7.5 Infrared and UV-Vis Spectroscopy

Key Takeaways

  • Infrared (IR) spectroscopy measures quantized vibrational bond transitions (stretching and bending) that induce an oscillating net dipole moment; completely symmetric nonpolar stretches (e.g., trans-alkenes, O2, N2) lack dipole changes and are entirely IR-inactive.

  • Diagnostic IR absorption regions provide instant structural fingerprints: broad O-H stretches appear at 3200–3600 cm^-1 (alcohols) or 2500–3300 cm^-1 overlapping C-H (carboxylic acids), sharp N-H stretches at 3300 cm^-1 (doublet for primary amines, singlet for secondary), sharp intense C=O stretches at 1700–1750 cm^-1, and terminal alkynyl/nitrile stretches at 2200–2260 cm^-1.

  • Ultraviolet-Visible (UV-Vis) spectroscopy detects electronic excitations from the highest occupied molecular orbital (HOMO) to the lowest unoccupied molecular orbital (LUMO); extending pi-conjugation narrows the HOMO-LUMO energy gap, producing a bathochromic (red) shift toward longer absorption wavelengths (higher lambda_max).

Last updated: September 2026

7.5 Infrared and UV-Vis Spectroscopy

Note

Foundational Standard: Elucidating molecular architecture from physical data is one of the most heavily emphasized reasoning skills on the MCAT. Mastering spectroscopy requires treating spectra not as isolated empirical lists, but as quantum mechanical probes: IR detects vibrational dipole oscillations, UV-Vis evaluates electronic orbital gaps across conjugated π\pi-systems, and NMR (both 1H^1\text{H} and 13C^{13}\text{C}) maps local magnetic shielding governed by electron density and stereochemical connectivity.

Spectroscopy measures the interaction of electromagnetic radiation with matter. As photon energy spans the infrared, visible, ultraviolet, and radiofrequency spectra, distinct molecular transitions are excited: nuclear spins, electronic energy levels, and vibrational bond coordinates.


Infrared (IR) Spectroscopy: Principles, Dipole Requirements & Diagnostic Absorptions

Infrared radiation (4000−400 cm−14000-400\text{ cm}^{-1}, where wavenumber ν~=1/λ\tilde{\nu} = 1/\lambda) possesses energy corresponding to quantized vibrational transitions (stretching and bending) of covalent bonds.

Hooke's Law and Bond Vibrations

A vibrating covalent bond behaves approximately as a classical harmonic oscillator governed by Hooke's law:

ν~=12πckμ\tilde{\nu} = \frac{1}{2\pi c} \sqrt{\frac{k}{\mu}}

where kk is the bond force constant (bond strength) and μ\mu is the reduced mass of the bonded atom pair (μ=m1m2m1+m2\mu = \frac{m_1 m_2}{m_1 + m_2}):

  • Bond Strength (kk): Stronger bonds possess higher spring constants and vibrate at higher wavenumbers: triple bonds (C≡C\text{C}\equiv\text{C}, ≈2200 cm−1\approx 2200\text{ cm}^{-1}) vibrate at higher frequencies than double bonds (C=C\text{C}=\text{C}, ≈1650 cm−1\approx 1650\text{ cm}^{-1}), which in turn vibrate higher than single bonds (C−C\text{C}-\text{C}, ≈1000 cm−1\approx 1000\text{ cm}^{-1}).
  • Reduced Mass (μ\mu): Lighter atoms vibrate at higher wavenumbers. Bonds involving light hydrogen atoms (C−H\text{C}-\text{H}, O−H\text{O}-\text{H}, N−H\text{N}-\text{H}) have small reduced masses and absorb in the highest-energy region (2800−3600 cm−12800-3600\text{ cm}^{-1}).

The Dipole Moment Selection Rule

For a molecular vibration to absorb an infrared photon, the vibration must cause a change in the molecule's net electric dipole moment:

(dμdipoledx)≠0\left( \frac{d\mu_{\text{dipole}}}{dx} \right) \neq 0
  • Polar bonds (such as C=O\text{C}=\text{O} and O−H\text{O}-\text{H}) undergo massive dipole oscillations during stretching and produce exceptionally intense absorption bands.
  • Symmetrical nonpolar bonds—such as the internal triple bond of 2-butyne (CH3−C≡C−CH3\text{CH}_3-\text{C}\equiv\text{C}-\text{CH}_3), the double bond of trans-3-hexene, or homonuclear diatomics (O2\text{O}_2, N2\text{N}_2)—experience zero net change in dipole moment during symmetric stretching and are completely IR-inactive (silent on the spectrum).

The Two Spectral Domains

  1. Diagnostic Region (4000−1400 cm−14000-1400\text{ cm}^{-1}): Contains distinct stretching vibrations characteristic of specific functional groups. This is the primary region tested on the MCAT.
  2. Fingerprint Region (1400−600 cm−11400-600\text{ cm}^{-1}): Contains complex bending vibrations and single-bond skeleton movements unique to an individual compound, functioning as an unforgeable molecular fingerprint.

