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Ultraviolet Spectroscopy

Ultraviolet Spectroscopy. Chapter 16, Smith (Pages 595-597). What is our approach to spectroscopy?. We will learn how to get the essential information from four kinds of spectroscopy and combine that information to deduce the structure of a compound.

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Ultraviolet Spectroscopy

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  1. Ultraviolet Spectroscopy Chapter 16, Smith (Pages 595-597)

  2. What is our approach to spectroscopy? • We will learn how to get the essential information from four kinds of spectroscopy and combine that information to deduce the structure of a compound. • The first kind is Ultraviolet Spectroscopy (UV).

  3. What is the most important thing to remember about spectroscopy? • That “spectroscopic data” is a physical property of molecules and that properties of molecules are a direct result of the structure of those molecules. • Thus, various forms of spectroscopy will give us “data” that reveals a little bit (i.e., partial structures) about the structure of a compound.

  4. How will we use this data? • We will correlate the spectroscopic data with specific partial structures. • We will find as many partial structures as possible from the data and then combine all of the partial structures into a complete structure of the only compound whose structure could produce the spectra we interpreted.

  5. What kind of data do we get? • In general, we get numbers (units). • Specific numbers reveal specific partial structures. • For example, the number 3400 cm-1 in an IR spectrum reveals the -OH group as a partial structure. • The number 3 over a signal at d = 2.0 in a 1H NMR spectrum reveals a methyl group next to a carbonyl group.

  6. Must I memorize dozens of numbers? • No, we hope to see enough examples so that you will become so familiar with the numbers that you know them much as you know your telephone number--not because you memorized the numbers but because you use them frequently enough that you simply remember them.

  7. What kinds of numbers are important for UV? • A constant with the Greek symbol epsilon (e), which tells us how much UV light a given compound absorbs. • Epsilon (e) is the molar absorptivity or molar extinction coefficient. • The value of e can vary from zero (no absorption of UV) to over 10,000 (very strong absorption)

  8. How do we characterize various values of epsilon? • Strong (e > 1000) • Weak (e < 100) • End absorption (e can’t be determined) • No absorption (e = 0)

  9. How do we use these four classifications of UV? • We associate or correlate partial structures with each of the four categories. • The next few slides will show these correlations.

  10. Partial structures:Strong UV (e > 1000) • Conjugated p systems--(alternating double bond--single bond--double bond) give e > 1000.

  11. If e > 1000, what kind of partial structure is indicated? • The compound MUST CONTAIN a conjugated p system. • It might be aromatic (like benzene). • It might be a conjugated polyene (like 1,3-butadiene).

  12. If a compound contains a conjugated p system what is e? • e must be > 1000

  13. Problem • A compound has a strong UV and the calculation of p + r for the compound is three. • What partial structure is present in the compound?

  14. Problem • A compound (C7H8) has e = 15,000. Draw the structure of the compound.

  15. Partial structures:Weak UV (e < 100) • Aldehydes or Ketones give e < 100

  16. If e < 100, what kind of partial structure is indicated? • The compound must have an aldehyde or ketone carbonyl. • There is no heteroatom next to the carbonyl carbon (only C or H).

  17. Given an aldehyde or ketone, what is e? • e < 100

  18. Problem • A compound (C4H8O) has e < 100. Draw two possible structures for the compound.

  19. Partial structures:UV End Absorption (No e) • Esters give end absorption.

  20. IfUV = end absorption, what partialstructure is indicated? • A carbonyl group with an Oxygen atom next to the carbonyl carbon is indicated. • An ester is a carbonyl with an O but not OH (acid) next to a carbonyl.

  21. Problem • A compound (C2H4O2) shows end absorption in its UV spectrum, what is its structure?

  22. Partial structures:No UV (inactive) • For CHM 201: UV = Wavelength l = 200-400 nm, the range of a typical instrument. • The UV absorption in such compounds as ethene lies outside the above region. • All partial structures, not covered in our strong, weak or end absorption categories will be considered inactive in the UV. (A ground rule, because of 200-400 nm)

  23. How is UV absorption measured? • A sample of a given concentration (C) in moles/liter = molarity, is placed in a 1 cm wide cuvette (pathlength L), and ultraviolet light, starting at a wavelength (l) of 400 nm and scanning down to 200 nm is passed thru. • The absorbance (A) is plotted vs wavelenth (l). • A is proportional to C x L for a compound that absorbs UV light.

  24. What info is recorded by the analyst? • The plot of A vs. l will have one or more maxima or lamda max (lmax). • The A value at each lmax is recorded. • Since A is proportional to C x L, the proportionality can be made an equation by inserting a proportionality constant e. • A = eCL (e is calculated and recorded for each lmax).

  25. Absorbance • The incident UV light = 1.00 • The compound absorbs some of it, say 80%. • The absorbance A is recorded as 0.80, because the compound absorbed 80% of the incident radiation. • A has no units; it’s a decimal.

  26. A typical calculation • Data: A = 0.815, L = 1 cm; C = 5.43 x 10-5 M; and l = 275 nm; solvent = cyclohexane • A = eCL; e = A/CL • e = (0.815)/(5.43 x 10-5 M)(1 cm) = 15,000 (no units); reported as e = 15,000, lmax = 275 nm (cyclohexane) • What kind of partial structure is indicated?

  27. How does UV work? • Loosely held p electrons in a given molecular orbital are excited into a higher energy molecular orbital by UV energy.

  28. p* Orbitals • An electron moves (transitions) from one orbital to an empty (unoccupied) orbital that normally is empty. • The name of the orbital where the electron winds up is always called p*. • The name of the orbital where the electron starts out is either a p or an n (n stands for nonbonding)

  29. Strong UV vs. Weak UV • Strong UV = p to p* transition • Weak UV = n to p* transition

  30. Molecular Orbital Theory • MO theory is a complementary theory to Valence-Shell-Electron-Pair-Replusion or VSEPR theory. • Every time two atomic orbitals overlap to make a bond, they make two new orbitals—a bonding and an antibonding orbital.

  31. Molecular Orbital Theory • Electrons normally fill bonding orbitals. • The antibonding orbitals (*) are normally empty of electrons, because they are of high energy and there is no net bonding in these orbitals. • The theory is most applicable to p bonds in organic chemistry.

  32. Summary • Strong UV, e > 1000, (conj p sys) mostly aromatic (like benzene) • Weak UV, e < 100, (aldehyde or ketone) • End Absorption, no e (ester) • No UV (everything else) • e = constant (defined, no units)

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