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UV / VISIBLE SPECTROSCOPY

         Mr. Santosh M. Damkondwar
                     January 21, 2013
Spectroscopy
• It is the branch of science that deals with the
  study of interaction of matter with light.
                        OR
• It is the branch of science that deals with the
  study of interaction of electromagnetic
  radiation with matter.
Electromagnetic
Radiation
Electromagnetic Radiation
• Electromagnetic radiation consist of discrete
  packages of energy which are called as
  photons.

• A photon consists of an oscillating electric field
  (E) & an oscillating magnetic field (M) which
  are perpendicular to each other.
Electromagnetic Radiation
• Frequency (ν):
  – It is defined as the number of times electrical field
    radiation oscillates in one second.
  – The unit for frequency is Hertz (Hz).
                 1 Hz = 1 cycle per second


• Wavelength (λ):
  – It is the distance between two nearest parts of the
    wave in the same phase i.e. distance between two
    nearest crest or troughs.
Electromagnetic Radiation




• The relationship between wavelength &
  frequency can be written as:
                     c=νλ
• As photon is subjected to energy, so
              E=hν=hc/λ
Electromagnetic Radiation
Electromagnetic Radiation




Violet   400 - 420 nm Yellow   570 - 585 nm
Indigo   420 - 440 nm Orange   585 - 620 nm
Blue     440 - 490 nm Red      620 - 780 nm
Green    490 - 570 nm
Principles of
Spectroscopy
Principles of Spectroscopy
• The principle is based on the measurement of
  spectrum of a sample containing atoms /
  molecules.

• Spectrum is a graph of intensity of absorbed or
  emitted radiation by sample verses frequency
  (ν) or wavelength (λ).

• Spectrometer is an instrument design to
  measure the spectrum of a compound.
Principles of Spectroscopy
1. Absorption Spectroscopy:
• An analytical technique which concerns with
  the    measurement of       absorption   of
  electromagnetic radiation.

• e.g. UV (185 - 400 nm) / Visible (400 - 800 nm)
  Spectroscopy, IR Spectroscopy (0.76 - 15 μm)
Principles of Spectroscopy
2. Emission Spectroscopy:
  • An analytical technique in which emission
    (of a particle or radiation) is dispersed
    according to some property of the emission
    & the amount of dispersion is measured.

  • e.g. Mass Spectroscopy
Interaction of
EMR               with
                 Matter
Interaction of EMR with matter
1. Electronic Energy Levels:
• At room temperature the molecules are in the
  lowest energy levels E0.

• When the molecules absorb UV-visible light
  from EMR, one of the outermost bond / lone
  pair electron is promoted to higher energy
  state such as E1, E2, …En, etc is called as
  electronic transition and the difference is as:
  ∆E = h ν = En - E0 where (n = 1, 2, 3, … etc)
  ∆E = 35 to 71 kcal/mole
Interaction of EMR with matter
2. Vibrational Energy Levels:
• These are less energy level than electronic
  energy levels.

• The spacing between energy levels are
  relatively small i.e. 0.01 to 10 kcal/mole.

• e.g. when IR radiation is absorbed, molecules
  are excited from one vibrational level to
  another or it vibrates with higher amplitude.
Interaction of EMR with matter
3. Rotational Energy Levels:
• These energy levels are quantized & discrete.

• The spacing between energy levels are even
  smaller than vibrational energy levels.

       ∆Erotational < ∆Evibrational < ∆Eelectronic
Lambert’s
Law
Lambert’s Law
• When a monochromatic radiation is passed
  through a solution, the decrease in the
  intensity of radiation with thickness of the
  solution is directly proportional to the
  intensity of the incident light.

• Let I be the intensity of incident radiation.
      x be the thickness of the solution.
   Then
Lambert’s Law
                    dI
                        I
                    dx
                    dI
        So,              KI
                    dx
    Integrate equation between limit
                 I = Io at x = 0 and
                    I = I at x=l,
    We get,
                    I
           ln              Kl
                I0
Lambert’s Law
                         I
      2 . 303 log                Kl
                         I0
            I                  K
      log                            l
            I0               2 . 303
                  I0
   Where, log             A           Absorbance
                     I
                 K
                          E       Absorption coefficient
             2 . 303

                 A  E .l              Lambert’s Law
Beer’s
Law
Beer’s Law
• When a monochromatic radiation is passed
  through a solution, the decrease in the
  intensity of radiation with thickness of the
  solution is directly proportional to the
  intensity of the incident light as well as
  concentration of the solution.

