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UV-VIS Molecular Spectroscopy

UV-VIS Molecular Spectroscopy. Chapter 13-14 From 190 to 900 nm!. Reflection and Scattering Losses. LAMBERT-BEER LAW. Power of radiation after passing through the solvent. Power of radiation after passing through the sample solution. Absorption Variables. Beer’s law and mixtures.

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UV-VIS Molecular Spectroscopy

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  1. UV-VIS Molecular Spectroscopy Chapter 13-14 From 190 to 900 nm!

  2. Reflection and Scattering Losses

  3. LAMBERT-BEER LAW Power of radiation after passing through the solvent Power of radiation after passing through the sample solution

  4. Absorption Variables

  5. Beer’s law and mixtures • Each analyte present in the solution absorbs light! • The magnitude of the absorption depends on its e • A total = A1+A2+…+An • A total = e1bc1+e2bc2+…+enbcn • If e1 = e2 =en then simultaneous determination is impossible • Need nl’s where e’s are different to solve the mixture

  6. Assumptions Ingle and Crouch, Spectrochemical Analysis

  7. Deviations from Beer’s Law Successful at low analyte concentrations (0.01M)! High concentrations of other species may also affect

  8. A + C AC Chemical Equilibria Consider the equilibrium: If e is different for A and AC then the absorbance depends on the equilibrium. [A] and [AC] depend on [A]total.  A plot of absorbance vs. [A]total will not be linear.

  9. Instrumental deviation with polychromatic radiation

  10. Effects of Stray Light

  11. Instrument Noise

  12. Effects of Signal-to-Noise Bad at High T Bad at Low T

  13. Components of instrumentation: • Sources • Sample Containers • Monochromators • Detectors

  14. Components of instrumentation: • Sources: Agron,Xenon, Deuteriun, or Tungsten lamps • Sample Containers: Quartz, Borosilicate, Plastic • Monochromators: Quarts prisms and all gratings • Detectors: Pohotomultipliers

  15. SourcesDeuterium and hydrogen lamps (160 – 375 nm) D2 + Ee → D2* → D’ + D’’ + h Excited deuterium molecule with fixed quantized energy Dissociated into two deuterium atoms with different kinetic energies Ee = ED2* = ED’ + ED’’ + hv Ee is the electrical energy absorbed by the molecule. ED2* is the fixed quantized energy of D2*, ED’ and ED’’ are kinetic energy of the two deuterium atoms.

  16. SourcesTungsten lamps (350-2500 nm) Blackbody type , temperature dependent Why add I2 in the lamps? W + I2 → WI2 • Low limit: 350 nm • Low density • Glass envelope

  17. General Instrument Designs Single beam Requires a stabilized voltage supply

  18. General Instrument Designs Double Beam: Space resolved Need two detectors

  19. General Instrument Designs Double Beam: Time resolved

  20. Double Beam Instruments • Compensate for all but the most short term fluctuation in • radiant output of the source • Compensate drift in transducer and amplifier • Compensate for wide variations in source intensity with • wavelength

  21. Multi-channel Design

  22. Molar absorptivities • e = 8.7 x 10 19 P A • A: cross section of molecule in cm2 (~10-15) • P: Probability of the electronic transition (0-1) • P>0.1-1  allowable transitions • P<0.01  forbidden transitions Molecular Absorption • M + hn  M* (absorption 10-8 sec) • M*  M + heat(relaxation process) • M*  A+B+C (photochemical decomposition) • M*  M + hn (emission)

  23. Visible Absorption Spectra

  24. The absorption of UV-visible radiation generally results from excitation of bonding electrons. • can be used for quantitative and qualitative analysis

  25. Molecular orbital is the nonlocalized fields between atoms that are occupied by bonding electrons. (when two atom orbitals combine, either a low-energy bonding molecular orbital or a high energy antibonding molecular orbital results.) • Sigma () orbital The molecular orbital associated with single bonds in organic compounds • Pi () orbital The molecular orbital associated with parallel overlap of atomic P orbital. • n electrons No bonding electrons

