ICP-MS is an analytical technique that combines an inductively coupled plasma source with a mass spectrometer to detect elemental ions. The ICP source converts atoms in a sample to ions at very high temperatures, which are then separated and detected based on their mass-to-charge ratio in the mass spectrometer. ICP-MS provides excellent detection limits and precision for elemental analysis and can detect many elements simultaneously while also allowing for isotopic analysis. The technique requires high vacuum and specialized components to generate the plasma, transmit ions into the mass spectrometer, separate ions by mass, and detect them.
ICP-MS??? Inductively CoupledPlasma Mass Spectrometry or ICP-MS is an analytical technique used for elemental determinations. An ICP-MS combines a high-temperature ICP (Inductively Coupled Plasma) source with a mass spectrometer. The ICP source converts the atoms of the elements in the sample to ions. These ions are then separated and detected by the mass spectrometer.
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Atomic Spectroscopy TechniquesThree techniques share the same basic components Atomic Absorption (Flame and Furnace) ICP-AES ICP-MS All three are used for the analysis of metals
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Comparison of TechniquesICP-MS ICP-AES GFAAS FAAS Detection Limits Excellent Good Excellent Good Productivity Excellent Excellent Low Good Precision 1-3% 0.3 – 2 % 1 – 5 % 0.1 – 1 % Chemical Interferences Moderate Few Many Many Ionization Minimal Minimal Minimal Some Mass Effects High on low mass None None None Dissolved solids 0.1 – 0.4 % 2 – 25 % Up to 20 % 0.5 – 3 % # Elements 75 73 50 68 Sample Usage Low Medium Very Low High Isotope Analysis Yes No No No Method Development Skill required Skill required Skill required Easy Running Costs High High Medium Low Capital Costs Very high High Medium Low
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ICP-MS Components •Sample Introduction • Plasma Generation • Interface • Ion Optics • Mass Analyzer • Vacuum System
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• Sample IntroductionDelivers finely divided sample (usually aerosol) to plasma • Plasma Source Ion Source Ar plasma 10 000K • Interface Allows transfer of atmospheric pressure ion source to high-vacuum mass analyser
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Ion Optics Focusesion beam and helps eliminate neutral species and photons • Mass Analyzer Separates and measures individual ions by mass • Vacuum System Provides low pressure environment for mass spectrometer to operate effectively (no collisional losses) Enables transition from plasma to high-vacuum via interface region
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The Detector Convertsions into electrical pulses Magnitude of the electrical pulse is proportional to the number of ions in sample
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Sample nebulized inspraychamber Argon transports sample and sustains plasma RF generator supplies energy to induction coil Sample atomized and ionized in the plasma Ions are transmitted through the interface, most of the gas removed Quadrupole filters the ions by mass Detector counts the ions Steps Involved in ICP-MS
Sample Introduction SystemLow uptake concentric nebulizer standard External spraychamber Double pass glass spray chamber Room temperature to -15º C Moves with torch Three channel peristaltic pump Computer controlled Smart Rinse enabled for optimized rinseout
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The Plasma • A plasma is a cloud of ionized gas • Plasma temperature 6000 - 7000 K • Most elements >90% ionized • Singly charged positive ions predominate • Small molecular and doubly charged ion population • Complete elemental analysis in a single determination
Process to formPlasma • A flow of argon gas is passed between outer and middle tube of torch • RF power is applied to load coil producing intense electromagnetic field • A high-voltage spark produces free electrons • Free electrons are accelerated by electric field • Accelerated free electrons produce high energy collision and ionization of Argon gas • Self-sustaining plasma is formed at open end of quartz torch
ICP: Why arethere four gas flows? Auxiliary Flow holds plasma away from torch/injector tube prevents torch melting Plasma Flow forms the plasma Nebulizer Flow punches cooler channel through centre of plasma carries sample Sheath Gas (some ICPMS instruments) Allows control of the velocity of the center channel independent of the sample delivery rate