• Let I be the intensity of incident radiation.
      x be the thickness of the solution.
       C be the concentration of the solution.
   Then
Beer’s Law
                     dI
                          C .I
                     dx
                     dI
         So,              K ' C .I
                     dx
     Integrate equation between limit
                  I = Io at x = 0 and
                     I = I at x=l,
     We get,
                     I
            ln              K ' C .l
                     I0
Beer’s Law
                           I0
         2 . 303 log             K .C .l
                           I
                I0              K
         log                        C .l
                I          2 . 303

    Where, log I 0  A                      Absorbance
                       I
               K                            Molar extinction
                        E
             2 . 303                        coefficient
           A  E .C .l                      Beer’s Law
Beer’s Law
                  A  E .C .l

             I                          I
      T         OR  log T  log             A
            I0                          I0

      From the equation it is seen that the absorbance
which is also called as optical density (OD) of a solution
in a container of fixed path length is directly
proportional to the concentration of a solution.
PRINCIPLES OF
UV - VISIBLE
SPECTROSCOPY
Principle
• The UV radiation region extends from 10 nm
  to 400 nm and the visible radiation region
  extends from 400 nm to 800 nm.
      Near UV Region: 200 nm to 400 nm
         Far UV Region: below 200 nm
• Far UV spectroscopy is studied under vacuum
  condition.
• The common solvent used for preparing
  sample to be analyzed is either ethyl alcohol
  or hexane.
Electronic
Transitions
The possible electronic   transitions   can
graphically shown as:
The possible electronic transitions are

   1     • σ → σ* transition
   2     • π → π* transition

   3     • n → σ* transition

   4     • n → π* transition

   5     • σ → π* transition

   6     • π → σ* transition
1     • σ → σ* transition

• σ electron from orbital is excited to
  corresponding anti-bonding orbital σ*.

• The energy required is large for this
  transition.

• e.g. Methane (CH4) has C-H bond only and
  can undergo σ → σ* transition and shows
  absorbance maxima at 125 nm.
2      • π → π* transition

• π electron in a bonding orbital is excited to
  corresponding anti-bonding orbital π*.

• Compounds containing multiple bonds like
  alkenes, alkynes, carbonyl, nitriles, aromatic
  compounds, etc undergo π → π* transitions.

• e.g. Alkenes generally absorb in the region
  170 to 205 nm.
3      • n → σ* transition

• Saturated compounds containing atoms with
  lone pair of electrons like O, N, S and
  halogens are capable of n → σ* transition.

• These transitions usually requires less energy
  than σ → σ* transitions.

• The number of organic functional groups
  with n → σ* peaks in UV region is small (150
  – 250 nm).
4     • n → π* transition

• An electron from non-bonding orbital is
  promoted to anti-bonding π* orbital.

• Compounds containing double bond
  involving hetero atoms (C=O, C≡N, N=O)
  undergo such transitions.

• n → π* transitions require minimum energy
  and show absorption at longer wavelength
  around 300 nm.
5      • σ → π* transition
 &      • π → σ* transition                  6
• These electronic transitions are forbidden
  transitions & are only theoretically possible.

• Thus, n → π* & π → π* electronic transitions
  show absorption in region above 200 nm
  which    is   accessible   to     UV-visible
  spectrophotometer.

• The UV spectrum is of only a few broad of
  absorption.
Terms used
in
UV / Visible
Spectroscopy
Chromophore
The part of a molecule responsible for imparting
color, are called as chromospheres.
                         OR
The functional groups containing multiple bonds
capable of absorbing radiations above 200 nm
due to n → π* & π → π* transitions.

e.g. NO2, N=O, C=O, C=N, C≡N, C=C, C=S, etc
Chromophore
To interpretate UV – visible spectrum following
points should be noted:

1. Non-conjugated alkenes show an intense
   absorption below 200 nm & are therefore
   inaccessible to UV spectrophotometer.

