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UV-Visible Spectroscopy
By: Asst. Prof. Sanjaykumar Uchibagle
1. Introduction
2. Absorption Law (Beers & Lamberts Law)
3. Theory of Electronic Spectroscopy
1. Types of Electronic Transitions (K, R, B, E Bands)
2. The Chromophore Concept
3. Auxochrome
4. Absorption and Intensity Shifts
a. Bathochromic effect. (Red Shift)
b. Hypsochromic shift (Blue Shift)
c. Hyperchromic effect (Abs Increase)
d. Hypochromic effect (Abs Decrease)
5. Effect of Temperature and Solvent on the Fineness
of Absorption Band.
6. Woodward-fieser Rules for Calculating Absorption
Maximum in Dienes
7. Instrumentation.
A. Light Source
b. Collimating System
c. Monochromator
d. Sample Holder
e. Detector.
1. Introduction
 light travels in the form of waves.
 These are characterized by their
wavelengths or frequencies or
wavenumbers.
 The emission or absorption of radiation is
quantised and each quantum of radiation
is called a photon.
 Wavelength. It is the distance between
the two adjacent crests (C—C) or troughs
(T—T) in a particular wave. It is denoted
by the letter (lambda). It can be
expressed in Angstrom units or in
millimicrons (mμ).
1 Å = 10–8 cm; 1 mμ = 10–7 cm.
 Spectroscopy is the branch of Science that deals with the study
of interaction of electromagnetic radiation with matter.
 Spectrometer is an instrument design to measure the spectrum
of a compound.
 Instrument used to measure the absorbance in UV (200- 400nm)
or Visible (400-800nm) region is called UV- Visible
Spectrophotometer.
 A Spectrophotometer records the degree of absorption by a
sample at different wavelengths and the resulting plot of
absorbance (A) versus wavelength (λ) is known as a Spectrum
2. Absorption Law (Beers & Lamberts Law)
Lambert’s Law : When a beam of monochromatic radiation passes
through a homogeneous absorbing medium, the rate of decrease of
intensity of radiation with thickness of absorbing medium is proportional
to the intensity of the incident radiation.
Mathematically, the law is expressed as
Where, I = intensity of radiation after passing through a thickness x, of the
medium.
= rate of decrease of intensity of radiation with thickness of the absorbing
medium
2. Absorption Law (Beers & Lamberts Law)
Beer’s Law : When a beam of monochromatic radiation is passed through
a solution of an absorbing substance, the rate of decrease of intensity of
radiation with thickness of the absorbing solution is proportional to the
intensity of incident radiation as well as the concentration of the solution.
Mathematically, this law is stated as
Where, c = conc. of the solution in moles litre–1.
k = molar absorption coefficient and its value depends upon the
nature of the absorbing substance
3. Theory of Electronic Spectroscopy
1. Molecule absorbs – UV light- its electrons - Ground state to the higher
energy state
2. In the higher energy state, if the spins of the electrons are paired,
called an excited singlet state.
3. On the other hand, if the spins of the electrons in the excited state
are parallel, it is called an excited triplet state.
The triplet state is always lower in energy than the corresponding excited
singlet state.
Therefore, triplet state is more stable as compared to the excited singlet
state
σ→σ* transitions.
1. It is a high energy
process since, bonds are, in
general, very strong.
2. The organic ompounds
in which all the valence
shell electrons are involved
in the formation of sigma
bonds do not show
absorption in the normal
ultra-violet region.
n→σ* transition.
This type of transition takes
place in saturated compounds
containing one hetero atom
with unshared pair of electrons
(n electrons).
π→π* transitions.
This type of transition occurs
in the unsaturated centers of
the molecule; i.e., in
compounds containing double
or triple bonds and also in
aromatics.
n→π* transition.
In this type of
transition, an electron
of unshared electron
pair on hetero atom
gets excited to π*
antibonding orbital.
(a) K* Bands.
1. K-bands originate due to π→π*
transition from a compound
containing a conjugated system.
2. Such type of bands arise in
compounds like dienes, polyenes,
enones.
3. K-bands also appear in an
aromatic compound which is
substituted by a chromophore.
4. The intensity of K-band, is
usually more than 104 .
5. The K-band absorption due to
conjugated ‘enes’ and ‘enones’ are
effected differently by changing
the polarity of the solvent
(b) R* band.
1. Such type of bands
originate due to n→π*
transition of a single
chromophoric group
and having at least one
lone pair of electrons on
the hetero atom.
2. R-bands are also
called forbidden bands.
These are less intense.
(c) B-band.
1. Such type of bands
arise due π→π*
transition in aromatic or
hetero-aromatic
molecules.
2. Benzene shows
absorption peaks between
230–270mμ.
