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Atomic Emission Atomic Emission Spectroscopy Spectroscopy Yongsik Lee Yongsik Lee May 14, 2004 May 14, 2004
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Atomic Emission Spectroscopy Yongsik Lee May 14, 2004.

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Page 1: Atomic Emission Spectroscopy Yongsik Lee May 14, 2004.

Atomic Emission Atomic Emission SpectroscopySpectroscopy

Yongsik LeeYongsik Lee

May 14, 2004May 14, 2004

Page 2: Atomic Emission Spectroscopy Yongsik Lee May 14, 2004.

Introduction to AESIntroduction to AES► Atomization Emission Sources

Flame – still used for metal atoms Electric Spark and Arc Direct current Plasmas Microwave Induced Plasma Inductively Coupled Plasma – the most important te

chnique► Advantages of plasma

Simultaneous multi-element Analysis – saves sample amount

Some non-metal determination (Cl, Br, I, and S) Concentration range of several decades (105 – 106)

► Disadvantages of plasma very complex Spectra - hundreds to thousands of lin

es High resolution and expensive optical components Expensive instruments, highly trained personnel req

uired

Page 3: Atomic Emission Spectroscopy Yongsik Lee May 14, 2004.

10A Plasam Source AES10A Plasam Source AES

►Plasma an electrically conducting gaseous mixture conta

ining significant concentrations of cations and electrons.

►Three main types Inductively Coupled Plasma (ICP) Direct Current Plasma (DCP) Microwave Induced Plasma (MIP)

Page 4: Atomic Emission Spectroscopy Yongsik Lee May 14, 2004.

ICP► Inductively Coupled Plasma (ICP)

Plasma generated in a device called a Torch

Torch up to 1" diameter Ar cools outer tube, defines plasma shape Rapid tangential flow of argon cools outer q

uartz and centers plasma Rate of Argon Consumption 5 - 20 L/Min Radio frequency (RF) generator 27 or 41 M

Hz up to 2 kW Telsa coil produces initiation spark

► Ions and e- interact with magnetic field and begin to flow in a circular motion.

► Resistance to movement (collisions of e- and cations with ambient gas) leads to ohmic heating.

► Sample introduction is analogous to atomic absorption.

Page 5: Atomic Emission Spectroscopy Yongsik Lee May 14, 2004.

Sample introductionSample introduction

►NebulizerNebulizer►Electrothermal vaporizerElectrothermal vaporizer

►Table 8-2 methods of sample introductonTable 8-2 methods of sample introducton

Page 6: Atomic Emission Spectroscopy Yongsik Lee May 14, 2004.

Nebulizer

► convert solution to fine spray or aerosol

►Ultrasonic nebulizer uses ultrasound waves t

o "boil" solution flowing across disc

► Pneumatic nebulizer uses high pressure gas

to entrain solution

Page 7: Atomic Emission Spectroscopy Yongsik Lee May 14, 2004.

Electro-thermal vaporizer Electro-thermal vaporizer ETVETV

► Electrothermal vaporizer (ETV) electric current rapidly h

eats crucible containing sample

sample carried to atomizer by gas (Ar, He)

only for introduction, not atomization

Page 8: Atomic Emission Spectroscopy Yongsik Lee May 14, 2004.

Plasma structurePlasma structure

►Brilliant white core Ar continuum and lines

► Flame-like tail up to 2 cm

► Transparent region where measurements are m

ade (no continuum)

Page 9: Atomic Emission Spectroscopy Yongsik Lee May 14, 2004.

Plasma Plasma characteristics

► Hotter than flame (10,000 K) - more complete atomization/ excitation

► Atomized in "inert" atmosphere► Ionization interference small due to

high density of e- ► Sample atoms reside in plasma for

~2 msec and► Plasma chemically inert, little oxide

formation► Temperature profile quite stable an

d uniform.

Page 10: Atomic Emission Spectroscopy Yongsik Lee May 14, 2004.

