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[http://www.iscpubs.com/articles/index.php?3-al_all-al/a0403ell.pdf] </ref> <ref> ''Shane Elliott, Barry Sturman, Stephen Anderson, Elke Brouwers, Jos Beijnen'', ICP-MS: When Sensitivity Does Matter, Spectroscopy Magazine, [[April 1]], [[2007]]. [http://www.spectroscopymag.com/spectroscopy/article/articleDetail.jsp?id=440521&pageID=1&sk=&date=]
[http://www.iscpubs.com/articles/index.php?3-al_all-al/a0403ell.pdf] </ref> <ref> ''Shane Elliott, Barry Sturman, Stephen Anderson, Elke Brouwers, Jos Beijnen'', ICP-MS: When Sensitivity Does Matter, Spectroscopy Magazine, [[April 1]], [[2007]]. [http://www.spectroscopymag.com/spectroscopy/article/articleDetail.jsp?id=440521&pageID=1&sk=&date=]
</ref> <ref>{{cite journal | author = Vladimir N. Epov, R. Douglas Evans, Jian Zheng, O. F. X. Donard and
</ref> <ref>{{cite journal | author = Vladimir N. Epov, R. Douglas Evans, Jian Zheng, O. F. X. Donard and
Masatoshi Yamada | title = Rapid fingerprinting of <sup>239</sup>Pu and <sup>240</sup>Pu in environmental samples with high U levels using on-line ion chromatography coupled with high-sensitivity quadrupole ICP-MS detection | journal = [[J. Anal. At. Spectrom.]] | year = 2007 | volume = 22 | pages = 1131–1137 | doi = 10.1039/b704901c.pdf | doi_brokendate = 2008-09-08}}</ref>
Masatoshi Yamada | title = Rapid fingerprinting of <sup>239</sup>Pu and <sup>240</sup>Pu in environmental samples with high U levels using on-line ion chromatography coupled with high-sensitivity quadrupole ICP-MS detection | journal = [[J. Anal. At. Spectrom.]] | year = 2007 | volume = 22 | pages = 1131–1137 | doi = 10.1039/b704901c}}</ref>


