Chapter 8: An Introduction to Optical Atomic Spectrometry
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Chapter 8: An Introduction to Optical Atomic Spectrometry
Optical Atomic Spectra. • Atomization Methods. • Sample Introduction Methods. -
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Chapter 8: An Introduction to Optical Atomic Spectrometry • Optical Atomic Spectra • Atomization Methods • Sample Introduction Methods - Optical Spectrometry as opposed to MS - Optics are similar to Molecular Absorption and Fluorescence Spectrometry
Basics - Generally solution samples (sometimes solids) - Aspirate sample into flame or plasma - Or heat sample to atomize - Observe emission from excited state (AE) - Or use light source to measure atomic absorption (AA) - Or use light source to generate atomic fluorescence (AF)
Atomic spectra are line spectra
Some prominent lines in the atomic spectrum of mercury (Hg)
Other atomic spectra – many lines per spectra, lines are very narrow
λ in Å Absorption & emission lines come from discrete transitions
λ in Å Absorption & emission lines come from discrete transitions
Resonance fluorescence lines Others involve the ground involve a two state step process
Atomic line widths are important when considering spectral resolution, absorption experiments, etc.
Doppler broadening occurs due to the observed compression and expansion of light waves as an atom moves toward or away from the radiation source
Other broadening effects include - pressure or collisional broadening (10-4 Å) - broadening from uncertainty effects - electric & magnetic field effects Temperature effects from Boltzmann equation Pj Ej Nj ----- = ------ exp - -----Po kT No N = population of state P = statistical factor Ej = energy difference k = Boltzmann constant T = temp o & j signify ground & excited states
Molecular emission in flames & plasmas is generally unwanted may obscure part of the spectrum & cause interference
Note similarity of spectra
Hollow Cathode Lamp (HCL) and Electrodeless Discharge Lamp (EDL)
These lamps produce only the spectral output from the element of interest and therefore are ideally suited to atomic absorption experiments
The sample must be converted to its atomic state which can be done at high temp. in a flame, furnace, plasma, arc or spark
Introducing the sample to the high temperature source can be tricky
Pneumatic nebulizers a) concentric tube b) cross-flow c) fritted disk d) Babington
Solid sample introduction: 1) Laser ablation – zap sample with laser and sweep atoms into flame/plasma 2) Direct sample insertion – place sample directly in atomizer (e.g. furnace) 3) Electrothermal atomizers – electrically heat graphite or tantalum boat 4) Arc/Spark ablation – coat sample on electrode or place in electrode well or cup 5) Glow discharge technique – see p 204
Chapter 9: Atomic Absorption & Atomic Fluorescence Spectrometry • Sample Atomization • Atomic Absorption (AA) • Atomic Fluorescence (AF) - Both AA and AF require a light source - Like Molecular Absorption & Fluorescence, in AA high intensity is NOT required, in AF high intensity results in greater sensitivity
occurs in flame, plasma, etc. Molecular emission is generally unwanted & can cause interference AA