Key Diagnostic IR Stretching Frequencies

Functional Group BandWavenumber Range (cm−1\text{cm}^{-1})Appearance & ShapePhysical / Mechanistic Origin
Hydroxyl (Alcohol O−H\text{O}-\text{H})3200−3600 cm−13200-3600\text{ cm}^{-1}Broad, rounded "U-shape"Intermolecular hydrogen bonding broadens vibrational energy levels
Hydroxyl (Carboxylic Acid O−H\text{O}-\text{H})2500−3300 cm−12500-3300\text{ cm}^{-1}Extremely broad, ragged engulfing C−H\text{C}-\text{H}Stable hydrogen-bonded dimer formation shifts band downfield into C−H\text{C}-\text{H}
Amine / Amide (N−H\text{N}-\text{H})3300−3500 cm−13300-3500\text{ cm}^{-1}Sharp, moderate intensityPrimary (R-NH2\text{R-NH}_2): two peaks (symmetric/asymmetric); Secondary (R2NH\text{R}_2\text{NH}): one peak
spsp C−H\text{C}-\text{H} (Terminal Alkyne)≈3300 cm−1\approx 3300\text{ cm}^{-1}Sharp, narrowHigh ss-character (50%50\%) creates very strong, stiff C−H\text{C}-\text{H} bond
sp2sp^2 C−H\text{C}-\text{H} (Alkene / Aromatic)3010−3100 cm−13010-3100\text{ cm}^{-1}Sharp, just to the left of 3000 cm−13000\text{ cm}^{-1}33.3%33.3\% ss-character
sp3sp^3 C−H\text{C}-\text{H} (Aliphatic Alkyl)2850−2960 cm−12850-2960\text{ cm}^{-1}Sharp cluster, just to the right of 3000 cm−13000\text{ cm}^{-1}25%25\% ss-character (universal in organic compounds containing saturated carbons)
Aldehyde C−H\text{C}-\text{H} (Fermi Doublet)2720 and 2820 cm−12720\text{ and } 2820\text{ cm}^{-1}Two small, sharp "fang" peaksFermi resonance between C−H\text{C}-\text{H} stretch and carbonyl bending overtone
Nitrile (C≡N\text{C}\equiv\text{N}) & Alkyne (C≡C\text{C}\equiv\text{C})2200−2260 cm−12200-2260\text{ cm}^{-1}Sharp, narrow (C≡N\text{C}\equiv\text{N} is intense; C≡C\text{C}\equiv\text{C} is weak)Stiff triple bonds in an otherwise blank spectral window
Carbonyl (C=O\text{C}=\text{O})1650−1750 cm−11650-1750\text{ cm}^{-1}Very sharp, intense "V-shape"Massive dipole moment of polarized C=O\text{C}=\text{O} double bond
Alkene (C=C\text{C}=\text{C}) & Aromatic Ring1600−1680 cm−11600-1680\text{ cm}^{-1}Medium to weak sharp bandsAromatic rings typically show 2−32-3 sharp bands near 1450,1500,1600 cm−11450, 1500, 1600\text{ cm}^{-1}

Dissecting the Carbonyl Region (1650−1750 cm−11650-1750\text{ cm}^{-1})

The exact position of the carbonyl band reflects electronic resonance and inductive effects:

  • Esters (≈1735−1750 cm−1\approx 1735-1750\text{ cm}^{-1}): The electronegative alkoxy oxygen exerts an inductive electron-withdrawing effect that strengthens the C=O\text{C}=\text{O} σ\sigma-bond, shifting the frequency upward.
  • Aldehydes (≈1725 cm−1\approx 1725\text{ cm}^{-1}) and Ketones (≈1715 cm−1\approx 1715\text{ cm}^{-1}): Standard baseline carbonyl frequencies.
  • Carboxylic Acids (≈1710 cm−1\approx 1710\text{ cm}^{-1}): Sightly lower due to hydrogen-bonded dimer formation.
  • Conjugation Effect (Δν~≈−20 to −40 cm−1\Delta\tilde{\nu} \approx -20\text{ to }-40\text{ cm}^{-1}): When a carbonyl is conjugated with a C=C\text{C}=\text{C} double bond or an aromatic ring, delocalization of π\pi-electrons into the carbonyl weakens double-bond character (increasing single-bond character), shifting the absorption downward to 1680−1690 cm−11680-1690\text{ cm}^{-1}.
  • Amides (≈1650−1680 cm−1\approx 1650-1680\text{ cm}^{-1}): Heavy resonance donation from the nitrogen lone pair (40%40\% double-bond character in C−N\text{C}-\text{N}) severely weakens the C=O\text{C}=\text{O} double bond, shifting the stretching band down to ≈1650 cm−1\approx 1650\text{ cm}^{-1}.

