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FIS 340
Elemental Analysis
| Term | Definition |
|---|---|
| ways to obtain an x-ray | bombard the target with electrons (particle) or other x-rays (photons) |
| SEM-EDS- general operating principle | from a heated filament (W, Crystal), an electron beam goes through lenses (to focus it) in the vacuum column, then to the sample in its chamber. The sample's electrons are excited, and release characteristic x-rays as they relax and can then be measured. |
| XRF- general operating principle | x-ray beams are sent from their tube (Mo, Rh) to the sample, exciting the sample's electrons. As the electrons relax, they give off characteristic x-rays |
| Which elemental analysis methods are quantitative? | ICP-MS, ICP-OES, LIBS, LAICPMS (SEM-EDS and XRF are semi-quant) |
| Which elemental analysis methods are qualitative? | SEM-EDS, XRF, ICP-MS, ICP-OES, LIBS, LAICPMS |
| Classify each method as Surface, Micro-Bulk, or Bulk analysis | SEM-EDS: surface XRF: Micro-bulk ICP-MS/OES: bulk LIBS: surface or micro-bulk LAICPMS: micro-bulk |
| What is the typical LOD for each method? | SEM-EDS: 1000 ppms XRF: 100 ppms ICP-MS/OES: < 0.01 ug/L LIBS: 5-50 ppms LAICPMS: < 1 ppms |
| Classify each method's precision as poor, fair, good, or excellent | SEM-EDS: poor XRF: fair ICP-MS/OES: excellent LIBS: good LAICPMS: excellent |
| Elemental Analysis | the identification and/or quantification of elements/isotopes present in a material |
| Characteristic X-Rays | used to identify the elemental composition of materials, an energy photon generated by an inelastic collision or interaction that occurs between an external particle or photon and an atom |
| Bremsstrahlung Radiation | radiation produced from the acceleration (either + or -) of a charged particle like an electron |
| Interaction Volume | region within a sample where incident x-rays penetrate, causing atoms to fluoresce |
| plasma | a superheated gas with positively charged ions and negatively charged electrons (the fourth state of matter beyond gas) |
| isotope | atomic number (# of protons) is the same, but number of neutrons is different (chemical characteristics the same, physical properties different) |
| isobar | atomic number (# of protons) is different, but atomic weight happens to be the same so species appear at the same mass (chemical characteristics differ, physical properties similar) |
| polyatomic interference | an issue in ICP-MS analysis where two ions have the same m/z, and so cannot be distinguished from each other |
| laser ablation | a progressive and superficial destruction of a material by melting, fusion, sublimation, erosion, and explosion |
| provenance | using analysis to determine the area of origin or history about a piece of data or evidence |
| SEM-EDS source | electron beam created by the heating of a tungsten filament |
| XRF source | x-ray source (photon source: Rh, Mo) |
| ICP-MS/OES source | hot plasma- the heat ionizes the sample |
| LIBS source | laser beam |
| LAICPMS source | monochromatic laser beam |
| SEM-EDS and XRF detectors | EDS: energy dispersive spectrometry WDS: wavelength dispersive spectrometry |
| classify each method as nondestructive, minimally destructive, or destructive | SEM-EDS: Non XRF: Non ICP-MS/OES: destructive LIBS: minimally destructive LAICPMS: minimally destructive |
| SEM x and y axis units | x-axis: energy (keV) y-axis: counts |
| XRF x and y axis units | x-axis: energy (keV) y-axis: counts |
| ICP-MS x and y axis units | x-axis: m/z ratio y-axis: concentration |
| ICP-OES x and y axis units | x-axis: wavelength (nm) y-axis: intensity |
| LIBS x and y axis units | x-axis: wavelength (nm) y-axis: emission intensity |
| LAICPMS x and y axis units | x-axis: m/z ratio y-axis: counts |
| SEM-EDS sample volume | < 1 um cube |
| XRF sample volume | > 20 um cube |
| ICP-MS/OES sample volume | 2-15 mL |
| LIBS sample volume | 30-100 um diameter |
| LAICPMS sample volume | 10-100 um diameter |