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Instrumentation
of
UV-Visible Spectroscopy
Prepared by
Prof.(Dr.) Dinesh Kumar Mehta
MMCP, (MMDU), Mullana
INSTRUMENTATION
Unlike a spectrometer (which is any instrument that can measure the
properties of light over a range of wavelengths), a spectrophotometer
measures only the intensity of light as a function of its wavelength. The
key components of a spectrophotometer are:
• Light source
• Monochromator
• Sample area
• Detector and Recorder
Light Source:
The most suitable sources of light are
1. Deuterium lamp which emits the light in the UV-region (160-375
nm)
2. Tungsten lamp or tungsten-halogen lamp which emits radiation in
the Visible and near infrared regions (350-2500 nm)
3. Xenon arc lamp which emits radiation in the range 190-800 nm
4. Light emitting diodes (LED) which emits radiation in the visible
range 400-800 nm.
The instruments automatically swap lamps when scanning between
the UV and UV-VIS regions.
Monochromator
The main function of the monochromator is to disperse the beam of
light obtained from the primary source, into its component (Figure 3).
The principle components of monochromator are
• An entrance slit
• A collimating lens
• A dispersing device
• A focusing lens
• An exit slit
The radiation emitted from the primary source (polychromatic
radiation) enters the monochromator through the entrance slit. The
beam is collimated and then strikes the dispersing element (Prism or
grit) at a particular angle.
Sample area
One of the two divided beams is passed through the sample solution
and the other beam is passed through the reference solution. Although,
the samples for recording spectra are most commonly liquids, but the
absorbance of gases and even of solids can be measured. Both sample
and reference solutions are placed in a transparent cell, known as
cuvette. The cuvettes are rectangular in shape, and usually have an
internal width of 1 cm.
It is important that the material of cells must be transparent to the
radiation throughout the region under study. The cells are usually made
of glass, plastic as well as silica or quartz
Detector and Recorder
A detector converts a light signal into an electrical signal. After the
beams are passed through the sample under study as well as the
reference cell, the intensities of the respective transmitted beams are
then compared over the whole wavelength range of the instrument.
Generally two photocells are used as detector in UV spectrometer to
record the spectra. One of the photocell receives the beam from
sample cell and second detector receives the beam from the reference.
The intensity of the radiation from the reference cell is stronger than
the beam of sample cell.
This results in the generation of pulsating or alternating currents in the
photocells.
Spectrophotometers consist of either a photomultiplier tube detector
or a photodiode detector.
The commonly used detector in UV-Vis spectroscopy is
Photomultiplier tube. It consists of three components:
• A cathode which emits electrons when struck by photons of
radiation known as photoemissive cathode
• Several dynodes which emit several electrons for each electron
striking them an anode
In its functioning, when a photon of radiation strikes the cathode,
emission of several electrons take place. These emitted electrons are
then accelerated towards the many dynodes. The first dynode is 90V
more positive than the cathode. The electrons strike the first dynode,
causing the emission of several electrons for each incident electron.
These electrons are then accelerated towards the second dynode, to
produce more electrons which are accelerated towards dynode
three and so on. Finally all the electrons are collected at the anode.
Several dynodes are arranged between the anode and the cathode to
produce an amplification effect. Each photon usually produces 106
-107
electrons, resulting in the amplified current that can be measured.
Photomultipliers are very sensitive to both UV and visible radiations
and have fast response times. It is significant to note that Intense light
may damage photomultipliers, hence they are limited to measuring low
power radiation.
Photodiodes are increasingly being used as detectors in modern
spectrophotometers. Photodiode detectors have a wider dynamic range
and are more robust than photomultiplier tube detectors. In a
photodiode, light falling on the semiconductor material allows
electrons to flow through it, thereby depleting the charge in a capacitor
connected across the material. The amount of charge that is required to
recharge the capacitor at regular intervals is proportional to the
intensity of the light. The limits of detection are approximately 170–
1100 nm for silicon-based detectors.
Some modern spectrophotometers contain an array of photodiode
detectors instead of a single detector as mentioned in above figure.
The amount of charge needed to recharge the capacitors is proportional
to the number of photons detected by each diode, which in turn is
proportional to the light intensity. The absorption spectrum is obtained
by measuring the variation in light intensity over the entire wavelength
range.
Sample Preparation
The UV-Vis spectra are usually measured in very dilute solutions.
Usually 1 mg of the compound of molecular weight of 100-200 is
dissolved in 100 ml of suitable solvent and only a portion is used for
recording the spectra. The solvent should not absorb radiation and must
be transparent over the desired range of wavelength. The solvents,
which do not contain conjugated system, are most suitable for
recording the UV-spectra. The solvent should also be inert to the
sample. Some commonly used solvents are water, 95% ethanol,
methanol and hexane.