Ultraviolet-Visible (UV-Vis) Spectroscopy & Electronic Conjugation

UV-Vis spectroscopy (200−800 nm200-800\text{ nm}) measures the absorption of light that promotes valence electrons from a lower-energy bonding or non-bonding orbital to a higher-energy antibonding molecular orbital.

Electronic Transitions and Molecular Orbitals

  • π→π∗\pi \to \pi^* Transitions: Occur in compounds containing π\pi-bonds (alkenes, alkynes, carbonyls, aromatics).
  • n→π∗n \to \pi^* Transitions: Occur when an atom with non-bonding lone pairs (O\text{O}, N\text{N}, S\text{S}) is adjacent to a π\pi-system (e.g., carbonyl compounds).
  • HOMO to LUMO: Light absorption promotes an electron from the Highest Occupied Molecular Orbital (HOMO) to the Lowest Unoccupied Molecular Orbital (LUMO). The absorbed wavelength is governed by Planck's relation:
ΔE=hcλmax\Delta E = \frac{hc}{\lambda_{\text{max}}}

Conjugation and the Bathochromic Shift

As the number of alternating single and double bonds (conjugated π\pi-system) increases:

  1. Orbital mixing creates an expanded set of delocalized molecular orbitals.
  2. The energy gap between the HOMO and LUMO (ΔE\Delta E) progressively narrows.
  3. Because wavelength is inversely proportional to energy (λ=hc/ΔE\lambda = hc/\Delta E), narrowing the gap causes λmax\lambda_{\text{max}} to shift to longer wavelengths.

Directional Spectral Shifts:

  • Bathochromic Shift (Red Shift): Shift of λmax\lambda_{\text{max}} to a longer wavelength (lower energy), caused by increased conjugation or polar solvent interactions.
  • Hypsochromic Shift (Blue Shift): Shift of λmax\lambda_{\text{max}} to a shorter wavelength (higher energy).
  • Hyperchromic Effect: An increase in molar absorptivity (peak intensity ε\varepsilon).
  • Hypochromic Effect: A decrease in molar absorptivity (peak intensity ε\varepsilon).

Biological Chromophores

  • Conjugation Leading to Visible Color: Isolated double bonds absorb in the deep UV (ethene absorbs at 171 nm171\text{ nm}). Butadiene absorbs at 217 nm217\text{ nm}. When conjugation extends to ≈8−11\approx 8-11 conjugated double bonds (as in β\beta-carotene, with 11 conjugated double bonds), ΔE\Delta E drops into the visible range: β\beta-carotene absorbs strongly in the blue region (λmax≈450 nm\lambda_{\text{max}} \approx 450\text{ nm}) and reflects the complementary wavelengths, appearing brilliant orange.
  • Protein Concentration (Beer-Lambert Law): The aromatic amino acids tryptophan and tyrosine possess conjugated indole and phenol rings that absorb UV light at 280 nm280\text{ nm}. Spectrophotometers exploit this absorption to determine protein concentration using the Beer-Lambert Law:
A=ε⋅b⋅cA = \varepsilon \cdot b \cdot c

where AA is absorbance, ε\varepsilon is molar absorptivity (M−1cm−1\text{M}^{-1}\text{cm}^{-1}), bb is cuvette path length (1 cm1\text{ cm}), and cc is molar concentration.

Test Your Knowledge

An unknown pure organic compound with the molecular formula C5H11NO produces a strong, sharp IR band at 1655 cm^-1 and a distinct doublet of moderate intensity at 3350 and 3450 cm^-1. No absorption is observed above 3500 cm^-1 or between 2200 and 2300 cm^-1. Which functional group is present in this molecule?

A

A secondary amine directly attached to a ketone.

B

A primary amide containing an unsubstituted -CONH2 functional group.

C

A carboxylic acid possessing an intramolecular hydrogen bond.

D

An aliphatic nitrile carrying a tertiary alcohol substituent.

Test Your Knowledge

A series of conjugated polyenes is analyzed via ultraviolet-visible (UV-Vis) spectroscopy: 1,3-butadiene, 1,3,5-hexatriene, and 1,3,5,7-octatetraene. As the number of conjugated double bonds increases across this homologous series, what happens to the HOMO-LUMO energy gap and the wavelength of maximum absorbance (lambda_max)?

A

The HOMO-LUMO gap expands because additional pi-bonding orbitals lower the ground-state energy, shifting lambda_max to shorter wavelengths (hypsochromic shift).

B

The HOMO-LUMO gap remains completely constant because molecular orbital energies are determined solely by carbon hybridization rather than chain length.

C

The HOMO-LUMO gap expands because electron-electron repulsion destabilizes the antibonding pi* orbitals, producing a hyperchromic blue shift.

D

The HOMO-LUMO gap narrows because greater orbital mixing brings the highest occupied and lowest unoccupied molecular orbitals closer in energy, shifting lambda_max to longer wavelengths (bathochromic shift).

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