Chapter 2b IR Spectroscopy
2.1 Introduction to Infrared Absorption Spectroscopy
Infrared absorption spectroscopy involves the absorption of radiation in the infrared range.
It is a widely used method to investigate the structures of organic substances.
The instrument used is called an infrared spectrophotometer.
Typical range: 2.5 µm (4000 cm<sup>-1</sup>) to 17.2 µm (580 cm<sup>-1</sup>).
Near infrared: Below 2.5 µm.
Far infrared: Above 17.2 µm.
Organic molecules typically absorb in the mid-infrared region.
Absorption bands can be referred to by wavelength (µm) or wave number (cm<sup>-1</sup>).
Band intensity is expressed in absorbance (A) or transmittance (T); related as A = log(1/T).
2.2 Basic Theory of IR Spectroscopy
2.2.1 Molecular Vibrations
Molecules undergo continuous rotation and vibrations.
Comparisons can be made with a weightless spring connecting two balls (atoms).
Two main types of molecular vibrations:
Stretching Vibrations
Diatomic Molecules: Periodic compression and extension along the bond.
Triatomic or Higher Molecules:
Symmetric Stretching: Atoms move together in the same direction around a central atom.
Asymmetric Stretching: One atom approaches the center while another moves away.
Bending Vibrations
Changes in bond angles between non-linked atoms.
Types include:
Scissoring: In-plane bending.
Rocking: In-plane bending in the same direction.
Wagging: Out-of-plane bending.
Twisting: One atom moves above while the other moves below.
Bending vibrations require less energy than stretching vibrations.
2.2.3 Origin of IR Modes
Infrared spectra arise from the quantization of vibrational energy levels.
A molecule absorbs infrared radiation that matches the energy required for specific vibrational transitions.
The absorption wavelengths depend on the vibrational energy levels.
2.3 Calculation of Vibrational Frequency: Hooke's Law
The force constant (k) relates to bond strength; higher k = stronger bonds.
Formula: v = (1/2π)√(k/μ)
μ = reduced mass of the diatomic system equation: μ = (m1*m2)/(m1+m2)
Using Hooke's law, vibrational frequency can be approximated for single bonds.
Factors Affecting Vibrational Frequency
Atom Mass: Lower mass = higher frequency.
Force Constant (k): Higher k (stronger bond) = higher frequency.
Dipole Moment: Intensity of absorption is influenced by the bond's polarity.
2.4 Number of Fundamental Vibrations
Fundamental vibrational modes depend on molecule geometry:
Non-linear polyatomic: 3n - 6 modes.
Linear polyatomic: 3n - 5 modes.
Presence of weak vibrations and overlaps may lead to fewer observable bands.
2.5 Selection Rules
For infrared activity, vibrations must result in a change in dipole moment.
Symmetric stretches of centro-symmetric molecules do not exhibit IR activity.
2.6 Position and Intensity of Bands
2.6.1 Position of Absorption Bands
The position reflects bond character; distinct bands correspond to specific functional groups.
Divided into functional group region (2.5 to 8 µm) and fingerprint region (below 8 µm).
2.6.2 Intensity of Absorption Bands
Depends on the character of bonds and change in dipole moments.
Increased band intensity is often a function of higher dipole moments in stronger polar bonds.
2.7 Factors Influencing Vibrational Frequency
1. Electronic Effect
Inductive effects and resonance can modify bond strength.
Higher inductive effects usually lower the force constant, affecting frequency.
Conjugation can lead to decreased frequency shifts due to increased bond length.
2. Hydrogen Bonding
Strength of hydrogen bonds alters the absorption frequencies:
Strong hydrogen bonding causes shifts to lower wave number.
Broadening observed in intermolecular bonding; sharper bands in intramolecular.
2.8 Instrumentation: Mechanics of Recording IR Spectra
Parts of an infrared spectrophotometer:
Source, sample containers, monochromator, detector, recorder.
Common infrared sources: Nernst glower, silicon carbide (Globar).
FT-IR spectrometer provides better sensitivity and faster recording times.
2.9 Characteristic Absorption Regions of Various Bonds
Correlation tables show expected frequencies and intensities for various bonds and functional groups.
2.10 Spectral Features of Some Classes of Compounds
2.10.1 Hydrocarbons
Alkanes: Peaks at 2960-2850 cm<sup>-1</sup> (C-H stretching).
Alkenes: Vinylic C-H at 3000 cm<sup>-1</sup>.
Alkynes: Strong C-H stretching near 3300 cm<sup>-1</sup>; weak C≡C at 2100-2260 cm<sup>-1</sup>.
2.10.2 Functional Group Identification
Alcohols: O-H stretching at 3640-3610 cm<sup>-1</sup> (free), 3400-3200 cm<sup>-1</sup> (hydrogen bonded).
Aldehydes: C=O stretching at 1740-1720 cm<sup>-1</sup>.
Ketones: Lower frequency for C=O than aldehydes.
Carboxylic Acids: Broad O-H stretching at 3000-2500 cm<sup>-1</sup>.
2.11 Interpretation of IR Spectra
2.11.1 Specific Absorption Regions
Absorption bands categorized for quick identification based on frequency.
2.11.2 Practical Tips
Begin with high-frequency bands and use absence of bands as a tool for identification.
2.12 Applications of Infrared Spectroscopy
Identification of organic compounds, functional groups, reaction progress, purity assessment.
Example Interpretations
Example 2.2: Expected Absorption for Compounds
Isopropyl alcohol: O-H stretching (3200-3400 cm<sup>-1</sup>), C-H stretching (2850-2950 cm<sup>-1</sup>).
Dimethyl ether: C-O stretching (1060-1150 cm<sup>-1</sup>).
Toluene: C-H stretching (3000-3100 cm<sup>-1</sup>).
Example 2.3: Absorption Bands for Carbonyl Compounds
Approximate positions highlighted for carbonyl stretching in aldehydes and ketones.