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UV-Vis transitions
sigma —> sigma*
pi —> pi*
n —> sigma*
n —> pi
sigma —> sigma*
Has/requires the highest energy
n —> sigma*
2nd highest energy
Absorbing species
Organic and inorganic compounds
Chromophores
Functional groups that absorb in the UV-Vis regions
Auxochromes
Functional groups that do not absorb but have the effect shifting of chromophore peaks to different wavelength
Bathochromic shift (red shift)
Shift in the lambda max, longer wavelength
Hypsochromic shift (blue shift)
Shift in the lambda max, shorter wavelength
Hyperchromic shift
increase in the intensity of UV maxima
Hypochromic shift
Decrease in the intensity of UV maxima
Basic instrumentation in UV-Vis
Light source —> wavelength selector —> sample —> detector —> output
Basic instrumentation - Radiation source
deuterium lamp
Tungsten halogen lamp
Deuterium lamp - radiation source
Has a tungsten filament and a nickel plate anode filled deuterium gas. Subjected to high voltage; radiation in the UV region (165-300nm). Emits in one direction only.
Xenon and mercury lamps
Emit in all directions, typically has a half life of ~1000n
Tungsten halogen lamp - radiation source
Emits continuous radiation in 325-3000nm. Used when polychromatic light is required. Has a very low noise bulb filled with inert gas.
To prevent tungsten lamp from darkening
Formation of volatile halide from evaporated tungsten with iodine
At 300k
Tungsten starts to sublime
Basic instrumentation - wavelength selector
filter
Monochromator
Photometer
spectrometer/spectrophotometer
Filter - wavelength selector
Absorption and interference filters. Quantitative work prism and grating are commonly used.
Monochromator - wavelength selector
Prism and grating
Prism
Diffraction grating
Grating monochromator
Transmission grating
Photometer - wavelength selector
Uses filter as wavelength selector. For single wavelength selection used for visible rehion.
Spectrometer/spectrophotometer
Uses monochromator as wavelength selector. For wavelength scanning multiple selection, covers UV-Vis and IR regions
Basic instrumentation - sample holder
Cuvette and microcells
Cuvette
Small tube like container with straight sides and a square cross-section.
acrylic plastic cells
Silicate glass cells
Fused quartz cells
Cuvette pathlength
Distance of light that passes through the interior walls of a cuvette. Sizes vary from 1mm - 100mm
Acrylic plastic cells - cuvette (sample holder)
Lowest in cost, not resistant to all solvents. Used in the visible region only because its transparent from 350 - 900nm.
Silicate glass cells - cuvette (sample holder)
More durable than acrylic plastic cells. Used in the visible region only because it is transparent from 350 - 2500nm.
Fused quartz cells - cuvette (sample holder)
Very expensive, transparent in both UV and visible regions (200-2500nm)
Microcells
Can be used when sample volume is extremely liquid (5 uL). Part of light beam is blocked.
Care of cells (microcells)
avoid touching the optical surfaces
Must be wiped with photographic tissue if contaminated
If seriously contaminated, may be cleaned with mild sulfonic surfactant.
Severe cases, treatment with strong acid (HCl or HNO3)
Basic instrumentation - detector
spectroscope
Spectrograph
Spectrophotometer
Spectroscope
Used naked eye as detector
Spectrograph
Uses a photographic film as the detector
Spectrophotometer
Uses photon detector. Normally contain either a photomultiplier tube or photodiode. Some of this modern instrument contain several photodiodes.
Detector - types of instruments
single beam
Double beam in time
Double beam in space
Multichannel
Single beam
There is only one light beam or optical path from the source in the detector.
Spectronic 20
Determination of transmittance involves three successive steps.
Double beam in space
Two beams are formed in space by V-shaped mirror called beam splitter. Radiation is split into two beams simultaneously. Requires two detectors = more expensive
Double beam in time
Two beams are separated in time by a rotating sector mirror. Beam is alternatively sent through reference and sample cells. Only matter of milliseconds separate the beams.
Multichannel
Able to scan an entire spectrum in 0.1s. Dispersive system is placed after the sample or reference. Utilizes diode array detectors.
Problems in measurements
strong absorbance
Weak absorbance
Interference
Sample decomposition
Strong absorbance
Remedy is dilute the sample to an absorbance level within the linear dynamic range. Select one or more wavelengths in the lower absorptivity.
Weak absorbance
Noise results in loss of precision. Any single measurement may be inaccurate. Can be reduced by reducing noise level or increasing slit width to allow more light through the species.
Interference
Scattering and fluorescence
Scattering interference
For pharmaceutical and biological analyses that contains suspended solutions. Reduced by filtering the samples prior the analyses.
Significant scattering
Light is lost and sensitivity and accuracy of quantitative analysis are seriously impaired.
Rayleigh scattering
Particles are small relative to the wavelength of light. Inversely proportional to the fourth wavelength.
Tyndall scattering
Particles are large relative to the wavelength of light and is inversely proportional to the square of lambda.
Fluorescence interference
To eliminate the error in this interference, a filter in the light beam can eliminate the error.
conventional instrument - filter is placed between the sample n detector
Reversed optics - filter id placed between source and sample
Sample decomposition
Some samples are sensitive to photochemical reaction. In extreme cases, a filter may be necessary to eliminate this light.
Qualitative analysis
detection of impurities
Detection of isomers
Detection of functional groups
Quantitative analysis
determination of concentration
Multicomponent analysis
Spectrophotometric titrations
Solvent cut off wavelength
Wavelength below which the solvent itself absorbs all of the light.