chem 454
February 19 President's Day
ok-- here's the President's day Quiz
if you want to try it
(notes and material continues into 2/21)
Optical Atomic Spectra. Mostly Absorption
This text uses A (Angstrom)
- A usage seems to be declining; nm favored
- 1 A = 10-10 m
- 1 A= 0.1 nm
We typically treat speed of light in air
- as same as in vacuum, c
- (precise work needs a correction)
Na (doublet at 589.0, 589.6 nm)
- 5890 and 5896 A
- why a doublet ?
- electron spin
- couples with 3p
- change with energy
- no change with 3s
- two transition energies
Population of 3p state
Intensity of radiation follows Boltzmann expression
- N(3 p)/ N(3s) =3.0 * exp [-(hc/l)/(kT)]
Temperature population
- 1000 7.271E-11
- 1500 2.512E-07
- 2500 0.0001702
- 3000 0.0008682
- 3500 0.0027804
- 4000 0.0066564
- 5000 0.0225952
- 7500 0.1152704
-
2510 0.0001769
- text: 10 degree temp change at 2500 K
- produces 4% change in intensity
- contrast: in absorption, signal is proportional to 3s population
- 0.999829 at 2500 K
- 0.9991328 at 3000 K
- absorption is much less affected by temperature fluctuations
As radiation shifts from red (K) to yellow (Na) to 300 am
- population of excited state reduced
- need hotter source to excite
Line Width (of the emitted light)
Natural Line Width-- limited by Dt DE >h
- text... with 10 nsec lifetime
- line width is 1 x 10-4 A (1x10-5 nm)
Lifetime can be reduced further by collisions
- if molecule changes state on collision
- lifetime reduced to collision period
- not a problem at reduced pressures and lower temp
- worsens as pressure rises
- pressure broadening effect
- some- temperature effect
- (often it's every 5-20 collisions)
Doppler Broadening
- Dl/l = vel /c
- if vel =3 x 103 m/sec
- Dl/l= 1 x 10-5
- at 589 nm thst's 0.006 nm
- much more than natural line width
- as Temperature rises, velocity rises
- (goes as square root of Temp);
- Can give rise to unusual effects
- assume light source-is hot (broadened emission)
- but surrounded by its own vapor (narrower absorption band)
- emerging spectrum has a dip near the center of the band
- also sample of cooler vapor
- won't absorb as much light near the "wings"
Atom Sources
Heating the Sample (emission or absorption)
- mix with fuel / oxidizer / plasma gas
- nebulizer
chemically convert to volatile species
- (Occasional, specialized Player)
- As, Also Sn, Sb, Hi (Pb) as hydride
- Hg (as metal vapor)
- fed into flame as vapor
directly as a solid
- heat a small "boat" in a flame (rare}
sample ablation (arc, spark laser (sometimes)
- Electrothermal (common)
- rapid heating of graphite usually
- graphite oven in AA
Key question :which is reliable, reproducible?
Flames
fuels :natural gas , acetylene
oxidizers:
- air (wastes energy heating N2)
- oxygen (may be harder to control than air flame)
- nitrous oxide (more energetic oxidizer than 02)
flame is really a continuing explosion
- burner premixes fuel and most of the oxidized
- flame travels 40 2000 m/sec
- gas had better travel out just as fast
- faster and the flame blows out
- slower and torch backfires
- each flame has a range of gas flow rates at which it -can form stable flames
flame has hot inner "cone"
- max temp around 1 cm (0.2-2 cm)
- cool below the cone (unburnt gas)
- cooler above the cone
Ideally, biggest signal from hottest zone
- but, some species also oxidize in the falme
- (get better signal right above the cone)
- may heIp to have flame (oxygen poor with other elements
- most burners have height adjustments
Flame AA
(AES) is typically an empirical instrument
- set it up, introduce a sample
- vary height for max signal
- adjust nebulizer for maximum signal
- adjust fuel / oxidizer ratio (flame temperature)
- align lamp and burner for largest signal)
-
- or rely on typical settings, past experience
AA Instruments
- Flame (or Graphite Oven)
- Cold Cathode Lamp
- need a supply of suitable lamps
- best are single element
- but mixed cathodes (alloys) are more economical
- Chopper
- shift to lower noise frequency
- can cancel out emission from flame itself
- (may be single beam or double beam design)
- Sample Chamber (flame)
- Monochromator
- mainly to select which line
- instrument bandwidth >> line width
- Detector, usually a PMT
- typically signal averaging and log computation
AA is much noisier than in conventional spectrophotometry
- Best analysis is typically + 1%
Corrections often built in
- How much of the absorbance signal is not atomic?
Deuterium Lamp Correction
- On alternate chopper cycles use D-lamp
- UV continuum radiation
- (correct signal for any absorbance of this light)
- is quite effective when flame has small tendency to scatter light
Zeeman Effect
Lamp produces light of two polarizations
- Light is of the same frequency
If lamp or sample is placed in strong magnetic field
- Some peaks split into two components at different freq
- splitting is proportional to the field
- For light of the desired polarization the absorption band changes
- it is no longer absorbed by the samples
- Basically can turn on/off atomic absorption
- what's due to AA and what's due to Artifacts?
Quick tricks
- most elements absorb at several wavelengths
- typically to different final states
- generally, much lower absorbance at these secondary wavelengths
- can be used with much more concentrated solutions
- also, with concentrated solutions analyst often rotates burner by 90o
- reduces path length by 20-50 fold
we really want Abs 0.2 - 0.7 neighborhood
- for standards and samples
- dilute as required
- dangerous for absorption of sample to lie
- beyond calibration samples
- calibration is often not linear at high end
What are the interferences?
Rarely an adjacent atomic line, overlapping
- if so, select another line
Refractory Elements, Oxide Formation
- Most atom that form very stable oxides
- cannot be detected in cooler flames
- Al is example-- needs acetylene and N20 flame)
- These can also cause light scattering when measuring other elements
Phosphates
- can produce extremely stable compounds
- these do not dissociate well in the flame
- (may be able to avoid by forming other complexes first-- treat with chelating agent)
Ionization
- Any ions that form decrease the population of atoms
- (they have different absorption spectra)
- Easy to ionize alkali and alkaline earth elements
- can form ions even in the cooler flames
- Matrix species (like K)
- can affect degree of ionization of other components
- text example in the text- Sr shows low response (loss to ions)
- Add K and K+, e- suppresses Sr+ and Sr2+ formation
- so Sr response is much higher
- These are part of reason for Standard Additions Method
- But one can often reduce possible interferences
- add complexing agents
- add source of K+ (as above)
Atomic Fluorescence Spectroscopy (skip coverage)
- Author probably too involved in the field
- No commercial instruments
- Pretty good alternative instruments already exist
- unless replacement is much better, easier to use, more reliable, cheaper
- by a factor of 10 or more.
- not likely to get established
end 2/19
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