===Dynamic reaction cell===
===Dynamic reaction cell===
Introduced by [[Perkin-Elmer]] on their Elan DRC (followed by Elan DRC II and Elan DRC-e) instrument, the Dynamic Reaction Cell is a chamber placed before the traditional [[quadrupole]] room of an ICP-MS device, for eliminating isobaric interferences.<ref>{{cite journal | title = A dynamic reaction cell for ICP-MS. Part 1: The rf-field energy contribution in thermodynamics of ion-molecule reactions | author = V. Baranov, S. Tanner | journal = [[J. Anal. At. Spectrom.]] | year = 1999 | volume = 14 | pages = 1133–1142 | doi = 10.1039/a809889a}}</ref> <ref>{{cit ejournal | title = A dynamic reaction cell for ICP-MS. Part 2: Reduction of interferences produced within the cell | author = S. Tanner, V. Baranov | journal = [[J. Am. Soc. Mass Spectrom.]] | year = 1999 | volume = 10 | pages = 1083-1094 | doi = 10.1016/S1044-0305(99)00081-1}}</ref> <ref>A beginner's Guide to ICP-MS ''R. Thomas'' [http://www.spectroscopymag.com]</ref> <ref>{{cite journal | title = Reaction cells and collision cells for ICP-MS: a tutorial review | author = S. Tanner, V. Baranov, D. Bandura | journal = [[Spectrochimica Acta]] B | volume = 57 | year = 2002 | pages = 1361–1452 | doi = 10.1016/S0584-8547(02)00069-1}}</ref> The room has a quadrupole (do not confuse this quadrupole with the main one, placed after DRC and before the detector, which has longer rods and is, in general, bigger) and can be filled-up with so-called reaction (or collision) gases (ammonia, methane, oxygen or hydrogen), with one gas type at a time or a mixture of two of them, which reacts with the introduced sample, eliminating some of the interference.
Introduced by [[Perkin-Elmer]] on their Elan DRC (followed by Elan DRC II and Elan DRC-e) instrument, the Dynamic Reaction Cell is a chamber placed before the traditional [[quadrupole]] room of an ICP-MS device, for eliminating isobaric interferences.<ref>{{cite journal | title = A dynamic reaction cell for ICP-MS. Part 1: The rf-field energy contribution in thermodynamics of ion-molecule reactions | author = V. Baranov, S. Tanner | journal = [[J. Anal. At. Spectrom.]] | year = 1999 | volume = 14 | pages = 1133–1142 | doi = 10.1039/a809889a}}</ref> <ref>{{cite journal | title = A dynamic reaction cell for ICP-MS. Part 2: Reduction of interferences produced within the cell | author = S. Tanner, V. Baranov | journal = [[J. Am. Soc. Mass Spectrom.]] | year = 1999 | volume = 10 | pages = 1083-1094 | doi = 10.1016/S1044-0305(99)00081-1}}</ref> <ref>A beginner's Guide to ICP-MS ''R. Thomas'' [http://www.spectroscopymag.com]</ref> <ref>{{cite journal | title = Reaction cells and collision cells for ICP-MS: a tutorial review | author = S. Tanner, V. Baranov, D. Bandura | journal = [[Spectrochimica Acta]] B | volume = 57 | year = 2002 | pages = 1361–1452 | doi = 10.1016/S0584-8547(02)00069-1}}</ref> The room has a quadrupole (do not confuse this quadrupole with the main one, placed after DRC and before the detector, which has longer rods and is, in general, bigger) and can be filled-up with so-called reaction (or collision) gases (ammonia, methane, oxygen or hydrogen), with one gas type at a time or a mixture of two of them, which reacts with the introduced sample, eliminating some of the interference.
The DRC is characterized by the following paramters, that can be modified: RPq (the corresponding q parameter from the [[Mathieu equation]]), RPa (the corresponding a parameter from the [[Mathieu equation]]), which refer to the voltage applied to the quadrupole rods and the gas flow of the reaction gas.
The DRC is characterized by the following paramters, that can be modified: RPq (the corresponding q parameter from the [[Mathieu equation]]), RPa (the corresponding a parameter from the [[Mathieu equation]]), which refer to the voltage applied to the quadrupole rods and the gas flow of the reaction gas.
Ammonia gas is the best solution for the majority of interferences, but it is far for being the perfect gas. Sometimes, for specific isotopes, other gas must be used for better results or even mathematical correction, if no gas offers a satisfactory advantage.
Ammonia gas is the best solution for the majority of interferences, but it is far for being the perfect gas. Sometimes, for specific isotopes, other gas must be used for better results or even mathematical correction, if no gas offers a satisfactory advantage.

Revision as of 08:55, 8 September 2008

Inductively coupled plasma mass spectrometry
ICP-MS Instrument
AcronymICP-MS
ClassificationMass spectrometry
AnalytesInorganic compounds
Organometallics
Other techniques
RelatedInductively coupled plasma atomic emission spectroscopy

ICP-MS (Inductively coupled plasma mass spectrometry) is a type of mass spectrometry that is highly sensitive and capable of the determination of a range of metals and several non-metals at concentrations below one part in 1012. It is based on coupling together an inductively coupled plasma as a method of producing ions (ionization) with a mass spectrometer as a method of separating and detecting the ions. ICP-MS is also capable of monitoring isotopic speciation for the ions of choice.

Categories

  • ICP (Inductively Coupled Plasma) - A plasma is a gas that contains a sufficient concentration of ions and electrons to make the gas electrically conductive. The plasmas used in spectrochemical analysis are essentially electrically neutral, with each positive charge on an ion balanced by a free electron. In these plasmas the positive ions are almost all singly-charged and there are few negative ions, so there are nearly equal numbers of ions and electrons in each unit volume of plasma

