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INFRARED SPECTROSCOPY
THEORY
PRESENTED BY: ANUPAMA RAMACHANDRAN
1st Year M Pharm Pharmacology
1
CONTENTS
• INTRODUCTION
• IR SPECTROSCOPY
• PRINCIPLE
• MOLECULAR VIBRATIONS
• COUPLED INTERACTIONS
• DEGREE OF FREEDOM
• SUMMARY
• REFERENCE
2
INTRODUCTION
• Spectroscopy is the measurement and interpretation of EMR absorbed or emitted
when the molecules or atoms or ions of a sample moves from one energy state to
another energy state.
• Spectroscopy is an instrumentally aided study of the interactions between matter
(sample being analyzed) and energy (any portion of the electromagnetic
spectrum)
3
SPECTROSCOPY
ABSORPTION SPECTROSCOPY EMISSION SPECTROSCOPY
*UV SPECTROSCOPY * FLUORIMETRY
*IR SPECTROSCOPY * FLAME PHOTOMETRY
*NMR SPECTROSCOPY
4
IR SPECTROSCOPY
• Energy of molecule = Electronic energy+ Vibrational energy + Rotational
energy
• IR spectroscopy is concerned with the study of absorption of infrared
radiation, which causes vibrational transition in the molecule. Hence, IR
spectroscopy also known as Vibrational spectroscopy.
• IR spectra mainly used in structure elucidation to determine the functional
groups.
5
6
IR REGION: 0.8 µm (800nm) to 1000 µm (1mm)
subdivided into
1.Near IR: 0.8-2 µm
2.Middle IR: 2-15 µm
3.Far IR: 15-1000 µm
Most of the analytical applications are confined to the middle IR region
because absorption of organic molecules are high in this region.
7
• GROUP FREQUENCY REGION:( 4000 to 1500 cm-1)
Contain relatively few peaks.
Associated with stretching vibrations.
Almost all the stretching vibrations are above 1450 cm-1.
IR stretching frequencies
8
FINGER PRINT REGION: (1500 – 400 cm-1 )
• Usually consist of bending vibrations within the molecule.
• pattern of peaks are more complicated & is much difficult pickout
individual bonds in this region
• Each compound produce its own unique pattern of peaks like a finger
print in this region .
9
• In pharmaceutical analysis, infrared radiation (mid IR) of wavelength
25µ to 2.5µ or wave numbers from 400cm-1 to 4000 cm-1.
• we use wave no. instead of wave length for mentioning characteristic
peak ,because wave numbers are larger values & easy to handle than
wave lengths.
• Wave no: no. of waves present per cm
•
1
𝑤𝑎𝑣𝑒𝑙𝑒𝑛𝑔𝑡ℎ 𝑖𝑛 𝜇
× 104
= wave no. per cm
10
• Molecules are made up of atoms linked by chemical bonds. The
movement of atoms and the chemical bonds is like spring and balls
(vibration).
• This characteristic vibration are called Natural frequency of vibration.
PRINCIPLE OF IR SPECTROSCOPY
11
• When energy in the form of infrared radiation is applied ,then it
causes vibration between the atoms of the molecules and when,
Applied infrared frequency = Natural frequency of vibration
Then, Absorption of IR radiation takes place and a peak is observed.
Different functional groups absorb characteristic frequencies
of IR radiation. Hence gives the characteristic peak value. Therefore, IR
spectrum of a chemical substance is a finger print of a molecule for its
identification.
12
CRITERIA FOR A COMPOUND TO ABSORB IR
RADIATION
• 1. Correct wavelength of radiation
• 2. Change in dipole moment
1. Correct wavelength of radiation:
A molecule to absorb IR radiation, the natural frequency of vibrations
of some part of a molecule is the same as the frequency of incident
radiation.
13
2. Change in dipole moment
• A molecule can only absorb IR radiation when its absorption cause a
change in its electric dipole
• A molecule is said to have an electric dipole when there is a slight
positive and a slight negative charge on its component of atoms.
14
MOLECULAR VIBRATIONS
• Any change in shape of the
molecule.
2 types,
1) fundamental vibrations
2) non fundamental vibrations
15
FUNDAMENTAL VIBRATIONS
There are 2 types of vibrations:
1.Stretching vibrations
2.Bending vibrations
16
1.STRETCHING VIBRATIONS:
 Vibration or oscillation along the line of bond
Change in bond length
 Occurs at higher energy: 4000-1250 cm-1
2 types:
a)Symmetrical stretching
b)Asymmetrical stretching
17
a) Symmetrical stretching:
• 2 bonds increase or decrease in length simultaneously.