2. Non-conjugated carbonyl group compound
   give a weak absorption band in the 200 - 300
   nm region.
Chromophore
e.g.      O
               Acetone which has λmax = 279 nmO
          C
   H 3C       CH3

and that cyclohexane has λmax = 291 nm.

     When double bonds are conjugated in a
compound λmax is shifted to longer wavelength.
e.g. 1,5 - hexadiene has λmax = 178 nm
     2,4 - hexadiene has λmax = 227 nm
                    CH 2                  CH 3
H 2C                       H 3C
Chromophore
3. Conjugation of C=C and carbonyl group shifts
   the λmax of both groups to longer wavelength.
e.g. Ethylene has λmax = 171 nm
                                   O
     Acetone has λmax = 279 nm
                                    C
     H 2C   CH 2             H 3C       CH3

      Crotonaldehyde has λmax = 290 nm
                       O

               H 2C    C
                           CH3
Auxochrome
The functional groups attached to a
chromophore which modifies the ability of the
chromophore to absorb light , altering the
wavelength or intensity of absorption.
                       OR
The functional group with non-bonding electrons
that does not absorb radiation in near UV region
but when attached to a chromophore alters the
wavelength & intensity of absorption.
Auxochrome
e.g. Benzene λmax = 255 nm

                             OH



     Phenol λmax = 270 nm

                             NH2


     Aniline λmax = 280 nm
Absorption
& Intensity
Shifts
1 • Bathochromic Shift (Red Shift)
• When absorption maxima (λmax) of a
  compound shifts to longer wavelength, it is
  known as bathochromic shift or red shift.

• The effect is due to presence of an auxochrome
  or by the change of solvent.

• e.g. An auxochrome group like –OH, -OCH3
  causes absorption of compound at longer
  wavelength.
1 • Bathochromic Shift (Red Shift)
• In alkaline medium, p-nitrophenol shows red
  shift. Because negatively charged oxygen
  delocalizes more effectively than the unshared
  pair of electron.
                           -                                    -
           O       +
                       O                        O       +   O
               N                                    N

                                      -
                                 OH

                               A lk a lin e

                               m e d iu m               -
               OH                                   O

        p-nitrophenol
        λmax = 255 nm                         λmax = 265 nm
2 • Hypsochromic Shift (Blue Shift)
• When absorption maxima (λmax) of a
  compound shifts to shorter wavelength, it is
  known as hypsochromic shift or blue shift.


• The effect is due to presence of an group
  causes removal of conjugation or by the
  change of solvent.
2 • Hypsochromic Shift (Blue Shift)
• Aniline shows blue shift in acidic medium, it
  loses conjugation.

                                              +        -
             NH2           +         NH   3       Cl
                       H

                   A c id ic

                   m e d iu m

         Aniline
       λmax = 280 nm            λmax = 265 nm
3 • Hyperchromic Effect
• When absorption intensity (ε) of a compound is
  increased, it is known as hyperchromic shift.

• If    auxochrome introduces          to    the
  compound, the intensity of          absorption
  increases.

           N                      N     CH3



        Pyridine          2-methyl pyridine
    λmax = 257 nm           λmax = 260 nm
4    • Hypochromic Effect

• When absorption intensity (ε) of a compound is
  decreased, it is known as hypochromic shift.



                                          CH3

      Naphthalene        2-methyl naphthalene
       ε = 19000              ε = 10250
Shifts and Effects
                           Hyperchromic shift



                   Blue                         Red
Absorbance ( A )




                   shift                        shift



                           Hypochromic shift

                                   λmax
                             Wavelength ( λ )
APPLICATIONS OF
UV / VISIBLE
SPECTROSCOPY
Applications
• Qualitative & Quantitative Analysis:
  – It is used for characterizing aromatic compounds
    and conjugated olefins.
  – It can be used to find out molar concentration of the
    solute under study.
• Detection of impurities:
  – It is one of the important method to detect
    impurities in organic solvents.
• Detection of isomers are possible.
• Determination of molecular weight using Beer’s
  law.
REFERENCES
Reference Books
• Introduction to Spectroscopy
  – Donald A. Pavia