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INSTRUMENTATIONS UV-VIS.pdf

  • 1. Instrumentation of UV-Visible Spectroscopy Prepared by Prof.(Dr.) Dinesh Kumar Mehta MMCP, (MMDU), Mullana
  • 2. INSTRUMENTATION Unlike a spectrometer (which is any instrument that can measure the properties of light over a range of wavelengths), a spectrophotometer measures only the intensity of light as a function of its wavelength. The key components of a spectrophotometer are: • Light source • Monochromator • Sample area • Detector and Recorder Light Source: The most suitable sources of light are 1. Deuterium lamp which emits the light in the UV-region (160-375 nm) 2. Tungsten lamp or tungsten-halogen lamp which emits radiation in the Visible and near infrared regions (350-2500 nm) 3. Xenon arc lamp which emits radiation in the range 190-800 nm 4. Light emitting diodes (LED) which emits radiation in the visible range 400-800 nm.
  • 3. The instruments automatically swap lamps when scanning between the UV and UV-VIS regions. Monochromator The main function of the monochromator is to disperse the beam of light obtained from the primary source, into its component (Figure 3). The principle components of monochromator are • An entrance slit • A collimating lens • A dispersing device • A focusing lens • An exit slit The radiation emitted from the primary source (polychromatic radiation) enters the monochromator through the entrance slit. The beam is collimated and then strikes the dispersing element (Prism or grit) at a particular angle.
  • 4. Sample area One of the two divided beams is passed through the sample solution and the other beam is passed through the reference solution. Although, the samples for recording spectra are most commonly liquids, but the absorbance of gases and even of solids can be measured. Both sample and reference solutions are placed in a transparent cell, known as cuvette. The cuvettes are rectangular in shape, and usually have an internal width of 1 cm. It is important that the material of cells must be transparent to the radiation throughout the region under study. The cells are usually made of glass, plastic as well as silica or quartz Detector and Recorder A detector converts a light signal into an electrical signal. After the beams are passed through the sample under study as well as the reference cell, the intensities of the respective transmitted beams are
  • 5. then compared over the whole wavelength range of the instrument. Generally two photocells are used as detector in UV spectrometer to record the spectra. One of the photocell receives the beam from sample cell and second detector receives the beam from the reference. The intensity of the radiation from the reference cell is stronger than the beam of sample cell. This results in the generation of pulsating or alternating currents in the photocells. Spectrophotometers consist of either a photomultiplier tube detector or a photodiode detector. The commonly used detector in UV-Vis spectroscopy is Photomultiplier tube. It consists of three components: • A cathode which emits electrons when struck by photons of radiation known as photoemissive cathode • Several dynodes which emit several electrons for each electron striking them an anode In its functioning, when a photon of radiation strikes the cathode, emission of several electrons take place. These emitted electrons are then accelerated towards the many dynodes. The first dynode is 90V
  • 6. more positive than the cathode. The electrons strike the first dynode, causing the emission of several electrons for each incident electron. These electrons are then accelerated towards the second dynode, to produce more electrons which are accelerated towards dynode three and so on. Finally all the electrons are collected at the anode. Several dynodes are arranged between the anode and the cathode to produce an amplification effect. Each photon usually produces 106 -107 electrons, resulting in the amplified current that can be measured. Photomultipliers are very sensitive to both UV and visible radiations and have fast response times. It is significant to note that Intense light
  • 7. may damage photomultipliers, hence they are limited to measuring low power radiation. Photodiodes are increasingly being used as detectors in modern spectrophotometers. Photodiode detectors have a wider dynamic range and are more robust than photomultiplier tube detectors. In a photodiode, light falling on the semiconductor material allows electrons to flow through it, thereby depleting the charge in a capacitor connected across the material. The amount of charge that is required to recharge the capacitor at regular intervals is proportional to the intensity of the light. The limits of detection are approximately 170– 1100 nm for silicon-based detectors.
  • 8. Some modern spectrophotometers contain an array of photodiode detectors instead of a single detector as mentioned in above figure. The amount of charge needed to recharge the capacitors is proportional to the number of photons detected by each diode, which in turn is proportional to the light intensity. The absorption spectrum is obtained by measuring the variation in light intensity over the entire wavelength range. Sample Preparation The UV-Vis spectra are usually measured in very dilute solutions. Usually 1 mg of the compound of molecular weight of 100-200 is dissolved in 100 ml of suitable solvent and only a portion is used for recording the spectra. The solvent should not absorb radiation and must be transparent over the desired range of wavelength. The solvents, which do not contain conjugated system, are most suitable for recording the UV-spectra. The solvent should also be inert to the sample. Some commonly used solvents are water, 95% ethanol, methanol and hexane.