3. When a chromophoric
group is attached to the
benzene ring, the B-bands
are observed at longer
wave-lengths than the
more intense K-bands.
(d) E-bands.
1. Such bands originate due to the electronic transitions in the benzenoid
system of three ethylenic bonds which are in closed cyclic conjugation.
2. These are further characterized as E1 and E2-bands. E1 and E2 bands of
benzene appear at 184 and 204 mμ respectively.
3. E1 band which appears at lower wave-length is usually more intense
than the E2-band for the same compound which appears at longer
wavelength.
3.2. The Chromophore Concept
1. It is defined as any isolated covalently
bonded group that shows a
characteristic absorption in the ultra-
violet or the visible region.
2. All those compounds which absorb
light of wavelength between 400-800
mμ appear coloured to the human eye.
3. Exact colour depends upon the
wavelength of light absorbed by the
compound
4. Nitro-compounds are generally yellow
in colour.
5. Similarly, aryl conjugated azo group is
a chromophore for providing colour to
azo dyes.
3.3. The Auxochrome Concept
1. An auxochrome can be defined as any group-which does not itself act as a chromophore
but whose presence brings about a shift of the absorption band towards the red end of
the spectrum (longer wavelength).
2. The absorption at longer wavelength is due to the combination of a chromophore and an
auxochrome to give rise to another chromophore.
3. An auxochromic group is called colour enhancing group.
4. Some common auxochromic groups are —OH, —OR, —NH2, —NHR, —NR2, —SH etc.
5. For example, benzene shows an absorption maximum at 255 mμ [Abs. max 203] whereas
aniline absorbs at 280 mμ [Abs max 1430]. Hence, amino (—NH2) group is an
auxochrome.
4. Absorption and Intensity Shifts
(a) Bathochromic effect/Red Shift
1. It is an effect by virtue of which the
absorption maximum is shifted towards
longer wavelength due to the presence of an
auxochrome or by the change of solvent.
2. Such an absorption shift towards longer
wavelength is called Red shift or
bathochromic shift.
3. For example, benzene shows an absorption
maximum at 255 mμ [Abs. max 203] whereas
aniline absorbs at 280 mμ [Abs max 1430].
Hence, amino (—NH2) group is an
auxochrome.
(b) Hypsochromic shift/Blue Shift
1. It is an effect by virtue of which the
absorption maximum is shifted towards
shorter wavelength..
2. The absorption shifted towards shorter
wavelength is called Blue shift or
hypsochromic shift
3. . In the case of aniline, absorption
maximum occurs at 280 mμ because the
pair of electrons on nitrogen atom is in
conjugation with the π bond system of the
benzene ring. In its acidic solutions, a blue
shift is caused and absorption occurs at
shorter wavelength (~203 mμ).
(c) Hyperchromic effect.
1. It is an effect due to which the
intensity of absorption maximum
increases.
2. The introduction of an auxochrome
usually increases intensity of absorption.
3.For example, benzene shows an
absorption maximum at 255 mμ [Abs.
max 203] whereas aniline absorbs at
280 mμ [Abs max 1430]. Hence, amino
(—NH2) group is an auxochrome.
(d) Hypochromic effect.
1 It is defined as an effect due to which the
intensity of absorption maximum
decreases.
2. For example, biphenyl absorbs at 250
mμ, Abs max 19000 whereas 2-methyl
biphenyl absorbs at 237 mμ, Abs max
10250
5. Effect of Temperature
1. It is known that the vibrational
and the rotational states
depend on temperature.
2. As the temperature is
decreased, vibrational and the
rotational energy state of the
molecules are also lowered.
3. Thus, when the absorption of
light occurs at a lower
temperature, smaller
distribution of excited states
result. It produces finer
structure in the absorption
band than what is noticed at
higher temperature.
1.The solvent used also
effects the fineness of
absorption band in UV
spectrum.
2.If the dielectric constant
of the solvent is high, there
will be stronger solute-
solvent interactions.
3.Due to this, vibrational
and rotational energy states
of molecules increase and
thus, the fineness of the
absorption band falls.
Solvent on the Fineness of Absorption
Band.
Solvent Effects
1. A most suitable solvent is one
which does not itself absorb in the
region under investigation.
2. A dilute solution of the sample is
always prepared for the spectral
analysis. Most commonly used
solvent is 95% Ethanol.
3. Ethanol is a best solvent as it is
cheap and is transparent down to
210 mμ.
4.Some other solvents which are
transparent above 210 mμ are n-
hexane, methyl alcohol, cyclohexane,
acetonitrile, diethyl ether etc
7. Instrumentation.
A. Light Source
b. Collimating System
c. Monochromator
d. Sample Holder
e. Detector.
Ideal Property of Source.
1. Stable
2. Not Fluctuating
3. Emit of light continuous &
Uniform Intensity for which its
Used.