• Elementary Organic Spectroscopy
  – Y. R. Sharma


• Physical Chemistry
  – Puri, Sharma & Pathaniya
Resources
• http://www2.chemistry.msu.edu/faculty/reu
  sch/VirtTxtJml/Spectrpy/UV-
  Vis/spectrum.htm

• http://en.wikipedia.org/wiki/Ultraviolet%E2
  %80%93visible_spectroscopy

• http://teaching.shu.ac.uk/hwb/chemistry/tut
  orials/molspec/uvvisab1.htm

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UV visible spectroscopy

  • 1. UV / VISIBLE SPECTROSCOPY Mr. Santosh M. Damkondwar January 21, 2013
  • 2. Spectroscopy • It is the branch of science that deals with the study of interaction of matter with light. OR • It is the branch of science that deals with the study of interaction of electromagnetic radiation with matter.
  • 4. Electromagnetic Radiation • Electromagnetic radiation consist of discrete packages of energy which are called as photons. • A photon consists of an oscillating electric field (E) & an oscillating magnetic field (M) which are perpendicular to each other.
  • 5.
  • 6. Electromagnetic Radiation • Frequency (ν): – It is defined as the number of times electrical field radiation oscillates in one second. – The unit for frequency is Hertz (Hz). 1 Hz = 1 cycle per second • Wavelength (λ): – It is the distance between two nearest parts of the wave in the same phase i.e. distance between two nearest crest or troughs.
  • 7. Electromagnetic Radiation • The relationship between wavelength & frequency can be written as: c=νλ • As photon is subjected to energy, so E=hν=hc/λ
  • 9. Electromagnetic Radiation Violet 400 - 420 nm Yellow 570 - 585 nm Indigo 420 - 440 nm Orange 585 - 620 nm Blue 440 - 490 nm Red 620 - 780 nm Green 490 - 570 nm
  • 11. Principles of Spectroscopy • The principle is based on the measurement of spectrum of a sample containing atoms / molecules. • Spectrum is a graph of intensity of absorbed or emitted radiation by sample verses frequency (ν) or wavelength (λ). • Spectrometer is an instrument design to measure the spectrum of a compound.
  • 12. Principles of Spectroscopy 1. Absorption Spectroscopy: • An analytical technique which concerns with the measurement of absorption of electromagnetic radiation. • e.g. UV (185 - 400 nm) / Visible (400 - 800 nm) Spectroscopy, IR Spectroscopy (0.76 - 15 μm)
  • 13. Principles of Spectroscopy 2. Emission Spectroscopy: • An analytical technique in which emission (of a particle or radiation) is dispersed according to some property of the emission & the amount of dispersion is measured. • e.g. Mass Spectroscopy
  • 14. Interaction of EMR with Matter
  • 15. Interaction of EMR with matter 1. Electronic Energy Levels: • At room temperature the molecules are in the lowest energy levels E0. • When the molecules absorb UV-visible light from EMR, one of the outermost bond / lone pair electron is promoted to higher energy state such as E1, E2, …En, etc is called as electronic transition and the difference is as: ∆E = h ν = En - E0 where (n = 1, 2, 3, … etc) ∆E = 35 to 71 kcal/mole
  • 16. Interaction of EMR with matter 2. Vibrational Energy Levels: • These are less energy level than electronic energy levels. • The spacing between energy levels are relatively small i.e. 0.01 to 10 kcal/mole. • e.g. when IR radiation is absorbed, molecules are excited from one vibrational level to another or it vibrates with higher amplitude.
  • 17. Interaction of EMR with matter 3. Rotational Energy Levels: • These energy levels are quantized & discrete. • The spacing between energy levels are even smaller than vibrational energy levels. ∆Erotational < ∆Evibrational < ∆Eelectronic
  • 19. Lambert’s Law • When a monochromatic radiation is passed through a solution, the decrease in the intensity of radiation with thickness of the solution is directly proportional to the intensity of the incident light. • Let I be the intensity of incident radiation. x be the thickness of the solution. Then