An inductively coupled plasma (ICP) for spectrometry is sustained in a torch that consists of three concentric tubes, usually made of quartz. The end of this torch is placed inside an induction coil supplied with a radio-frequency electric current. A flow of argon gas (usually 14 to 18 liters per minute) is introduced between the two outermost tubes of the torch and an electrical spark is applied for a short time to introduce free electrons into the gas stream. These electrons interact with the radio-frequency magnetic field of the induction coil and are accelerated first in one direction, then the other, as the field changes at high frequency (usually 27.12 million cycles per second). The accelerated electrons collide with argon atoms, and sometimes a collision causes an argon atom to part with one of its electrons. The released electron is in turn accelerated by the rapidly-changing magnetic field. The process continues until the rate of release of new electrons in collisions is balanced by the rate of recombination of electrons with argon ions (atoms that have lost an electron). This produces a ‘fireball’ that consists mostly of argon atoms with a rather small fraction of free electrons and argon ions. The temperature of the plasma is very high, of the order of 10,000 K.

The ICP can be retained in the quartz torch because the flow of gas between the two outermost tubes keeps the plasma away from the walls of the torch. A second flow of argon (around 1 liter per minute)is usually introduced between the central tube and the intermediate tube to keep the plasma away from the end of the central tube. A third flow (again usually around 1 liter per minute) of gas is introduced into the central tube of the torch. This gas flow passes through the centre of the plasma, where it forms a channel that is cooler than the surrounding plasma but still much hotter than a chemical flame. Samples to be analyzed are introduced into this central channel, usually as a mist of liquid formed by passing the liquid sample into a nebulizer.

As a droplet of nebulized sample enters the central channel of the ICP, it evaporates and any solids that were dissolved in the liquid vaporize and then break down into atoms. At the temperatures prevailing in the plasma a significant proportion of the atoms of many chemical elements are ionized, each atom losing its most loosely-bound electron to form a singly charged ion.

  • MS (Mass Spectrometry) the ions from the plasma are extracted through a series of cones into a mass spectrometer, usually a quadrupole. The ions are separated on the basis of their mass-to-charge ratio and a detector receives an ion signal proportional to the concentration.

The concentration of a sample can be determined through calibration with elemental standards. ICP-MS also lends itself to quantitative determinations through Isotope Dilution, a single point method based on an isotopically enriched standard.

Other mass analyzers coupled to ICP systems include double focusing magnetic-electrostatic sector systems with both single and multiple collector, as well as time of flight systems (both axial and orthogonal accelerators have been used).

Other types of spectrometers using ICP is ICP-AES (Atomic Emission Spectrometer) and ICP-OES (Optical Emission Spectrometer).

Routine Maintenance

As with any piece of instrumentation or equipment, there are many aspects that need to be encompassed in daily, weekly and annually maintenance procedures. The frequency of maintenance is typically defined by the sample volume and cummulative run time that the instrument is subjected to. One of the first things that should be carried out before the calibration of the ICP-MS, is a sensitivity check and optimization. This ensures that the operator is aware of any possible issues with the instrument and if so, to address them before begining a calibration. Typical indicators of sensitivity are Rhodium levels, Cerium/Oxide ratios and DI water blanks. One of the most frequent forms of routine maintenance is changing out sample and waste tubing on the peristaltic pump, as these tubes can get worn fairly quickly resulting in holes and clogs in the sample line, resulting in skewed results. Other parts that will need regular cleaning and/or replacing are: sample tips, nebulizer tips, sample cones, skimmer cones, injector tubes, torches and lenses. It may also be necessary to change the oil in the roughing and vacuum pumps, depending on the workload put on the instrument.

Metal speciation

A growing trend in the world of elemental analysis has revolved around the speciation of certain metals such as chromium and arsenic. One of the primary techniques to achieve this is to use an ICP-MS in combination with an HPLC. There are many advantages, from a clinical standpoint, in knowing the specific species present within a patient's body. For example, one species of chromium, known as Chromium III or Trivalent Chromium, is needed by the body and causes no ill effects; however, Chromium VI or Hexavalent Chromium, is very toxic to the body. Chromium VI will not only cause cancer and other serious medical issues to the exposed individual, but can also cause genetic mutations to occur within the person, meaning that any offspring produced can potentially be affected.[citation needed]