DC plasmaDC plasma

► First reported in 1920s► DC current (10-15 A) flows

between C anodes and W cathode

► Plasma core at 10,000 K, viewing region at ~5,000 K

► Simpler, less Ar than ICP - less expensive

► Less sensitive than ICP► Should replace the carbon

anodes in several hours

Page 11: Atomic Emission Spectroscopy Yongsik Lee May 14, 2004.

Atomic Emission Spectrometer

► May be >1,000 visible lines (<1 Å) on continuum► Need

higher resolution (<0.1 Å) higher throughput low stray light wide dynamic range (>1,000,000) precise and accurate wavelength calibration/intensities stability computer controlled

► Three instrument types: sequential (scanning and slew-scanning) Multichannel - Measure intensities of a large number of elements (5

0-60) simultaneously Fourier transform FT-AES

Page 12: Atomic Emission Spectroscopy Yongsik Lee May 14, 2004.

Desirable properties of an AE Desirable properties of an AE spectrometerspectrometer

Page 13: Atomic Emission Spectroscopy Yongsik Lee May 14, 2004.

Sequential vs. multichannelSequential vs. multichannel► Sequential instrument

PMT moved behind aperture plate, or grating + prism moved to focus new l on exit slit Pre-configured exit slits to detect up to 20 lines, slew scan

► characteristics Cheaper Slower

► Multichannel instrument Polychromators (not monochromator) - multiple PMT's Array-based system

► charge-injection device/charge coupled device► characteristics

Expensive ( > $80,000) Faster

Page 14: Atomic Emission Spectroscopy Yongsik Lee May 14, 2004.

Sequential vs. multichannelSequential vs. multichannel

Page 15: Atomic Emission Spectroscopy Yongsik Lee May 14, 2004.

Sequential monochromatorSequential monochromator

►Slew-scan spectrometers even with many lines, much spectrum contains n

o information rapidly scanned (slewed) across blank regions (b

etween atomic emission lines)►From 165 nm to 800 nm in 20 msec

slowly scanned across lines►0.01 to 0.001 nm increment

computer control/pre-selected lines to scan

Page 16: Atomic Emission Spectroscopy Yongsik Lee May 14, 2004.

Slew scan spectrometerSlew scan spectrometer

► Two slew-scan Two slew-scan gratingsgratings

► Two PMTs for Two PMTs for VIS and UVVIS and UV

►Most use holographic grating

Page 17: Atomic Emission Spectroscopy Yongsik Lee May 14, 2004.

Scanning echelle spectrometerScanning echelle spectrometer► PMT is moved to monitor signal from slotted aperture.

About 300 photo-etched slits 1 second for moving one slit

► Can be used as multi channel spectrometer► Mostly with DC plasma source

Page 18: Atomic Emission Spectroscopy Yongsik Lee May 14, 2004.

AES instrument typesAES instrument types

►Three instrument types: sequential (scanning and slew-scanning) Multichannel - Measure intensities of a large nu

mber of elements (50-60) simultaneously Fourier transform FT-AES

Page 19: Atomic Emission Spectroscopy Yongsik Lee May 14, 2004.

Multichannel polychromator AESMultichannel polychromator AES

• Rowland circle• Quantitative det. 20 more elementsWithin 5 minutes

In 10 minutes

Page 20: Atomic Emission Spectroscopy Yongsik Lee May 14, 2004.

Applications of AES

► AES relatively insensitive small excited state population at moderate temperature

► AAS still used more than AES less expensive/less complex instrumentation lower operating costs greater precision

► In practice ~60 elements detectable 10 ppb range most metals Li, K, Rb, Cs strongest lines in IR Large # of lines, increase chance of overlap

Page 21: Atomic Emission Spectroscopy Yongsik Lee May 14, 2004.

Detection power of ICP-AESDetection power of ICP-AES

Page 22: Atomic Emission Spectroscopy Yongsik Lee May 14, 2004.

ICP/OES INTERFERENCES► Spectral interferences:

caused by background emission from continuous or recombination phenomena,

stray light from the line emission of high concentration elements, overlap of a spectral line from another element, or unresolved overlap of molecular band spectra.