18
Symmetrical stretching
19
b) Asymmetrical stretching:
• in this, one bond length is increased and other is decreased
20
Asymmetrical stretching
21
2. BENDING VIBRATIONS
 Vibration or oscillation not along the line of bond
 These are also called as deformations
 In this, bond angle is altered
 Occurs at low energy: 1400-666 cm-1
 2 types:
a) In plane bending: scissoring, rocking
b) Out plane bending: wagging, twisting
22
a) In plane bending
i. Scissoring:
• This is an in plane bending
• 2 atoms approach each other
• Bond angles are decreased
23
Scissoring
24
ii. Rocking:
• Movement of atoms take place in the same direction.
25
Rocking
26
b) Out plane bending
i. Wagging:
• 2 atoms move to one side of the plane.
• They move up and down the plane.
27
Wagging
28
ii. Twisting:
• One atom moves above the plane and another atom moves below
the plane.
29
Twisting
30
COUPLED INTERACTIONS
• 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)
31
REQUIREMENTS FOR COUPLING
• The vibrations must be of the same symmetry species if interaction is
to occur.
• Strong coupling of stretching vibrations occurs when there is a
common atom between the two vibrating bonds.
• Coupling of bending vibrations occur when there is a common bond
between vibrating groups.
32
• 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
33
34
FACTORS AFFECTING FREQUENCY OF IR
ABSORPTION
• Relative mass of the atom.
• Force constant of the bonds.
• Geometry of the atom.
35
DEGREE OF FREEDOM
• Fundamental vibration of molecule depend on degree of freedom.
• Each atom has 3 degree of freedom depend on x, y, z.
• For a molecule containing n no. of atoms has 3n degree of freedom.
• For non – linear molecule, 3 degree of freedom represent rotational &
transational motion.
• For non-linear, ( 3n -6) degree of freedom represent fudamental vibrations.
• For linear (3n-5) degree of freedom represent fundamental vibrations.
• All vibrational changes don’t appear as band.
• Only those vibrational changes that result in change in dipole moment
appear as band.
36
TYPICAL INFRARED SPECTRUM
37
38
SUMMARY
• Absorption spectroscopy.
• Vibrational transitions.
• Applied infrared frequency = Natural frequency of vibration.
• Structure elucidation to determine functional groups.
39
REFERENCES
1. Spectrometric identification of organic compounds, sixth edition,
Robert M. Silverstein & Francis X. Webster. Page no: 71 – 76
2. Principles of instrumental analysis, 6th edition, Douglas A. Skoog , E
James Holler, Stanley R Crouch . Page no: 430 – 455
3. Introduction to spectroscopy, Donald L Pavia, Gary M. Lampman,
James R. Vyvyan. Page no: 15 - 31
40
Thank you…
41

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IR SPECTROSCOPY

  • 1. INFRARED SPECTROSCOPY THEORY PRESENTED BY: ANUPAMA RAMACHANDRAN 1st Year M Pharm Pharmacology 1
  • 2. CONTENTS • INTRODUCTION • IR SPECTROSCOPY • PRINCIPLE • MOLECULAR VIBRATIONS • COUPLED INTERACTIONS • DEGREE OF FREEDOM • SUMMARY • REFERENCE 2
  • 3. INTRODUCTION • Spectroscopy is the measurement and interpretation of EMR absorbed or emitted when the molecules or atoms or ions of a sample moves from one energy state to another energy state. • Spectroscopy is an instrumentally aided study of the interactions between matter (sample being analyzed) and energy (any portion of the electromagnetic spectrum) 3
  • 4. SPECTROSCOPY ABSORPTION SPECTROSCOPY EMISSION SPECTROSCOPY *UV SPECTROSCOPY * FLUORIMETRY *IR SPECTROSCOPY * FLAME PHOTOMETRY *NMR SPECTROSCOPY 4
  • 5. IR SPECTROSCOPY • Energy of molecule = Electronic energy+ Vibrational energy + Rotational energy • IR spectroscopy is concerned with the study of absorption of infrared radiation, which causes vibrational transition in the molecule. Hence, IR spectroscopy also known as Vibrational spectroscopy. • IR spectra mainly used in structure elucidation to determine the functional groups. 5
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  • 7. IR REGION: 0.8 µm (800nm) to 1000 µm (1mm) subdivided into 1.Near IR: 0.8-2 µm 2.Middle IR: 2-15 µm 3.Far IR: 15-1000 µm Most of the analytical applications are confined to the middle IR region because absorption of organic molecules are high in this region. 7
  • 8. • GROUP FREQUENCY REGION:( 4000 to 1500 cm-1) Contain relatively few peaks. Associated with stretching vibrations. Almost all the stretching vibrations are above 1450 cm-1. IR stretching frequencies 8
  • 9. FINGER PRINT REGION: (1500 – 400 cm-1 ) • Usually consist of bending vibrations within the molecule. • pattern of peaks are more complicated & is much difficult pickout individual bonds in this region • Each compound produce its own unique pattern of peaks like a finger print in this region . 9