It is also beneficial for a clinician to utilize speciation analysis from a preventative standpoint. Many patients, who suffer from elevated levels of certain metals, do not know when or where the exposure incident(s) are occurring. By identifying the exact species, a physician can better narrow the search for possible exposure sites, therefore helping the patient to avoid certain areas in the future.[citation needed]

Quantification of proteins and biomolecules by ICP-MS

There is an increasing trend of using ICP-MS as a tool in Speciation Analysis, which normally involves a front end chromatograph separation and an elemental selective detector, such as AAS and ICP-MS. For example, ICP-MS may be combined with size exclusion chromatography and quantitative preparative native continuous polyacrylamide gel electrophoresis (QPNC-PAGE) for identifying and quantifying native metal cofactor containing proteins in biofluids. Also the phosphorylation status of proteins can be analyzed.

Recently a new type of protein tagging reagents called metal coded affinity tags (MeCAT) were introduced to label proteins quantitatively with metals, especially lanthanides.[1] The MeCAT labelling allows relative and absolute quantification of all kind of proteins or other biomolecules like peptides. MeCAT comprises a site-specific biomolecule tagging group with at least a strong chelate group which binds metals. The MeCAT labelled proteins can be accurately quantified by ICP-MS down to low attomol amount of analyte which is at least 2-3 orders of magnitude more sensitive than other mass spectrometry based quantification methods. By introducing several MeCAT labels to a biomolecule and further optimization of LC-ICP-MS detection limits in the zeptomol range are within the realms of possibility. By using different lanthanides MeCAT multiplexing can be used for pharmacokinetics of proteins and peptides or the analysis of the differential expression of proteins (proteomics) e.g. in biological fluids. Breakable PAGE SDS-PAGE (DPAGE, dissolvable PAGE), two-dimensional gel electrophoresis or chromatography is used for separation of MeCAT labelled proteins. Flow-injection ICP-MS analysis of protein bands or spots from DPAGE SDS-PAGE gels can be easily performed by dissolving the DPAGE gel after electrophoresis and staining of the gel. MeCAT labelled proteins are identified and relatively quantified on peptide level by MALDI-MS or ESI-MS.

Sample introduction

The first step in analysis is the introduction of the sample. This has been achieved in ICP-MS through a variety of means.

The most common method is the use of a nebulizer. This is a device which converts liquids into an aerosol, and that aerosol can then be swept into the plasma to create the ions. Nebulizers work best with simple liquid samples (i.e. solutions). However, there have been instances of their use with more complex materials like a slurry. Many varieties of nebulizers have been coupled to ICP-MS, including pneumatic, cross-flow, Babington, ultrasonic, and desolvating types. The aerosol generated is often treated to limit it to only smallest droplets, commonly by means of a double pass or cyclonic spray chamber. Use of autosamplers makes this easier and faster.

Less commonly, the laser ablation has been used as a means of sample introduction. In this method, a laser is focused on the sample and creates a plume of ablated material which can be swept into the plasma. This is particularly useful for solid samples, though can be difficult to create standards for leading the challenges in quantitative analysis.

Other methods of sample introduction are also utilized. Electrothermal vaporization (ETV) and in torch vaporization (ITV) use hot surfaces (graphite or metal, generally) to vaporize samples for introduction. These can use very small amounts of liquids, solids, or slurries. Other methods like vapor generation are also known.

Transfer of ions into vacuum

The carrier gas (usually argon or occasionally helium) is sent through the central channel and into the very hot plasma. The sample is then exposed to radio frequency which converts the gas into a plasma. The high temperature of the plasma is sufficient to cause a very large portion of the sample to form ions. This fraction of ionization can approach 100% for some elements (e.g. sodium), but this is dependent on the ionization potential. A fraction of the formed ions passes through a ~1mm hole (sampler cone) and then a ~0.4mm hole (skimmer cone). The purpose of which is to allow a vacuum that is required by the mass spectrometer.

The vacuum is created and maintained by a series of pumps. The first stage is usually based on a roughing pump, most commonly a standard rotary vane pump. This removes most of the gas and typically reaches a pressure of around 133 Pa. Later stages have their vacuum generated by more powerful vacuum systems, most often turbomolecular pumps. Older instruments may have used oil diffusion pumps for high vacuum regions.