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Interface: Ion SamplingTURBO-MOLECULAR PUMP VACUUM PUMP SAMPLER CONE SKIMMER CONE PLASMA ZONE OF SILENCE INTERFACE ~5 Torr ATMOSPHERE 760 Torr ROTARY ION OPTICS ~1x10 -4 Torr
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ICP-MS Cones SampleIons from the Plasma Sampler Cone Plasma encounters this cone first Skimmer Cone Located behind the sampler cone
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The Mass SpectrometerResponsible for the high sensitivity of ICPMS instruments. Separates ionized species on the basis of their mass to charge ratio. Requires high vacuum (~ 10 -6 Torr) to operate Resolution must allow detection of low concentration elements in presence of adjacent high concentration elements. Scanning speed must be fast enough to cope with transient signals from various sample introduction systems Must accept a wide distribution of ion energies
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Mass Spectrometer: CommonMass Analyzers Quadrupole Ion Trap Time of Flight Double-Focusing Magnetic Sector
Elements analysed byICP-MS in ARD Element Name Element Symbol Element Symbol Element Symbol Arsenic As Lithium Li Barium Ba Manganese Mn Beryllium Be Mercury Hg Bismuth Bi Nickel Ni Cadmium Cd Rubidium Rb Cesium Cs Selenium Se Chromium Cr Silver Ag Cobalt Co Strontium Sr Copper Cu Thallium Tl Gallium Ga Uranium U Indium In Vanadium V Lead Pb Zinc Zn
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Analysis of Samplesby ICP-MS Follow BCSIR SOP – 22 Prepare tuning solution Prepare standard solution of metals of different concentrations Always use de-ionized water having a resistivity of 17.5–18.5 MΩ/cm Use suprapure ICP-MS grade acids
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Seven Elements ofQuality Control during sample analysis by ICP-MS Certification of operator competence Calibration Analysis of externally supplied standards Analysis of blanks Analysis of duplicates Recovery of known additions Control charts
#19 11/21/11 The interface assembly provides a means of sampling the atmospheric pressure gases created in the plasma into a vacuum chamber and separates most of the unwanted gas stream from the ion beam. All ICP-MS instruments have one. Assembly always consists of two metal cones with small orifices at their tips mounted one behind the other, usually known as the “sampler” and “skimmer” cones, respectively. These are mounted in a large metal block that is water-cooled to dissipate the heat absorbed from the plasma. The region between the cones is kept at 1- 5 torr using a mechanical rotary vacuum pump. Ion extraction is performed with very little opportunity for gas-phase reactions –the gas forms a supersonic jet as it accelerates into the vacuum and cools so quickly that there is very little chance for secondary reactions to occur. The skimmer cone is placed inside the supersonic jet; ions are extracted into the mass spectrometer, most of the gases are lost as they are deflected around the tip of the cone. This results in a collimated ion beam which then passes through the ion optics for further focusing and elimination of neutral species.
#20 Plasma interface consists of two cones: a sampler cone and a skimmer cone. The skimmer cone is located downstream of the sampler cone in the instrument. The function of the cones is to enable sampling of ions from the plasma.
#22 11/21/11 There are many different types of mass spectrometers (used in many other instruments besides ICPMS). All of the types of mass spectrometers listed above have been used for ICPMS, but we will focus in this presentation on the quadrupole mass spectrometer, as this configuration is used in the vast majority of all ICPMS instruments.
#23 11/21/11 For a given set of RF/DC conditions in the quadrupole, only one mass will have a stable trajectory through the mass analyzer, all other ions will be lost. The RF/DC settings can be altered very quickly (<1ms) and this is how the mass spectrometer scans across the entire mass range. Precision assembly of 4 electrically conducting rods to which RF and DC voltages are applied opposing rod pairs, opposite polarity resulting electric fields in the center of the assembly filters the ions by mass only one mass/charge ratio has stable trajectory, others are excluded RF/DC ratio determines resolution Rigid, stable geometry, no moving parts Compact size Accepts ions of a wide energy range Good resolution/mass range capabilities for atomic spectroscopy