4. It should not be fatigue on
continuous used.
For Visible Spectroscopy.
1. Tungsten Halogen Lamp
For UV Radiation.
1. Hydrogen Discharge Lamp.
2. Xenon Discharge Lamp.
3. Mercury Arc Lamp.
Light Source
For Visible Spectroscopy.
1. Tungsten Halogen Lamp
 Its Construction is similar to the house hold lamp.
 Bulb contains a filament of Tungsten fixed in evacuated condition &
then filled with inert gas.
 The filament can be heated up to 3000 k, beyond this this Tungsten
starts sublimating.
 It is used when polychromatic radiation is required. To prevent this
along with inert gas some amount of halogen is introduced. (usually
Iodine)
 Sublimated form of Tungsten is reacted with Iodine to form complex,
which migrate back to the hot filament.
 It provides a supply of radiation in the wavelength range of 320-
2500nm.
 Demerit- It emit the major portion of near IR region
Light Source
For UV Spectroscopy.
1. Hydrogen Discharge Lamp.
 In this pair of electrode is enclosed in a glass tube (provide with
silica or quartz for UV radiation to pass it) filled with hydrogen gas.
 When current is passed through the electrode maintained at high
voltage, discharge of electron occurs with excites hydrogen molecule
which in turn cause emission of UV radiation.
 They are stable and robust. Covers a range 160-375nm
Light Source
For UV Spectroscopy.
1. Xenon Discharge Lamp
 It possesses 2 tungsten electrode separated by some distance.
 This are enclosed in a glass tube with quartz / Fused Silica & Xenon
gas is filled under pressure.
 An intense arc is formed between electrode by applying high voltage.
 This is good source of continuous plus additional intense radiation.
Its intensity is higher than Hydrogen Discharge Lamp.
 Demerit: The lamp since operate at high voltage become very hot
during operation & hence need thermal insulation.
Light Source
For UV Spectroscopy.
1. Mercury Arc Lamp
 In Mercury arc lamp, mercury vapor is stored under high pressure &
excitation of mercury atom is done by electrical discharge.
 Demerit: Not suitable for continuous spectral studies because it
doesn’t give continuous radiations.
b. Collimating System
The radiation emitted by source is collimated (parallel) by lenses, mirror and slits.
Lenses:
 Material used for the lenses must be transparent to the radiation being used.
 Ordinary silicate glass transmits between 350 to 3000 nm & is suitable for visible
and near IR region.
 Quartz or fused silica is used as a material for lenses to work below 300 nm.
Mirrors:
 This are used to reflect, focus or collimating light beam in spectrophotometer.
 To minimize the light loss, mirror are aluminized on their surface
Slits:
 Important device in resolving polychromatic to monochromatic
radiation To achieve this entrance & Exit Slits are Used.
 The width of slit plays imp. role in resolution of polychromatic
radiation.
c. Monochromator
This device is used to isolate the radiation of desired wavelength from wavelength of
continuous spectra. Ex.
1. Filters
2. Prism
3. Grating.
1.Filters:
 Selection of filter is usually done on compromise between peak transaction &
band pass width; the former should be as high as possible & latter as narrow as
possible.
Absorption Filters: Works by selective absorption of unwanted radiation and
transmit the radiation which is required. Ex. Glass & Gelatin.
Selection of absorption filters is done according to the
following procedure.
 Draw a filter wheel.
 Write the color VIBGYOR in anticlockwise
 If solution to be analyzed is blue in color
filter having complimentary color
orange is to be used.
 Similarly we can select the required filters
in colorimeter, based upon the color of the solution
 An absorption glass filter is made of solid sheet of
glass that has been colored by pigment which is
dissolved or dispersed in the glass.
 The color in the glass filter is produce by incorporating metal oxide like
Cr, Mn, Fe, Ni, Co, Cu etc.
Gelatin filter is an example of absorption filter prepared by adding
organic pigments.
 Here instead of solid glass sheet thin gelatin sheet are used
 This are not used now days.
 It tends to be deteriorate to be time & glass affected by heat and
moisture The Color of dye gets bleached.
Merits:
1. Simple in construction.
2. Cheaper.
3. Selection of filter easy
Demerits:
1. Less Accurate.
2. Band pass (bandwidth) is ±30nm
If we have to measure the 400nm; we
get the radiation from 370-430 nm,
Less Accurate Results Obtained.
Interference filters:
 Work on the interference phenomenon cause rejection of unwanted
wavelength by selective reflection.
 It is constructed by using two parallel glass plate, which are silvered
internally & separated by thin film of dielectric material of different
(CaF2, SiO, MgF2) refractive index.
Merits:
1. These filters have band pass of 10-15 nm with peak transmittance of
40-60%.