  • 20. Lambert’s Law dI  I dx dI So,   KI dx Integrate equation between limit I = Io at x = 0 and I = I at x=l, We get, I ln   Kl I0
  • 21. Lambert’s Law I 2 . 303 log   Kl I0 I K log   l I0 2 . 303 I0 Where, log  A Absorbance I K  E Absorption coefficient 2 . 303 A  E .l Lambert’s Law
  • 23. Beer’s Law • When a monochromatic radiation is passed through a solution, the decrease in the intensity of radiation with thickness of the solution is directly proportional to the intensity of the incident light as well as concentration of the solution. • Let I be the intensity of incident radiation. x be the thickness of the solution. C be the concentration of the solution. Then
  • 24. Beer’s Law dI   C .I dx dI So,   K ' C .I dx Integrate equation between limit I = Io at x = 0 and I = I at x=l, We get, I ln   K ' C .l I0
  • 25. Beer’s Law I0 2 . 303 log  K .C .l I I0 K log  C .l I 2 . 303 Where, log I 0  A Absorbance I K Molar extinction  E 2 . 303 coefficient A  E .C .l Beer’s Law
  • 26. Beer’s Law A  E .C .l I I T  OR  log T  log  A I0 I0 From the equation it is seen that the absorbance which is also called as optical density (OD) of a solution in a container of fixed path length is directly proportional to the concentration of a solution.
  • 27. PRINCIPLES OF UV - VISIBLE SPECTROSCOPY
  • 28. Principle • The UV radiation region extends from 10 nm to 400 nm and the visible radiation region extends from 400 nm to 800 nm. Near UV Region: 200 nm to 400 nm Far UV Region: below 200 nm • Far UV spectroscopy is studied under vacuum condition. • The common solvent used for preparing sample to be analyzed is either ethyl alcohol or hexane.
  • 30. The possible electronic transitions can graphically shown as:
  • 31. The possible electronic transitions are 1 • σ → σ* transition 2 • π → π* transition 3 • n → σ* transition 4 • n → π* transition 5 • σ → π* transition 6 • π → σ* transition
  • 32. 1 • σ → σ* transition • σ electron from orbital is excited to corresponding anti-bonding orbital σ*. • The energy required is large for this transition. • e.g. Methane (CH4) has C-H bond only and can undergo σ → σ* transition and shows absorbance maxima at 125 nm.
  • 33. 2 • π → π* transition • π electron in a bonding orbital is excited to corresponding anti-bonding orbital π*. • Compounds containing multiple bonds like alkenes, alkynes, carbonyl, nitriles, aromatic compounds, etc undergo π → π* transitions. • e.g. Alkenes generally absorb in the region 170 to 205 nm.
  • 34. 3 • n → σ* transition • Saturated compounds containing atoms with lone pair of electrons like O, N, S and halogens are capable of n → σ* transition. • These transitions usually requires less energy than σ → σ* transitions. • The number of organic functional groups with n → σ* peaks in UV region is small (150 – 250 nm).
  • 35. 4 • n → π* transition • An electron from non-bonding orbital is promoted to anti-bonding π* orbital. • Compounds containing double bond involving hetero atoms (C=O, C≡N, N=O) undergo such transitions. • n → π* transitions require minimum energy and show absorption at longer wavelength around 300 nm.
  • 36. 5 • σ → π* transition & • π → σ* transition 6 • These electronic transitions are forbidden transitions & are only theoretically possible. • Thus, n → π* & π → π* electronic transitions show absorption in region above 200 nm which is accessible to UV-visible spectrophotometer. • The UV spectrum is of only a few broad of absorption.
  • 37. Terms used in UV / Visible Spectroscopy
  • 38. Chromophore The part of a molecule responsible for imparting color, are called as chromospheres. OR The functional groups containing multiple bonds capable of absorbing radiations above 200 nm due to n → π* & π → π* transitions. e.g. NO2, N=O, C=O, C=N, C≡N, C=C, C=S, etc
