2.13: Assignment of Bands Based on Solvent Effects
- Page ID
- 366290
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\(\newcommand{\avec}{\mathbf a}\) \(\newcommand{\bvec}{\mathbf b}\) \(\newcommand{\cvec}{\mathbf c}\) \(\newcommand{\dvec}{\mathbf d}\) \(\newcommand{\dtil}{\widetilde{\mathbf d}}\) \(\newcommand{\evec}{\mathbf e}\) \(\newcommand{\fvec}{\mathbf f}\) \(\newcommand{\nvec}{\mathbf n}\) \(\newcommand{\pvec}{\mathbf p}\) \(\newcommand{\qvec}{\mathbf q}\) \(\newcommand{\svec}{\mathbf s}\) \(\newcommand{\tvec}{\mathbf t}\) \(\newcommand{\uvec}{\mathbf u}\) \(\newcommand{\vvec}{\mathbf v}\) \(\newcommand{\wvec}{\mathbf w}\) \(\newcommand{\xvec}{\mathbf x}\) \(\newcommand{\yvec}{\mathbf y}\) \(\newcommand{\zvec}{\mathbf z}\) \(\newcommand{\rvec}{\mathbf r}\) \(\newcommand{\mvec}{\mathbf m}\) \(\newcommand{\zerovec}{\mathbf 0}\) \(\newcommand{\onevec}{\mathbf 1}\) \(\newcommand{\real}{\mathbb R}\) \(\newcommand{\twovec}[2]{\left[\begin{array}{r}#1 \\ #2 \end{array}\right]}\) \(\newcommand{\ctwovec}[2]{\left[\begin{array}{c}#1 \\ #2 \end{array}\right]}\) \(\newcommand{\threevec}[3]{\left[\begin{array}{r}#1 \\ #2 \\ #3 \end{array}\right]}\) \(\newcommand{\cthreevec}[3]{\left[\begin{array}{c}#1 \\ #2 \\ #3 \end{array}\right]}\) \(\newcommand{\fourvec}[4]{\left[\begin{array}{r}#1 \\ #2 \\ #3 \\ #4 \end{array}\right]}\) \(\newcommand{\cfourvec}[4]{\left[\begin{array}{c}#1 \\ #2 \\ #3 \\ #4 \end{array}\right]}\) \(\newcommand{\fivevec}[5]{\left[\begin{array}{r}#1 \\ #2 \\ #3 \\ #4 \\ #5 \\ \end{array}\right]}\) \(\newcommand{\cfivevec}[5]{\left[\begin{array}{c}#1 \\ #2 \\ #3 \\ #4 \\ #5 \\ \end{array}\right]}\) \(\newcommand{\mattwo}[4]{\left[\begin{array}{rr}#1 \amp #2 \\ #3 \amp #4 \\ \end{array}\right]}\) \(\newcommand{\laspan}[1]{\text{Span}\{#1\}}\) \(\newcommand{\bcal}{\cal B}\) \(\newcommand{\ccal}{\cal C}\) \(\newcommand{\scal}{\cal S}\) \(\newcommand{\wcal}{\cal W}\) \(\newcommand{\ecal}{\cal E}\) \(\newcommand{\coords}[2]{\left\{#1\right\}_{#2}}\) \(\newcommand{\gray}[1]{\color{gray}{#1}}\) \(\newcommand{\lgray}[1]{\color{lightgray}{#1}}\) \(\newcommand{\rank}{\operatorname{rank}}\) \(\newcommand{\row}{\text{Row}}\) \(\newcommand{\col}{\text{Col}}\) \(\renewcommand{\row}{\text{Row}}\) \(\newcommand{\nul}{\text{Nul}}\) \(\newcommand{\var}{\text{Var}}\) \(\newcommand{\corr}{\text{corr}}\) \(\newcommand{\len}[1]{\left|#1\right|}\) \(\newcommand{\bbar}{\overline{\bvec}}\) \(\newcommand{\bhat}{\widehat{\bvec}}\) \(\newcommand{\bperp}{\bvec^\perp}\) \(\newcommand{\xhat}{\widehat{\xvec}}\) \(\newcommand{\vhat}{\widehat{\vvec}}\) \(\newcommand{\uhat}{\widehat{\uvec}}\) \(\newcommand{\what}{\widehat{\wvec}}\) \(\newcommand{\Sighat}{\widehat{\Sigma}}\) \(\newcommand{\lt}{<}\) \(\newcommand{\gt}{>}\) \(\newcommand{\amp}{&}\) \(\definecolor{fillinmathshade}{gray}{0.9}\)Spectra of organic molecules containing \(n\) and \(π\) electrons can frequently be assigned based on their solvent effects.