2. Cheap
3. Additional filters can be used to cut off undesirable wavelength
2. Prism.
 Prism is made up from glass, quartz or fused silica.
 Quartz or fused silica is the choice of material for UV.
 When the light is pass through the glass prism, dispersion of
polychromatic light in RAINBOW occurs.
 Now by rotation of Prism in different wavelength of the spectrum can be
made to pass through the exit slit on the sample.
 The effective wavelength depends on the dispersive power of Prism
material & Optical Angle of the Prism.
There are two types of mounting in
an instrument
 one is called ‘Cornu type’
(refractive), which has an optical
angle of 60o and its adjusted such
that on rotation the emerging
light is allowed to fall on exit slit.
 The other type is called “Littrow type”
(reflective), which has optical angle 30o
and its one surface is aluminized with
reflected light back to pass through prism
and to emerge on the same side of the light
source i.e. light doesn’t pass through the
prism on other side.
Grating:
 Are most effective one in converting a polychromatic light to monochromatic
light. As a resolution of +/- 0.1nm could be achieved by using gratings, they
are commonly used in spectrophotometers.
 Gratings are of two types.
1. Diffraction grating. 2. Transmission gratings.
1. Diffraction grating.
 More refined dispersion of light is obtained by means of diffraction gratings.
 These consist of large number of parallel lines ( grooves) about 15000-30000/
inch is ruled on highly polished surface of aluminium.
 These gratings are replica made from master gratings by coating the original
master grating with a epoxy resin and are removed after setting
2. Transmission gratings.
 It is similar to diffraction grating but refraction takes place instead of
reflection.
 Refraction produces reinforcement. this occurs when radiation transmitted
through grating reinforces with the partially refracted radiation.
Advantages:
 Grating gives higher and linear dispersions compared to prism
monochromator.
 Can be used over wide wavelength ranges.
 Gratings can be constructed with materials like aluminium which is
resistant to atmospheric moisture.
 Provide light of narrow wavelength.
 No loss of energy due to absorption
d. Sample Holder
 The cells or cuvettes are used for handling liquid samples.
 The cell may either be rectangular or cylindrical in nature.
 For study in UV region; the cells are prepared from quartz or fused silica
whereas color corrected fused glass is used for visible region.
 The surfaces of absorption cells must be kept scrupulously clean. No
fingerprints or blotches should be present on cells.
 Cleaning is carried out washing with distilled water or with dilute alcohol,
acetone.
e. Detectors.
 Device which converts light energy into electrical signals,
that are displayed on readout devices.
 The transmitted radiation falls on the detector which
determines the intensity of radiation absorbed by sample The
following types of detectors are employed in instrumentation
of absorption spectrophotometer.
 1. Barrier layer cell/Photovoltaic cell
 2. Phototubes/ Photo emissive tube
 3. Photomultiplier tube
Ideal Properties of Detectors.
 It should give quantitative response.
 It should have high sensitivity and low noise level.
 It should have a short response time.
 It should provide signal or response quantitative to wide
spectrum of radiation received.
1. Barrier layer cell/Photovoltaic cell
 The detector has a thin film metallic layer coated with silver or gold
and acts as an electrode.
 It also has a metal base plate which acts as another electrode.
 These two layers are separated by a semiconductor layer of
selenium.
 When light radiation falls on selenium layer, electrons become
mobile and are taken up by transparent metal layer.
 This creates a potential difference between two electrodes & causes
the flow of current.
 When it is connected to galvanometer, a flow of current observed
which is proportional to the intensity and wavelength of light falling
on it.
2. Phototubes/ Photo emissive tube
 Consists of a evacuated glass tube with a photocathode and a
collector anode.
 The surface of photocathode is coated with a layer of elements like
cesium, silver oxide or mixture of them.
 When radiant energy falls on photosensitive cathode, electrons are
emitted which are attracted to anode causing current to flow.
 More sensitive compared to barrier layer cell and therefore widely
used.
 The principle employed in this detector is that, multiplication of
photoelectrons by secondary emission of electrons
 In a vacuum tube, a primary photo-cathode is fixed which receives
radiation from the sample.
 Some eight to ten dynodes are fixed each with increasing potential of
75-100V higher than preceding one.
 Near the last dynode is fixed an anode or electron collector electrode.
 Photo-multiplier is extremely sensitive to light and is best suited
where weaker or low radiation is received
3. Photomultiplier tube
 The principle employed in this detector is that,multiplication of
photoelectrones by secondary emission of electrons.
 In a vaccum tube a primary photo-cathode is fixed which receives
radiation from the sample.
 Some eight to 10 dynodes are fixed each with increasing potential of
75-100V higher than preceeding one.
 Photomultiplier is extremely sensitive to light and is best suited
where weaker or low radiation is received.