  • 39. Chromophore To interpretate UV – visible spectrum following points should be noted: 1. Non-conjugated alkenes show an intense absorption below 200 nm & are therefore inaccessible to UV spectrophotometer. 2. Non-conjugated carbonyl group compound give a weak absorption band in the 200 - 300 nm region.
  • 40. Chromophore e.g. O Acetone which has λmax = 279 nmO C H 3C CH3 and that cyclohexane has λmax = 291 nm. When double bonds are conjugated in a compound λmax is shifted to longer wavelength. e.g. 1,5 - hexadiene has λmax = 178 nm 2,4 - hexadiene has λmax = 227 nm CH 2 CH 3 H 2C H 3C
  • 41. Chromophore 3. Conjugation of C=C and carbonyl group shifts the λmax of both groups to longer wavelength. e.g. Ethylene has λmax = 171 nm O Acetone has λmax = 279 nm C H 2C CH 2 H 3C CH3 Crotonaldehyde has λmax = 290 nm O H 2C C CH3
  • 42. Auxochrome The functional groups attached to a chromophore which modifies the ability of the chromophore to absorb light , altering the wavelength or intensity of absorption. OR The functional group with non-bonding electrons that does not absorb radiation in near UV region but when attached to a chromophore alters the wavelength & intensity of absorption.
  • 43. Auxochrome e.g. Benzene λmax = 255 nm OH Phenol λmax = 270 nm NH2 Aniline λmax = 280 nm
  • 45.
  • 46. 1 • Bathochromic Shift (Red Shift) • When absorption maxima (λmax) of a compound shifts to longer wavelength, it is known as bathochromic shift or red shift. • The effect is due to presence of an auxochrome or by the change of solvent. • e.g. An auxochrome group like –OH, -OCH3 causes absorption of compound at longer wavelength.
  • 47. 1 • Bathochromic Shift (Red Shift) • In alkaline medium, p-nitrophenol shows red shift. Because negatively charged oxygen delocalizes more effectively than the unshared pair of electron. - - O + O O + O N N - OH A lk a lin e m e d iu m - OH O p-nitrophenol λmax = 255 nm λmax = 265 nm
  • 48. 2 • Hypsochromic Shift (Blue Shift) • When absorption maxima (λmax) of a compound shifts to shorter wavelength, it is known as hypsochromic shift or blue shift. • The effect is due to presence of an group causes removal of conjugation or by the change of solvent.
  • 49. 2 • Hypsochromic Shift (Blue Shift) • Aniline shows blue shift in acidic medium, it loses conjugation. + - NH2 + NH 3 Cl H A c id ic m e d iu m Aniline λmax = 280 nm λmax = 265 nm
  • 50. 3 • Hyperchromic Effect • When absorption intensity (ε) of a compound is increased, it is known as hyperchromic shift. • If auxochrome introduces to the compound, the intensity of absorption increases. N N CH3 Pyridine 2-methyl pyridine λmax = 257 nm λmax = 260 nm
  • 51. 4 • Hypochromic Effect • When absorption intensity (ε) of a compound is decreased, it is known as hypochromic shift. CH3 Naphthalene 2-methyl naphthalene ε = 19000 ε = 10250
  • 52. Shifts and Effects Hyperchromic shift Blue Red Absorbance ( A ) shift shift Hypochromic shift λmax Wavelength ( λ )
  • 53. APPLICATIONS OF UV / VISIBLE SPECTROSCOPY
  • 54. Applications • Qualitative & Quantitative Analysis: – It is used for characterizing aromatic compounds and conjugated olefins. – It can be used to find out molar concentration of the solute under study. • Detection of impurities: – It is one of the important method to detect impurities in organic solvents. • Detection of isomers are possible. • Determination of molecular weight using Beer’s law.
  • 56. Reference Books • Introduction to Spectroscopy – Donald A. Pavia • Elementary Organic Spectroscopy – Y. R. Sharma • Physical Chemistry – Puri, Sharma & Pathaniya
  • 57. Resources • http://www2.chemistry.msu.edu/faculty/reu sch/VirtTxtJml/Spectrpy/UV- Vis/spectrum.htm • http://en.wikipedia.org/wiki/Ultraviolet%E2 %80%93visible_spectroscopy • http://teaching.shu.ac.uk/hwb/chemistry/tut orials/molspec/uvvisab1.htm

Hinweis der Redaktion

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