  • 10. • In pharmaceutical analysis, infrared radiation (mid IR) of wavelength 25µ to 2.5µ or wave numbers from 400cm-1 to 4000 cm-1. • we use wave no. instead of wave length for mentioning characteristic peak ,because wave numbers are larger values & easy to handle than wave lengths. • Wave no: no. of waves present per cm • 1 𝑤𝑎𝑣𝑒𝑙𝑒𝑛𝑔𝑡ℎ 𝑖𝑛 𝜇 × 104 = wave no. per cm 10
  • 11. • Molecules are made up of atoms linked by chemical bonds. The movement of atoms and the chemical bonds is like spring and balls (vibration). • This characteristic vibration are called Natural frequency of vibration. PRINCIPLE OF IR SPECTROSCOPY 11
  • 12. • When energy in the form of infrared radiation is applied ,then it causes vibration between the atoms of the molecules and when, Applied infrared frequency = Natural frequency of vibration Then, Absorption of IR radiation takes place and a peak is observed. Different functional groups absorb characteristic frequencies of IR radiation. Hence gives the characteristic peak value. Therefore, IR spectrum of a chemical substance is a finger print of a molecule for its identification. 12
  • 13. CRITERIA FOR A COMPOUND TO ABSORB IR RADIATION • 1. Correct wavelength of radiation • 2. Change in dipole moment 1. Correct wavelength of radiation: A molecule to absorb IR radiation, the natural frequency of vibrations of some part of a molecule is the same as the frequency of incident radiation. 13
  • 14. 2. Change in dipole moment • A molecule can only absorb IR radiation when its absorption cause a change in its electric dipole • A molecule is said to have an electric dipole when there is a slight positive and a slight negative charge on its component of atoms. 14
  • 15. MOLECULAR VIBRATIONS • Any change in shape of the molecule. 2 types, 1) fundamental vibrations 2) non fundamental vibrations 15
  • 16. FUNDAMENTAL VIBRATIONS There are 2 types of vibrations: 1.Stretching vibrations 2.Bending vibrations 16
  • 17. 1.STRETCHING VIBRATIONS:  Vibration or oscillation along the line of bond Change in bond length  Occurs at higher energy: 4000-1250 cm-1 2 types: a)Symmetrical stretching b)Asymmetrical stretching 17
  • 18. a) Symmetrical stretching: • 2 bonds increase or decrease in length simultaneously. 18
  • 20. b) Asymmetrical stretching: • in this, one bond length is increased and other is decreased 20
  • 22. 2. BENDING VIBRATIONS  Vibration or oscillation not along the line of bond  These are also called as deformations  In this, bond angle is altered  Occurs at low energy: 1400-666 cm-1  2 types: a) In plane bending: scissoring, rocking b) Out plane bending: wagging, twisting 22
  • 23. a) In plane bending i. Scissoring: • This is an in plane bending • 2 atoms approach each other • Bond angles are decreased 23
  • 25. ii. Rocking: • Movement of atoms take place in the same direction. 25
  • 27. b) Out plane bending i. Wagging: • 2 atoms move to one side of the plane. • They move up and down the plane. 27
  • 29. ii. Twisting: • One atom moves above the plane and another atom moves below the plane. 29
  • 31. COUPLED INTERACTIONS • 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) 31
  • 32. REQUIREMENTS FOR COUPLING • The vibrations must be of the same symmetry species if interaction is to occur. • Strong coupling of stretching vibrations occurs when there is a common atom between the two vibrating bonds. • Coupling of bending vibrations occur when there is a common bond between vibrating groups. 32
  • 33. • 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 33
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  • 35. FACTORS AFFECTING FREQUENCY OF IR ABSORPTION • Relative mass of the atom. • Force constant of the bonds. • Geometry of the atom. 35
  • 36. DEGREE OF FREEDOM • Fundamental vibration of molecule depend on degree of freedom. • Each atom has 3 degree of freedom depend on x, y, z. • For a molecule containing n no. of atoms has 3n degree of freedom. • For non – linear molecule, 3 degree of freedom represent rotational & transational motion. • For non-linear, ( 3n -6) degree of freedom represent fudamental vibrations. • For linear (3n-5) degree of freedom represent fundamental vibrations. • All vibrational changes don’t appear as band. • Only those vibrational changes that result in change in dipole moment appear as band. 36
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  • 39. SUMMARY • Absorption spectroscopy. • Vibrational transitions. • Applied infrared frequency = Natural frequency of vibration. • Structure elucidation to determine functional groups. 39
  • 40. REFERENCES 1. Spectrometric identification of organic compounds, sixth edition, Robert M. Silverstein & Francis X. Webster. Page no: 71 – 76 2. Principles of instrumental analysis, 6th edition, Douglas A. Skoog , E James Holler, Stanley R Crouch . Page no: 430 – 455 3. Introduction to spectroscopy, Donald L Pavia, Gary M. Lampman, James R. Vyvyan. Page no: 15 - 31 40