 Near the last dynode is fixed an anode or electrone collector
electrode.
3. Photomultiplier tube
DOUBLE BEAM SPECTROSCOPY
Thank You!

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UV-VISIBLE SPECTROSCOPY.pptx

  • 1. UV-Visible Spectroscopy By: Asst. Prof. Sanjaykumar Uchibagle
  • 2. 1. Introduction 2. Absorption Law (Beers & Lamberts Law) 3. Theory of Electronic Spectroscopy 1. Types of Electronic Transitions (K, R, B, E Bands) 2. The Chromophore Concept 3. Auxochrome 4. Absorption and Intensity Shifts a. Bathochromic effect. (Red Shift) b. Hypsochromic shift (Blue Shift) c. Hyperchromic effect (Abs Increase) d. Hypochromic effect (Abs Decrease)
  • 3. 5. Effect of Temperature and Solvent on the Fineness of Absorption Band. 6. Woodward-fieser Rules for Calculating Absorption Maximum in Dienes 7. Instrumentation. A. Light Source b. Collimating System c. Monochromator d. Sample Holder e. Detector.
  • 4. 1. Introduction  light travels in the form of waves.  These are characterized by their wavelengths or frequencies or wavenumbers.  The emission or absorption of radiation is quantised and each quantum of radiation is called a photon.  Wavelength. It is the distance between the two adjacent crests (C—C) or troughs (T—T) in a particular wave. It is denoted by the letter (lambda). It can be expressed in Angstrom units or in millimicrons (mμ). 1 Å = 10–8 cm; 1 mμ = 10–7 cm.
  • 5.
  • 6.  Spectroscopy is the branch of Science that deals with the study of interaction of electromagnetic radiation with matter.  Spectrometer is an instrument design to measure the spectrum of a compound.  Instrument used to measure the absorbance in UV (200- 400nm) or Visible (400-800nm) region is called UV- Visible Spectrophotometer.  A Spectrophotometer records the degree of absorption by a sample at different wavelengths and the resulting plot of absorbance (A) versus wavelength (λ) is known as a Spectrum
  • 7. 2. Absorption Law (Beers & Lamberts Law) Lambert’s Law : When a beam of monochromatic radiation passes through a homogeneous absorbing medium, the rate of decrease of intensity of radiation with thickness of absorbing medium is proportional to the intensity of the incident radiation. Mathematically, the law is expressed as Where, I = intensity of radiation after passing through a thickness x, of the medium. = rate of decrease of intensity of radiation with thickness of the absorbing medium
  • 8. 2. Absorption Law (Beers & Lamberts Law) Beer’s Law : When a beam of monochromatic radiation is passed through a solution of an absorbing substance, the rate of decrease of intensity of radiation with thickness of the absorbing solution is proportional to the intensity of incident radiation as well as the concentration of the solution. Mathematically, this law is stated as Where, c = conc. of the solution in moles litre–1. k = molar absorption coefficient and its value depends upon the nature of the absorbing substance
  • 9. 3. Theory of Electronic Spectroscopy 1. Molecule absorbs – UV light- its electrons - Ground state to the higher energy state 2. In the higher energy state, if the spins of the electrons are paired, called an excited singlet state. 3. On the other hand, if the spins of the electrons in the excited state are parallel, it is called an excited triplet state. The triplet state is always lower in energy than the corresponding excited singlet state. Therefore, triplet state is more stable as compared to the excited singlet state
  • 10. σ→σ* transitions. 1. It is a high energy process since, bonds are, in general, very strong. 2. The organic ompounds in which all the valence shell electrons are involved in the formation of sigma bonds do not show absorption in the normal ultra-violet region. n→σ* transition. This type of transition takes place in saturated compounds containing one hetero atom with unshared pair of electrons (n electrons). π→π* transitions. This type of transition occurs in the unsaturated centers of the molecule; i.e., in compounds containing double or triple bonds and also in aromatics. n→π* transition. In this type of transition, an electron of unshared electron pair on hetero atom gets excited to π* antibonding orbital.
  • 11. (a) K* Bands. 1. K-bands originate due to π→π* transition from a compound containing a conjugated system. 2. Such type of bands arise in compounds like dienes, polyenes, enones. 3. K-bands also appear in an aromatic compound which is substituted by a chromophore. 4. The intensity of K-band, is usually more than 104 . 5. The K-band absorption due to conjugated ‘enes’ and ‘enones’ are effected differently by changing the polarity of the solvent
  • 12. (b) R* band. 1. Such type of bands originate due to n→π* transition of a single chromophoric group and having at least one lone pair of electrons on the hetero atom. 2. R-bands are also called forbidden bands. These are less intense.