  26. Molecular Transitions for UV-Visible Absorptions • What electrons can we use for these transitions?

  27. MO Diagram for Formaldehyde (CH2O) H C O H s = p = n =

  28. In these diagrams, one electron has been excited (promoted) from the n to * energy levels (non-bonding to anti-bonding). One is a Singlet excited state, the other is a Triplet. Singlet vs. triplet

  29. Type of Transitions • σ→σ* High energy required, vacuum UV range CH4:  = 125 nm • n →σ* Saturated compounds, CH3OH etc ( = 150 - 250 nm) • n →* and →* Mostly used!  = 200 - 700 nm

  30. Examples of UV-Visible Absorptions LOW!

  31. UV-Visible Absorption Chromophores

  32. Effects of solvents • Blue shift (n- p*) (Hypsocromic shift) • Increasing polarity of solvent  better solvation of electron pairs (n level has lower E) •  peak shifts to the blue (more energetic) • 30 nm (hydrogen bond energy) • Red shift (n- p* andp –p*) (Bathochromic shift) • Increasing polarity of solvent, then increase the attractive polarization forces between solvent and absorber, thus decreases the energy of the unexcited and excited states with the later greater •  peaks shift to the red • 5 nm

  33. UV-Visible Absorption Chromophores

  34. Typical UV Absorption Spectra Chromophores?

  35. Effects of Multiple Chromophores

  36. The effects of substitution Auxochrome function group Auxochrome is a functional group that does not absorb in UV region but has the effect of shifting chromophore peaks to longer wavelength as well As increasing their intensity.

  37. Now solvents are your “container” • They need to be transparent and do not erase the fine structure arising from the vibrational effects Polar solvents generally tend to cause this problem Same solvent must be Used when comparing absorption spectra for identification purpose.

  38. Summary of transitions for organic molecules • s s* transition in vacuum UV (single bonds) • n s* saturated compounds with non-bonding electrons • l ~ 150-250 nm • e ~ 100-3000 ( not strong) • n p*, p  p* requires unsaturated functional groups (eq. double bonds) most commonly used, energy good range for UV/Vis • l ~ 200 - 700 nm • n p* : e ~ 10-100 • p  p*: e ~ 1000 – 10,000

  39. List of common chromophores and their transitions

  40. Organic Compounds • Most organic spectra are complex • Electronic and vibration transitions superimposed • Absorption bands usually broad • Detailed theoretical analysis not possible, but semi-quantitative or qualitative analysis of types of bonds is possible. • Effects of solvent & molecular details complicate comparison

  41. Rule of thumb for conjugation If greater then one single bond apart - e are relatively additive (hyperchromic shift) - l constant CH3CH2CH2CH=CH2lmax= 184 emax = ~10,000 CH2=CHCH2CH2CH=CH2lmax=185 emax = ~20,000 If conjugated - shifts to higher l’s (red shift) H2C=CHCH=CH2lmax=217 emax = ~21,000

  42. Spectral nomenclature of shifts

  43. What about inorganics? • Common anions np* nitrate (313 nm), carbonate (217 nm) • Most transition-metal ions absorb in the UV/Vis region. • In the lanthanide and actinide series the absorption process results from electronic transitions of 4f and 5f electrons. • For the first and second transition metal series the absorption process results from transitions of 3d and 4d electrons. • The bands are often broad. • The position of the maxima are strongly influenced by the chemical environment. • The metal forms a complex with other stuff, called ligands. The presence of the ligands splits the d-orbital energies.

  44. Transition metal ions

  45. Charge-Transfer-Absorption A charge-transfer complex consists of an electron-donor group bonded to an electron acceptor. When this product absorbs radiation, an electron from the donor is transferred to an orbital that is largely associated with the acceptor. • Large molar absorptivity (εmax >10,000) • Many organic and inorganic complexes

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