Sample Preparation

For most clinical methods using ICP-MS, there is a relativley simple and quick sample prep process. The main component to the sample is an internal standard, which also serves as the diluent. This internal standard consists primarily of deionized water, with nitric or hydrochloric acid, and Indium and/or Gallium. Depending on the sample type, usually 5 ml of the internal standard is added to a test tube along with 10-500 microliters of sample. This mixture is then vortexed for several seconds or until mixed well and then loaded onto the autosampler tray. For other applications that may involve very viscous samples or samples that have particulate matter, a process known as sample digestion may have to be carried out, before it can be pipetted and analyzed. This adds an extra first step to the above process, and therefore makes the sample prep more lengthy.

Ion Optics

Before mass separation, a beam of positive ions has to be extracted from the plasma and focused into the mass-analyzer. It is important to separate the ions from UV photons, energetic neutrals and from any solid particles that may have been carried into the instrument from the ICP. Traditionally, ICP-MS instruments have used transmitting ion lens arrangements for this purpose. Examples include the Einzel lens, the Barrel lens, Agilent's Omega Lens [2] and Perkin-Elmer's Shadow Stop [3]. Another approach is to use ion guides (quadrupoles, hexapoles, or octopoles) to guide the ions into mass analyzer along a path away from the trajectory of photons or neutral particles. Yet another approach is Varian patented [4] 90 degrees reflecting "Ion Mirror" optics, which are claimed to provide more efficient ion transport into the mass-analyzer, resulting in better sensitivity and reduced background [5] [6] [7]

Dynamic reaction cell

Introduced by Perkin-Elmer on their Elan DRC (followed by Elan DRC II and Elan DRC-e) instrument, the Dynamic Reaction Cell is a chamber placed before the traditional quadrupole room of an ICP-MS device, for eliminating isobaric interferences.[8] [9] [10] [11] The room has a quadrupole (do not confuse this quadrupole with the main one, placed after DRC and before the detector, which has longer rods and is, in general, bigger) and can be filled-up with so-called reaction (or collision) gases (ammonia, methane, oxygen or hydrogen), with one gas type at a time or a mixture of two of them, which reacts with the introduced sample, eliminating some of the interference. The DRC is characterized by the following paramters, that can be modified: RPq (the corresponding q parameter from the Mathieu equation), RPa (the corresponding a parameter from the Mathieu equation), which refer to the voltage applied to the quadrupole rods and the gas flow of the reaction gas. Ammonia gas is the best solution for the majority of interferences, but it is far for being the perfect gas. Sometimes, for specific isotopes, other gas must be used for better results or even mathematical correction, if no gas offers a satisfactory advantage.

CRI technology

The proprietary Collisional Reaction Interface (CRI) [12] technology used in the Varian ICP-MS is another effective approach to destroying interfering ions. These ions are removed by injecting a collisional gas (He), or a reactive gas (H2), or a mixture of the two, directly into the plasma as it flows through the skimmer cone and/or the sampler cone. Supplying the reactive/collisional gas into the tip of the skimmer cone and/or into the tip of the sampler cone induces extra collisions and reactions that destroy polyatomic ions in the passing plasma.

Axial field technology

Axial field technology (AFT) is a patented improvement of DRC made by Perkin-Elmer, which consists in two supplementary rods placed in the DRC room, smaller than normal quadrupole's rods, with the purpose of "pushing" the ions faster to the exit by generating a supplementary electric potential, minimizing the time needed for the gas to be in the DRC and improving analysis speed. The suplimetary potential of the AFT rods does not contribute significantly to the global energy, but drastically improve ion pasage time.