  • 13. (c) B-band. 1. Such type of bands arise due π→π* transition in aromatic or hetero-aromatic molecules. 2. Benzene shows absorption peaks between 230–270mμ. 3. When a chromophoric group is attached to the benzene ring, the B-bands are observed at longer wave-lengths than the more intense K-bands.
  • 14. (d) E-bands. 1. Such bands originate due to the electronic transitions in the benzenoid system of three ethylenic bonds which are in closed cyclic conjugation. 2. These are further characterized as E1 and E2-bands. E1 and E2 bands of benzene appear at 184 and 204 mμ respectively. 3. E1 band which appears at lower wave-length is usually more intense than the E2-band for the same compound which appears at longer wavelength.
  • 15. 3.2. The Chromophore Concept 1. It is defined as any isolated covalently bonded group that shows a characteristic absorption in the ultra- violet or the visible region. 2. All those compounds which absorb light of wavelength between 400-800 mμ appear coloured to the human eye. 3. Exact colour depends upon the wavelength of light absorbed by the compound 4. Nitro-compounds are generally yellow in colour. 5. Similarly, aryl conjugated azo group is a chromophore for providing colour to azo dyes.
  • 16. 3.3. The Auxochrome Concept 1. An auxochrome can be defined as any group-which does not itself act as a chromophore but whose presence brings about a shift of the absorption band towards the red end of the spectrum (longer wavelength). 2. The absorption at longer wavelength is due to the combination of a chromophore and an auxochrome to give rise to another chromophore. 3. An auxochromic group is called colour enhancing group. 4. Some common auxochromic groups are —OH, —OR, —NH2, —NHR, —NR2, —SH etc. 5. For example, benzene shows an absorption maximum at 255 mμ [Abs. max 203] whereas aniline absorbs at 280 mμ [Abs max 1430]. Hence, amino (—NH2) group is an auxochrome.
  • 17. 4. Absorption and Intensity Shifts (a) Bathochromic effect/Red Shift 1. It is an effect by virtue of which the absorption maximum is shifted towards longer wavelength due to the presence of an auxochrome or by the change of solvent. 2. Such an absorption shift towards longer wavelength is called Red shift or bathochromic shift. 3. For example, benzene shows an absorption maximum at 255 mμ [Abs. max 203] whereas aniline absorbs at 280 mμ [Abs max 1430]. Hence, amino (—NH2) group is an auxochrome.
  • 18. (b) Hypsochromic shift/Blue Shift 1. It is an effect by virtue of which the absorption maximum is shifted towards shorter wavelength.. 2. The absorption shifted towards shorter wavelength is called Blue shift or hypsochromic shift 3. . In the case of aniline, absorption maximum occurs at 280 mμ because the pair of electrons on nitrogen atom is in conjugation with the π bond system of the benzene ring. In its acidic solutions, a blue shift is caused and absorption occurs at shorter wavelength (~203 mμ).
  • 19. (c) Hyperchromic effect. 1. It is an effect due to which the intensity of absorption maximum increases. 2. The introduction of an auxochrome usually increases intensity of absorption. 3.For example, benzene shows an absorption maximum at 255 mμ [Abs. max 203] whereas aniline absorbs at 280 mμ [Abs max 1430]. Hence, amino (—NH2) group is an auxochrome.
  • 20. (d) Hypochromic effect. 1 It is defined as an effect due to which the intensity of absorption maximum decreases. 2. For example, biphenyl absorbs at 250 mμ, Abs max 19000 whereas 2-methyl biphenyl absorbs at 237 mμ, Abs max 10250
  • 21. 5. Effect of Temperature 1. It is known that the vibrational and the rotational states depend on temperature. 2. As the temperature is decreased, vibrational and the rotational energy state of the molecules are also lowered. 3. Thus, when the absorption of light occurs at a lower temperature, smaller distribution of excited states result. It produces finer structure in the absorption band than what is noticed at higher temperature. 1.The solvent used also effects the fineness of absorption band in UV spectrum. 2.If the dielectric constant of the solvent is high, there will be stronger solute- solvent interactions. 3.Due to this, vibrational and rotational energy states of molecules increase and thus, the fineness of the absorption band falls. Solvent on the Fineness of Absorption Band.
  • 22. Solvent Effects 1. A most suitable solvent is one which does not itself absorb in the region under investigation. 2. A dilute solution of the sample is always prepared for the spectral analysis. Most commonly used solvent is 95% Ethanol. 3. Ethanol is a best solvent as it is cheap and is transparent down to 210 mμ. 4.Some other solvents which are transparent above 210 mμ are n- hexane, methyl alcohol, cyclohexane, acetonitrile, diethyl ether etc
  • 23. 7. Instrumentation. A. Light Source b. Collimating System c. Monochromator d. Sample Holder e. Detector. Ideal Property of Source. 1. Stable 2. Not Fluctuating 3. Emit of light continuous & Uniform Intensity for which its Used. 4. It should not be fatigue on continuous used. For Visible Spectroscopy. 1. Tungsten Halogen Lamp For UV Radiation. 1. Hydrogen Discharge Lamp. 2. Xenon Discharge Lamp. 3. Mercury Arc Lamp.
