CH437 CLASS 19

ULTRAVIOLET-VISIBLE SPECTROSCOPY 2

Synopsis. Effect of conjugation on spectra. Conjugated dienes, , -unsaturated carbonyl compounds and aromatic compounds.

Interpretation of UV Spectra: Effect of Conjugation on the UV-Visible Spectra of Conjugated Dienes

The lower the energy gap between the HOMO and LUMO, the lower the energy of the photon that is needed to promote the * transition, and hence the longer the wavelength.

Conjugation has the effect of lowering the HOMO-LUMO energy gap, so that extensively conjugated compounds can absorb in the visible region of the electromagnetic spectrum and they appear colored. As a first example, compare the MO diagrams for ethylene and 1,3-butadiene.

The most important transition is the HOMO-LUMO transition (* for ethylene and 2*3 for 1,3-butadiene). This corresponds to (max ~175 nm for ethylene and 217 nm for 1,3-butadiene, so clearly

conjugation closes the HOMO-LUMO energy gap and increase max (bathochromic shift), as shown below

This gives rise to the UV spectrum below, where absorbance is plotted against wavelength ().

Taking the argument further, compare 1,3-butadiene (max = 217 nm) and 1,3,5-hexatriene (max = 258 nm). From this UV spectral data, we can calculate the HOMO-LUMO energy gap as 553 kJ/mol and 465 kJ/mol for 1,3-butadiene and 1,3,5-hexatriene, respectively. The spectra below show the HOMO-LUMO (* type) transitions for conjugated dienes with up to five double bonds.

Colored Organic Compounds

Extension of conjugation can lead to such a low HOMO-LUMO energy gap that the molecule absorbs in visible region of the electromagnetic spectrum and the compound appears colored. Such an example is -carotene, with 11 conjugated double bonds: its UV/visible spectrum and structure are shown below.

When normal (“white”) light strikes –carotene, the wavelengths from 400 nm to 500 nm are absorbed, corresponding to green – blue, while other wavelengths are reflected or transmitted to our eyes. We see white light with green-blue removed and hence we perceive a yellow-orange color for –carotene.

Effect of Substituents

For conjugated systems, just as extension of conjugation influences max, so does the presence of substituents (auxochromes). This occurs through interaction of the main chromophore -system with either the non-bonded electrons of a heteroatom (conjugation) or the electrons bonded in a C-H group (hyperconjugation). Either way, the net result is an extension of the chromophore conjugated -system, and a concurrent decrease in the HOMO-LUMO energy gap, as shown below.

UV-Visible Spectra of , -Unsaturated Carbonyl Compounds

Two principal transitions are associated with the carbonyl group, the weak (forbidden) n* and the strong (allowed) * transitions, but the latter is below the cutoff points of solvents:

Substitution on the carbonyl group by an auxochrome with a lone pair of electrons (e.g. –NR2, -OR, NH2, -OH, or -X as in amides, esters, acids or acid halides) leads to a hypsochromic effect on the n* transition and a lesser bathochromic shift on the * transition, but latter nearly always remains below the solvent cutoff wavelength. The hypsochromic effect, due to inductive (-I) effects of the more highly electronegative nitrogen, oxygen or halogen atom, is illustrated for the n* transition of the acetyl (CH3-C=O) group, below.

If the carbonyl group is part of a conjugated system, both the n* and the * are shifted to longer wavelengths (bathochromic shifts) and the latter becomes much more intense (hyperchromic shift). The former transition eventually becomes hidden by the latter, as illustrated below, showing the UV-visible spectra of conjugated aldehydes (CH3-(CH=CH)n-CHO).

The diagram below (not drawn to scale) illustrates the influence of conjugation on the molecular oribital energies and corresponding changes in the wavelengths of the n* and particularly the * transition.

Substituents and other features influence the * transition of the basic chromophore in a predictable way. A study of these led to the formulation of empirical rules for ,-unsaturated carbonyl compounds by Woodward and Fieser (Class 20).

UV-Visible Spectra of Aromatic Compounds

Absorptions that result from transitions within the benzene chromophore are more complex than the MO system would suggest: three absorption bands are actually observed. These are at max ~ 184 nm (max ~ 47,000) (allowed), max ~ 202 nm (max ~ 7,400) (forbidden) and max ~ 255 nm (max ~ 230) (forbidden). The  MO system of benzene is shown below.

Symmetry effects, combined with electron-electron repulsions, result in modification of the energy levels (from the MO energy level diagram above) that are involved in the UV absorption spectrum of benzene. They are basically * transitions:

The A1gB2u transition gives rise to the low intensity “secondary band” at ~255 nm and the A1gB1u transition results in the higher intensity “primary band” at ~ 202 nm in benzene. Both these transitions are influenced by substituents on the benzene ring.

Electron releasing groups (donors) increase the max value of both primary and secondary bands (red shift or bathochromic shift), as well as max (hyperchromic shift). Electron withdrawing groups have the same effect on maxand max of the primary band, but effects on the secondary band are less pronounced. Influence on the primary band transition is caused by extension of the delocalized by aromatic -system because of interaction with molecular orbitals on the substituent group:

Influence of substituents is summarized in the table below.

Substituent / Primary / Secondary
max/nm / max/cm l mol-1 / max/nm / max/cm l mol-1
H / 203.5 / 7400 / 254 / 204
CH3 / 206.5 / 7000 / 261 / 225
Cl / 209.5 / 7400 / 263.5 / 190
Br / 210 / 7900 / 261 / 192
OH / 210.5 / 6200 / 270 / 1450
O- / 235 / 9400 / 287 / 2600
OCH3 / 217 / 6400 / 269 / 1480
NH2 / 230 / 8600 / 280 / 1430
NH3+ / 203 / 7500 / 254 / 169
CN / 224 / 13000 / 271 / 1000
CO2H / 230 / 11600 / 273 / 970
CO2- / 224 / 8700 / 268 / 560
COCH3 / 245.5 / 9800
CHO / 249.5 / 11400
NO2 / 268.5 / 7800

The spectra (max) of substituted benzoyl derivatives can be predicted by the use of Scott’s empirical rules (see Class 20).

Both the primary and secondary bands in the spectra of polynucear aromatic hydrocarbons are shifted to higher wavelength – even the lower wavelength primary band is shifted to wavelengths over 200 nm, readily accessible by standard UV instruments. The spectra of naphthalene and anthracene are shown below.