Collision cell technology with kinetic energy discrimination (CCT-KED)

Thermo Scientific's XSeries2 instrument utilizes a collision/reaction cell for interference removal, consisting of a non-consumable hexapole and chicane ion deflector, which takes the ion beam off-axis and leads to low instrument backgrounds of <0.5 integrated counts per second (icps) at vacant masses such as 5 and 220. This hexapole is inherently part of the Thermo lens system and is present in the ion path, regardless of the use of the collision cell. The collision/reaction gas mixtures can be 1% NH3 in He, 7% H2 in He and 100% H2, where the NH3 and H2 are reactive gasses and the He is a collisional gas. The 3rd generation cell utilizes kinetic energy discrimination, which employes running the quadrupole bias slightly less negative (more positive) than the hexopole bias. Polyatomic ions generated within the plasma can have larger atomic radii than analyte ions of similar mass, i.e. the interferent NaAr+ (mass 63) is larger than the analyte Cu+ (mass 63). Thus, when using a collisional/reactive gas mixture, these larger species undergo more collisions/reactions in the cell, in which they lose increasingly more energy, and are then excluded from the quadrupole mass filter by the kinetic energy barrier.

Other implementations

Another implementation of this type of interference removal is an octopole (instead of a quadrupole) collision cell, implemented by Agilent's 7500 series. The ORS (Octopole Reaction System) uses only helium or hydrogen and the volume of the cell is smaller than that of a DRC. The small molecules of helium and hydrogen collide with the large, unwanted polyatomic ions formed in the plasma and break them up into other ions that can be separated in the quadrupole mass analyser. However, unlike the DRC the OCR system is based only on collision reactions and not on chemical reactions.

Plasma

The plasma used in an ICP-MS is made by ionizing argon gas (Ar → Ar+ + e-). The energy required for this reaction is obtained by pulsing an electrical current in wires that surround the argon gas. A complete description of plasma generation is given in the following section.

After injecting the sample, the plasma's extreme temperature causes the sample to separate into individual atoms (atomization). Next, the plasma ionizes these atoms (M → M+ + e-) so that they can be detected by the mass spectrometer.

Plasma Generation

An inductively coupled plasma (ICP) for spectrometry is sustained in a torch that consists of three concentric tubes, usually made of quartz. The end of this torch is placed inside an induction coil supplied with a radio-frequency electric current. A flow of argon gas (usually 14 to 18 liters per minute) is introduced between the two outermost tubes of the torch and an electrical spark is applied for a short time to introduce free electrons into the gas stream. These electrons interact with the radio-frequency magnetic field of the induction coil and are accelerated first in one direction, then the other, as the field changes at high frequency (usually 27.12 million cycles per second). The accelerated electrons collide with argon atoms, and sometimes a collision causes an argon atom to part with one of its electrons. The released electron is in turn accelerated by the rapidly-changing magnetic field. The process continues until the rate of release of new electrons in collisions is balanced by the rate of recombination of electrons with argon ions (atoms that have lost an electron). This produces a ‘fireball’ that consists mostly of argon atoms with a rather small fraction of free electrons and argon ions.

Advantage of Argon

Making the plasma from argon, instead of other gases, has several advantages. First, argon is abundant (in the atmosphere, as a result of the radioactive decay of potassium) and therefore cheaper than other noble gases. Argon also has a higher first ionization potential than all other elements except He, F, and Ne. Because of this high ionization energy, the reaction (Ar+ + e- → Ar) is more energetically favorable than the reaction (M+ + e- → M). This ensures that the sample (M+) remains ionized so that the mass spectrometer can detect it.

Elemental analysis

The ICP-MS allows determination of elements with atomic mass ranges 7 to 250. This encompasses Li to U. Some masses are prohibited such as 40 due to the abundance of argon in the sample. Other blocked regions may include mass 80 (due to the argon dimer), and mass 56 (due to ArO), the latter of which greatly hinders Fe analysis unless the instrumentation is fitted with a reaction chamber.

A typical ICP-MS will be able to detect in the region of nanograms per litre to 10 or 100 milligrams per litre or around 8 orders of magnitude of concentration units.

Unlike atomic absorption spectroscopy, which can only measure a single element at a time ICP-MS has the capability to scan for all elements simultaneously. This allows rapid sample processing.

Usage

One of the largest volume uses for ICP-MS is in the medical and forensic field, specifically, toxicology. A physcian may order a metal assay for a number of reasons, such as suspiscion of heavy metal poisoning, metabolic concerns, and even hepatological issues. Depending on the specific parameters unique to each patient's diagnostic plan, samples collected for analysis can range from whole blood, urine, plasma, serum, to even packed red blood cells. Another primary use for this instrument lies in the environmental field. Such applications include water testing for municipalities or private individuals all the way to soil, water and other material analysis for industrial purposes.