  • 24. Light Source For Visible Spectroscopy. 1. Tungsten Halogen Lamp  Its Construction is similar to the house hold lamp.  Bulb contains a filament of Tungsten fixed in evacuated condition & then filled with inert gas.  The filament can be heated up to 3000 k, beyond this this Tungsten starts sublimating.  It is used when polychromatic radiation is required. To prevent this along with inert gas some amount of halogen is introduced. (usually Iodine)  Sublimated form of Tungsten is reacted with Iodine to form complex, which migrate back to the hot filament.  It provides a supply of radiation in the wavelength range of 320- 2500nm.  Demerit- It emit the major portion of near IR region
  • 25.
  • 26. Light Source For UV Spectroscopy. 1. Hydrogen Discharge Lamp.  In this pair of electrode is enclosed in a glass tube (provide with silica or quartz for UV radiation to pass it) filled with hydrogen gas.  When current is passed through the electrode maintained at high voltage, discharge of electron occurs with excites hydrogen molecule which in turn cause emission of UV radiation.  They are stable and robust. Covers a range 160-375nm
  • 27. Light Source For UV Spectroscopy. 1. Xenon Discharge Lamp  It possesses 2 tungsten electrode separated by some distance.  This are enclosed in a glass tube with quartz / Fused Silica & Xenon gas is filled under pressure.  An intense arc is formed between electrode by applying high voltage.  This is good source of continuous plus additional intense radiation. Its intensity is higher than Hydrogen Discharge Lamp.  Demerit: The lamp since operate at high voltage become very hot during operation & hence need thermal insulation.
  • 28. Light Source For UV Spectroscopy. 1. Mercury Arc Lamp  In Mercury arc lamp, mercury vapor is stored under high pressure & excitation of mercury atom is done by electrical discharge.  Demerit: Not suitable for continuous spectral studies because it doesn’t give continuous radiations.
  • 29. b. Collimating System The radiation emitted by source is collimated (parallel) by lenses, mirror and slits. Lenses:  Material used for the lenses must be transparent to the radiation being used.  Ordinary silicate glass transmits between 350 to 3000 nm & is suitable for visible and near IR region.  Quartz or fused silica is used as a material for lenses to work below 300 nm. Mirrors:  This are used to reflect, focus or collimating light beam in spectrophotometer.  To minimize the light loss, mirror are aluminized on their surface Slits:  Important device in resolving polychromatic to monochromatic radiation To achieve this entrance & Exit Slits are Used.  The width of slit plays imp. role in resolution of polychromatic radiation.
  • 30. c. Monochromator This device is used to isolate the radiation of desired wavelength from wavelength of continuous spectra. Ex. 1. Filters 2. Prism 3. Grating. 1.Filters:  Selection of filter is usually done on compromise between peak transaction & band pass width; the former should be as high as possible & latter as narrow as possible. Absorption Filters: Works by selective absorption of unwanted radiation and transmit the radiation which is required. Ex. Glass & Gelatin.
  • 31. Selection of absorption filters is done according to the following procedure.  Draw a filter wheel.  Write the color VIBGYOR in anticlockwise  If solution to be analyzed is blue in color filter having complimentary color orange is to be used.  Similarly we can select the required filters in colorimeter, based upon the color of the solution  An absorption glass filter is made of solid sheet of glass that has been colored by pigment which is dissolved or dispersed in the glass.  The color in the glass filter is produce by incorporating metal oxide like Cr, Mn, Fe, Ni, Co, Cu etc.
  • 32. Gelatin filter is an example of absorption filter prepared by adding organic pigments.  Here instead of solid glass sheet thin gelatin sheet are used  This are not used now days.  It tends to be deteriorate to be time & glass affected by heat and moisture The Color of dye gets bleached. Merits: 1. Simple in construction. 2. Cheaper. 3. Selection of filter easy Demerits: 1. Less Accurate. 2. Band pass (bandwidth) is ±30nm If we have to measure the 400nm; we get the radiation from 370-430 nm, Less Accurate Results Obtained.
