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:

    1. 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.

    2. 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

  1. Atom Mass: Lower mass = higher frequency.

  2. Force Constant (k): Higher k (stronger bond) = higher frequency.

  3. 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.