In recent years, industrial and biological monitoring has presented another major need for metal analysis via ICP-MS. Individuals working in plants where exposure to metals is likely and unavoidable, such as a battery factory, are required by their employer, to have their blood or urine analyzed for metal toxicity on a regular basis. This monitoring has become a manditory practice implemented by OSHA, in an effort to protect workers from their work environment and ensure proper rotation of work duties (i.e. rotating employees from a high exposure position to a low exposure position).

Regardless of the sample type, blood, water, etc., it is important that it be free of clots or other particulate matter, as even the smallest clot can disrupt sample flow and block or clog the sample tips within the spray chamber.

ICP is used for motor oil analysis. Analyzing used motor oil reveals a great deal about how the engine is operating. Parts that wear in the engine will deposit traces in the oil which can be detected with ICP. ICP analysis can help to determine whether parts are failing. In addition, ICP can determine what amount of the original oil additives remain, and tell how much service life the oil has remaining. Oil analysis is often used by fleet manager or automotive enthusiasts who have an interest in finding out as much about their engine's operation as possible.

References

  1. ^ Ahrends R, Pieper S, Kühn A; et al. (2007). "A metal-coded affinity tag approach to quantitative proteomics". Molecular & Cellular Proteomics. 6: 1907. doi:10.1074/mcp.M700152-MCP200. PMID 17627934. {{cite journal}}: Explicit use of et al. in: |author= (help)CS1 maint: multiple names: authors list (link) CS1 maint: unflagged free DOI (link)
  2. ^ Kenichi Sakata et al, Inductively coupled plasma mass spectrometer and method, US patent 6265717 B1.
  3. ^ Scott D. Tanner et al, Device and method preventing ion source gases from entering reaction cell, US patent 6639665 B2.
  4. ^ Iouri Kalinitchenko, Ion Optical System for a Mass Spectrometer, United States Patent Number 6,614,021 B1 (2003).
  5. ^ Shane Elliott, Michael Knowles, and Iouri Kalinitchenko, A Change in Direction in ICP-MS, published on Mar, 2004 in American Laboratory, [1]
  6. ^ Shane Elliott, Barry Sturman, Stephen Anderson, Elke Brouwers, Jos Beijnen, ICP-MS: When Sensitivity Does Matter, Spectroscopy Magazine, April 1, 2007. [2]
  7. ^ Vladimir N. Epov, R. Douglas Evans, Jian Zheng, O. F. X. Donard and Masatoshi Yamada (2007). "Rapid fingerprinting of 239Pu and 240Pu in environmental samples with high U levels using on-line ion chromatography coupled with high-sensitivity quadrupole ICP-MS detection". J. Anal. At. Spectrom. 22: 1131–1137. doi:10.1039/b704901c. {{cite journal}}: line feed character in |author= at position 68 (help)CS1 maint: multiple names: authors list (link)
  8. ^ V. Baranov, S. Tanner (1999). "A dynamic reaction cell for ICP-MS. Part 1: The rf-field energy contribution in thermodynamics of ion-molecule reactions". J. Anal. At. Spectrom. 14: 1133–1142. doi:10.1039/a809889a.
  9. ^ S. Tanner, V. Baranov (1999). "A dynamic reaction cell for ICP-MS. Part 2: Reduction of interferences produced within the cell". J. Am. Soc. Mass Spectrom. 10: 1083–1094. doi:10.1016/S1044-0305(99)00081-1.
  10. ^ A beginner's Guide to ICP-MS R. Thomas [3]
  11. ^ S. Tanner, V. Baranov, D. Bandura (2002). "Reaction cells and collision cells for ICP-MS: a tutorial review". Spectrochimica Acta B. 57: 1361–1452. doi:10.1016/S0584-8547(02)00069-1.{{cite journal}}: CS1 maint: multiple names: authors list (link)
  12. ^ I. Kalinitchenko, Patent Application under the Patents Cooperation Treaty WO 2004/012223 A1