  • 33. Interference filters:  Work on the interference phenomenon cause rejection of unwanted wavelength by selective reflection.  It is constructed by using two parallel glass plate, which are silvered internally & separated by thin film of dielectric material of different (CaF2, SiO, MgF2) refractive index. Merits: 1. These filters have band pass of 10-15 nm with peak transmittance of 40-60%. 2. Cheap 3. Additional filters can be used to cut off undesirable wavelength
  • 34. 2. Prism.  Prism is made up from glass, quartz or fused silica.  Quartz or fused silica is the choice of material for UV.  When the light is pass through the glass prism, dispersion of polychromatic light in RAINBOW occurs.  Now by rotation of Prism in different wavelength of the spectrum can be made to pass through the exit slit on the sample.  The effective wavelength depends on the dispersive power of Prism material & Optical Angle of the Prism.
  • 35. There are two types of mounting in an instrument  one is called ‘Cornu type’ (refractive), which has an optical angle of 60o and its adjusted such that on rotation the emerging light is allowed to fall on exit slit.  The other type is called “Littrow type” (reflective), which has optical angle 30o and its one surface is aluminized with reflected light back to pass through prism and to emerge on the same side of the light source i.e. light doesn’t pass through the prism on other side.
  • 36. Grating:  Are most effective one in converting a polychromatic light to monochromatic light. As a resolution of +/- 0.1nm could be achieved by using gratings, they are commonly used in spectrophotometers.  Gratings are of two types. 1. Diffraction grating. 2. Transmission gratings. 1. Diffraction grating.  More refined dispersion of light is obtained by means of diffraction gratings.  These consist of large number of parallel lines ( grooves) about 15000-30000/ inch is ruled on highly polished surface of aluminium.  These gratings are replica made from master gratings by coating the original master grating with a epoxy resin and are removed after setting
  • 37. 2. Transmission gratings.  It is similar to diffraction grating but refraction takes place instead of reflection.  Refraction produces reinforcement. this occurs when radiation transmitted through grating reinforces with the partially refracted radiation.
  • 38. Advantages:  Grating gives higher and linear dispersions compared to prism monochromator.  Can be used over wide wavelength ranges.  Gratings can be constructed with materials like aluminium which is resistant to atmospheric moisture.  Provide light of narrow wavelength.  No loss of energy due to absorption
  • 39. d. Sample Holder  The cells or cuvettes are used for handling liquid samples.  The cell may either be rectangular or cylindrical in nature.  For study in UV region; the cells are prepared from quartz or fused silica whereas color corrected fused glass is used for visible region.  The surfaces of absorption cells must be kept scrupulously clean. No fingerprints or blotches should be present on cells.  Cleaning is carried out washing with distilled water or with dilute alcohol, acetone.
  • 40. e. Detectors.  Device which converts light energy into electrical signals, that are displayed on readout devices.  The transmitted radiation falls on the detector which determines the intensity of radiation absorbed by sample The following types of detectors are employed in instrumentation of absorption spectrophotometer.  1. Barrier layer cell/Photovoltaic cell  2. Phototubes/ Photo emissive tube  3. Photomultiplier tube
  • 41. Ideal Properties of Detectors.  It should give quantitative response.  It should have high sensitivity and low noise level.  It should have a short response time.  It should provide signal or response quantitative to wide spectrum of radiation received.
  • 42. 1. Barrier layer cell/Photovoltaic cell  The detector has a thin film metallic layer coated with silver or gold and acts as an electrode.  It also has a metal base plate which acts as another electrode.  These two layers are separated by a semiconductor layer of selenium.
  • 43.  When light radiation falls on selenium layer, electrons become mobile and are taken up by transparent metal layer.  This creates a potential difference between two electrodes & causes the flow of current.  When it is connected to galvanometer, a flow of current observed which is proportional to the intensity and wavelength of light falling on it.
  • 44. 2. Phototubes/ Photo emissive tube
  • 45.  Consists of a evacuated glass tube with a photocathode and a collector anode.  The surface of photocathode is coated with a layer of elements like cesium, silver oxide or mixture of them.  When radiant energy falls on photosensitive cathode, electrons are emitted which are attracted to anode causing current to flow.  More sensitive compared to barrier layer cell and therefore widely used.  The principle employed in this detector is that, multiplication of photoelectrons by secondary emission of electrons
  • 46.  In a vacuum tube, a primary photo-cathode is fixed which receives radiation from the sample.  Some eight to ten dynodes are fixed each with increasing potential of 75-100V higher than preceding one.  Near the last dynode is fixed an anode or electron collector electrode.  Photo-multiplier is extremely sensitive to light and is best suited where weaker or low radiation is received
  • 47. 3. Photomultiplier tube  The principle employed in this detector is that,multiplication of photoelectrones by secondary emission of electrons.  In a vaccum tube a primary photo-cathode is fixed which receives radiation from the sample.  Some eight to 10 dynodes are fixed each with increasing potential of 75-100V higher than preceeding one.  Photomultiplier is extremely sensitive to light and is best suited where weaker or low radiation is received.  Near the last dynode is fixed an anode or electrone collector electrode.