► Corrections Background emission and stray light compensated for by subtracting backgr

ound emission determined by measurements adjacent to the analyte wavelength peak.

Correction factors can be applied if interference is well characterized Inter-element corrections will vary for the same emission line among instru

ments because of differences in resolution, as determined by the grating, the entrance and exit slit widths, and by the order of dispersion.

Page 23: Atomic Emission Spectroscopy Yongsik Lee May 14, 2004.

Physical interferences of ICP

► cause effects associated with the sample nebulization and transport proce

sses. Changes in viscosity and surface tension can cause significant inac

curacies, ► especially in samples containing high dissolved solids ► or high acid concentrations.

Salt buildup at the tip of the nebulizer, affecting aerosol flow rate and nebulization.

► Reduction by diluting the sample or by using a peristaltic pump, by using an internal standard or by using a high solids nebulizer.

Page 24: Atomic Emission Spectroscopy Yongsik Lee May 14, 2004.

Interferences of ICPInterferences of ICP

►Chemical interferences: include molecular compound formation, ionizatio

n effects, and solute vaporization effects. Normally, these effects are not significant with t

he ICP technique. Chemical interferences are highly dependent on

matrix type and the specific analyte element.

Page 25: Atomic Emission Spectroscopy Yongsik Lee May 14, 2004.

Memory interferences:

► When analytes in a previous sample contribute to the signals measured in a new sample.

► Memory effects can result from sample deposition on the uptake tubing to the nebulizer from the build up of sample material in the plasma torch and spray

chamber. ► The site where these effects occur is dependent on the ele

ment and can be minimized by flushing the system with a rinse blank between samples.

► High salt concentrations can cause analyte signal suppressions and confuse interference tests.

Page 26: Atomic Emission Spectroscopy Yongsik Lee May 14, 2004.

Typical Calibration ICP curvesTypical Calibration ICP curves

Page 27: Atomic Emission Spectroscopy Yongsik Lee May 14, 2004.

Calibration curves of ICP-AESCalibration curves of ICP-AES

Page 28: Atomic Emission Spectroscopy Yongsik Lee May 14, 2004.

10B. Arc and Spark AES10B. Arc and Spark AES

►Arc and Spark Excitation Sources: Limited to semi-quantitative/qualitative

analysis (arc flicker) Usually performed on solids Largely displaced by plasma-AES

►Electric current flowing between two C electrodes

Page 29: Atomic Emission Spectroscopy Yongsik Lee May 14, 2004.

Carbon electrodesCarbon electrodes

► Sample pressed into electrode or mixed with Cu powder and pressed - Briquetting (pelleting)

► Cyanogen bands (CN) 350-420 nm occur with C electrodes in air -He, Ar atmosphere

► Arc/spark unstable each line measured >20 s needs multichannel detectio

n

Page 30: Atomic Emission Spectroscopy Yongsik Lee May 14, 2004.

Arc and Spark spectrographArc and Spark spectrograph

Page 31: Atomic Emission Spectroscopy Yongsik Lee May 14, 2004.

spectrographspectrograph

►Beginning 1930s►photographic film

Cheap Long integration times Difficult to develop/analyze Non-linearity of line "darkness“

►Gamma function►Plate calibration

Page 32: Atomic Emission Spectroscopy Yongsik Lee May 14, 2004.

Multichannel photoelectric spectromeMultichannel photoelectric spectrometerter

►multichannel PMT instruments for rapid determinations (<20 lines) but not vers

atile For routine analysis of solids

►metals, alloys, ores, rocks, soils portable instruments

►Multichannel charge transfer devicesMultichannel charge transfer devices Recently on the marketRecently on the market Orignally developed for plasma sourcesOrignally developed for plasma sources

Page 33: Atomic Emission Spectroscopy Yongsik Lee May 14, 2004.

HomeworkHomework

►10-1, 10-2, 10-5, 10-710-1, 10-2, 10-5, 10-7