
detect as a signal
Thin film overlaps
over non-
conducting surface
Absorption of IR
radiation
Non conducting
valence e- to higher
energy conducting
state
Electrical resistance
decreases
Voltage drops
Infrared radiations
Photovoltaic detector
Generates a small voltage
Detected as a signal
“Single/Double Beam
IR Absorption Spectrophotometers”
SINGLE BEAM
SPCETROPHOTOMETER
DOUBLE BEAM
SPECTROPHOTOMETER
 A single beam of light , which
can pass through one solution
at a time (sample or reference).
 A single beam of light splits
into two separate beams. One
passes through the sample,
another passes through the
reference.
Radiation
Source
Sample Cell
Mono-
chromator
Detector
Radiation
Source
Sample &
Reference
Compartment
Chopper Attenuator
Monochromator
Detector
Synchronous
rectifier
Synchronous
motor
Attenuator &
recorder
 All frequencies are
examined
simultaneously in
Fourier transform
infrared (FTIR)
spectroscopy.
“Applications Of
IR Absorption Spectrocopy”
Since different molecules with
different combination of
atoms produce their unique
spectra, infrared spectroscopy
can be used to qualitatively
identify substances.
Group Frequency Region Fingerprint Region
 consisting of the absorption bands
of the functional groups.
 frequency = 4000-1300cm-¹
 wavelength = 2.5-8
 IR spectra is called “fingerprints”
because no other chemical
species will have similar IR
spectrum.
 Single bonds give their absorption
bands in this region.
 Frequency=1300-650cm-1
 Wavelength=8-15.4
 Organic groups differ from one another both in the
strength of the bond and the masses of the atom
involved.
• 4000 and 1300 cm-¹
• Alcohols and amines
• 1300 and 909 cm-¹
• Complex interactions
• 909 and 65o cm-¹
• Benzene rings
 Observing rate of disappearance of characteristic
absorption band in reactants; or
 Rate of increasing absorption bands in products of a
particular product.
 E.g.: O—H = 3600-3650 cm-¹
C=O = 1680-1760 cm-¹
infrared absorption spectroscopy

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