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Basic Theory Atomic Absorption Spectroscopy Mimi Wong

AAS Basic Theory

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  • Basic TheoryAtomic Absorption SpectroscopyMimi Wong

  • Bohr model of ATOMIf higher energy is absorbed by the atom,the electron can be completely dissociated from the atom Positively charged ion

  • Bohr model of ATOMEnergy Level Diagram

  • Theory of AA

  • Light SourceHollow Cathode Lamp (HCL)are a type of discharge lamp that produce narrow emission from atomic species electric discharge ionizes rare gas atoms, which are accelerated into the cathode and sputter metal atoms into the gas phase. Collisions with gas atoms or electrons excite the metal atoms to higher energy levels, which decay to lower levels by emitting light

  • AtomizerThe analyte atoms be in the gas phase. Ions or atoms in a sample must undergo desolvation and vaporization in a high-temperature source FAAS: Air-Acetylene / Nitrous oxide-Acetylene analyzes solution onlyGFAAS: electro-thermal furnace accepts solution, slurries and solid samplesMXM(H2O)m,X-(MX)nDesolvationVaporizationAtomizationM*E (measured by detector)MExcitationE (=h) from HCL

  • Advantages of GFAAS vs. FAASmuch more efficient atomizer than flame can accept directly very small absolute quantities of sampleprovides a reducing environment for easily oxidized elementssamples are placed directly in the graphite furnace and the furnace is electrically heated in several steps to dry the sample, ash organic matter, and vaporize the analyte atoms

  • What happen inside atomizerLight (energy) from HCL is absorbed

  • Monochromatorconsists of a diffraction grating (dispersing element), slits, and spherical mirrors. The light source emits a broad spectrum of radiation as represented by the multi-colored line from the lamp to the grating Schematic of a Czerny-Turner monochromator

  • Detectorconvert photons to an electrical signal consists of a photocathode and a series of dynodes in an evacuated glass enclosure. When a photon of sufficient energy strikes the photocathode, it ejects a photoelectron due to the photoelectric effect The amplification depends on the number of dynodes and the accelerating voltage. This amplified electrical signal is collected at an anode at ground potential, which can be measured. Schematic of a PMT

  • SummaryAtomic Absorption AAhProcesses take place for a nebulized sample droplet in AA burner headHCL emits unique energy which can only be absorbed by a particular element

    single element analysisa = coefficient of absorptionb = length of burner headc = element concentrationI = intensity, By Beers Law

    E = (E E) = abc c = E /ab c I

  • Theory of ICP-AESMXM(H2O)m,X-(MX)nDesolvationVaporizationIonizationMExcitationM+DecayExcitationDecayAtomizationProcesses take place for a nebulized sample droplet in ICP dischargeatom emissionh1M*M+ * h2Ion Excited StateIon Ground StateGround StateExcited Statesion emission4321atomic /ionic emissionMeasure the emitted light during the excited atoms decay back to ground state

    multiple element analysis = coefficient of emissionb = length of burner headc = element concentrationIi = intensity, Eii= 1,2,3,4, . nBy Beers Law

    Ei = hi = bc c = Ei / b c I ienergy

  • Detection Limits

  • AA vs. ICP-AES : Detection LimitsRemarks:For comparing the typical ICP-AES, FAAS and GFAAS in the market* Can reach to108 with range extension** precision improves with the use of internal standards105 10 6*103103

    Sheet1

    ICP-AESFlame AASGFAAS

    Level of measurement

    Detection LimitVery good for most elementsVery good for some elementsExcellent for some elements

    Typical Linear Dynamic Range

    Precision

    short term0.3 - 2%**0.1 - 1%1 - 5%

    long term (>4 hrs)< 5%

    Sheet2

    Sheet3

  • AA vs. ICP-AES : Matrix & InterferencesRemarks:For comparing the typical ICP-AES, FAAS and GFAAS in the market* Can reach to108 with range extension** precision improves with the use of internal standards

    Sheet1

    ICP-AESFlame AASGFAAS

    Interferences

    Spectralcommonalmost nonefew

    Chemical (matrix)almost nonemanymany

    Ionizationminimalsomeminimal

    Dissolved solids (max tolerable conc)2 - 30%0.5 - 3%> 20%

    Semi-quantitative analysisyes & easynono

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  • AA vs. ICP-AES : Speed & CostRemarks:For comparing the typical ICP-AES, FAAS and GFAAS in the market

    Sheet1

    ICP-AESFlame AASGFAAS

    No. of elements> 75> 68> 50

    Sample throughput5-30 elements /min/sample15 sec/elements /sample4 min/elements /sample

    Sample UsagehighVery highVery low

    Routine operationeasyeasyeasy

    Method developmentskill requiredeasyskill required

    Unattended operationyesnoyes

    Combustible gasesnoyesno

    Hollow Cathode Lamp / Electrodeless Dicharge Lamp (EDL)noyesyes

    Capital costhighlowmedium/high

    Sample running costaffortablelowhigh

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  • Interference & Solutions

  • ApplicationChoosing a Technique for the Determination of Copper in an Electroplating BathSource: Choosing The Right Trace Element Technique, R. Thomas, Todays Chemist at Work, Vol 8, No. 10, 42-48

  • ApplicationChoosing a Technique for the Determination of Lead and Cadmium in Blood Source: Choosing The Right Trace Element Technique, R. Thomas, Todays Chemist at Work, Vol 8, No. 10, 42-48

  • Other ApplicationsPb poisoning : detection of Zn and Pb in human hair Se and Hg analysis in sea food, such as fish tissue, mussels, oyster & etc.

  • Advantages of AA over ICP-AESWide dynamic range measure from ppm to sub-ppb levels (FAAS + GFAAS)Low running cost Gas supply : Acetylene vs. ArgonLabour skill : Less in AASTraining time : Less in AASMethod development time : Less in AASMaintenance : Less in AAS Spectral Interference Zero

    AAS is a very mature technology