Solvation
Solvents that do not itself absorb in the region under investigation are the most suitable for UV-visible spectroscopy. Most commonly used solvents are 95% EtOH, \(\ce{H2O}\) and hexane. Often, both the intensity (\(\varepsilon\)) and \(λ_{max}\) shift with the change of the polarity of the solvent. While all solutes species interact with the surrounding solvent molecules to affect the electronic energies of the electronic state, charged and dipolar molecules interact especially strongly often resulting in pronounced spectral shifts.
- Bathochromic shift: shift to longer \(\lambda\), also called red shift.
- Hypsochromic shift: shift to shorter \(\lambda\), also called blue shift.
- Hyperchromism: increase in \(\varepsilon\) of a band.
- Hypochromism: decrease in \(\varepsilon\) of a band.
The strength and nature of these interactions influence many properties of the solute including reaction rates. Solvation is the process of reorganizing solvent and solute molecules into solvation complexes and involves bond formation, hydrogen bonding, and van der Waals forces.
For compounds having \(n\), \(\pi\), and \(\pi^{*}\) orbitals (e.g. formaldyde), we can observe \(n \rightarrow \pi^{*}\) and \(\pi \rightarrow \pi^{*}\) transitions. The absorption wavelength \(n \rightarrow \pi^{*}\) of is typically longer than that of \(\pi \rightarrow \pi^{*}\) since the energy gap of \(n \rightarrow \pi^{*}\) is smaller than \(\pi \rightarrow \pi^{*}\). Different types of transition are affected differently with changes in polarity.
\(\sigma→\sigma^{*}\) Transitions (Neglible Shifts)
Molecules showing this type of transition are non-polar since \(\sigma\) MOs are non-polar in nature. Therefore, changing the polarity of solvents has neglibable effect on this transition. By increasing polarity of the solvent, compounds like hydrocarbons does not experience any appreciable shift. Thus, value of absorption maximum for non-polar compound is same in ethanol (polar) and hexane (non-polar).
\(\pi \rightarrow \pi ^*\) Transitions (Bathochromic Shifts)
In case of \(\pi \rightarrow \pi ^*\) transitions, the excited states are more polar than the ground state and the dipole-dipole interactions with solvent molecules lower the energy of the excited state more than that of the ground state. Therefore a polar solvent decreases the energy of \(\pi \rightarrow \pi ^*\) transition and absorption maximum appears ~10-20 nm red shifted in going from hexane to ethanol solvent.
For this type of transition, \(λ_{max}\) value shifts to longer wavelength with increasing polarity solvents. If the excited state is polar, but the ground state is neutral, polar solvent will primarily interact with the excited state to stabilizes it (decrease it absolute energy). Hence, absorption shifts to longer wavelength.
(CC BY-NC 4.0; Ümit Kaya via LibreTexts)
\(n \rightarrow \sigma^*\) Transitions (Hypsochromic Shifts)
If excited state is neutral and ground states are polar. Polar solvents will preferentially solvate the ground state to lower its energy. Hence, absorption shifts to shorter wavelength with increasing polarity of the solvent.
(CC BY-NC 4.0; Ümit Kaya via LibreTexts)
\(n \rightarrow \pi^{*}\) Transitions (Hypsochromic Shifts)
Similar to \(n \rightarrow \sigma^{*}\) transitions, the value of \(λ_{max}\) shifts to shorter wavelength for this transition.
(CC BY-NC 4.0; Ümit Kaya via LibreTexts)
Influence of solvent on the UV bands (\(λ_{max}\)) of the \(n \rightarrow \pi^{*}\) and \(\pi \rightarrow \pi^{*}\) transitions of 4-methylpent-3-en-2-one is tabulate below.
Solvent | \(\pi \rightarrow \pi^{*}\) (nm) | \(n \rightarrow \pi^{*}\) (nm) |
---|---|---|
n-hexane | 230 | 327 |
ether | 230 | 326 |
ethanol | 237 | 315 |
water | 245 | 305 |
Note that the \(\pi \rightarrow \pi ^{*}\) increases wavelength (decreased excitation energy) and the \(n \rightarrow \pi ^{*}\) decreases wavelength (increases excitation energy).
Summary
In a polar solvent, the absorption of \(n \rightarrow \pi^{*}\) will shift to shorter wavelengths, while the \(\pi \rightarrow \pi^{*}\) will weakly (or not at all) shift to longer wavelengths because the polar solvent stabilizes these three orbitals in different extent, \(n > \pi^{*} > \pi\), since \(\pi^{*}\) orbitals are more polar than \(\pi\) orbital as polar solvent stabilizes polar substances more (see J. Chem. Phys. 121, 8435 (2004); doi:10.1063/1.1804957). Thus, as solvent polarity increases:
- \(\pi \rightarrow \pi ^{*}\) band shifts to longer \(λ_{max}\)
- \(n \rightarrow \sigma^{*}\) band shifts to shorter \(λ_{max}\)
- \(n \rightarrow \pi ^{*}\) band shifts to shorter \(λ_{max}\)