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This chapter explores Atomic Absorption Spectrometry (AAS), a versatile analytical technique used for the quantitative determination of various elements. the flame as a sample holder, desolvation and volatilization source, flame structure, line source, monochromator, optical detectors, and figures of merit. It also discusses interferences and terms to know.
Typology: Study notes
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Read: pp. 230 – 249
Problems: 9-1,3,5,6,
Figure 9-13a
λ
ε
λ
)bC = log P
o
In AAS, the flame functions as (i) sample holder, (ii) desolvation source, and (iii) volatilization source.
Figure 9-
Primary zone: C
2
, CH, and other
radical emission Secondary zone: oxygen present sostable molecular oxidesare formed for somemetals Interzonal regions: hot region, most widelyused for analysis
Figure 9-
h
ν
Optimum analysis position in the flame depends on theparticular element and its chemistry:
Figure 9-
Desired line of source is selected with monochromator:
Figure 9-
Figure 7-
n
λ
= d(sin i + sin r)
R =
λ
/
∆λ
= nN
N = grooves/mm
Properties: light gathering power, stray light rejection,
resolution, and linear dispersion
Single Single
Beam Spectrometer: Beam Spectrometer:
Figure 9-13a
Double Double
Beam Spectrometer: Beam Spectrometer:
Figure 9-13b
Detection limits: ng/mL (ppb) for flame
pg/mL (ppt) for electrothermal
Linear range: 10
3
4
for flame
2
for electrothermal
Precision: 1 – 2% RSD for flame
5 – 10% RSD for electrothermal
Accuracy: 1 –
2% for flame
% for flame
Remember: mg/L = ppm
ug/L = ppb
ng/L = ppt
Typical data for the determinationof lead (Pb
2+
) by graphite furnace
AAS in standards was 0.05 μ
g/mL (0.09 AU), 0.
μ
g/mL
μ
g/mL (0.31 AU)
and in a sample of cannedorange juice was 0.10 AU. Assume that these absorbancedata were obtained for 2
μ
aliquots of standards andsample. Calculate theconcentration of lead in theorange juice sample.
Figure 9-
Calibration equation: A = 1.4714 C + 0.015Orange juice sample: A = 0.
2
Pb
mL
/
g
058
.
0
4714
.
1
015
.
0
10
.
0
4714
.
1
015
.
0
A
C
Remember: Goal is neutral atoms in the gas phase! Remember: Goal is neutral atoms in the gas phase!
Absorption or emission of an interfering species overlaps orlies so close to the analyte absorption or emission thatresolution is not possible.
Rare with HCLs.
Presence of combustion products that exhibit broadbandabsorption or particulates that scatter radiation. Both diminishpower of transmitted beam and lead to positive errors.
If caused by fuel/oxidant mixture, then correction is possible
by running a blank and performing background subtraction.
More troublesome problem when absorption or scattering
results from the sample matrix.
Terms to Know!!!
ablation chemical interference matrix
aerosol detection limit nebulization
atomic absorption Doppler effect releasing agent
atomic emission graphite furnace self-absorption
atomic fluorescence hollow cathode lamp spectral interference
atomization ionization interference ionization suppressor
background correction
Boltzman distribution