Title: Instrumentation
1Instrumentation Methods ICP/MS, Uranium
- Jeff Brenner
- Minnesota Department of Health
2EPA Method 200.8Overview and Fundamentals of
ICP-MS
Determination of Metals Using Inductively Coupled
Plasma Mass Spectrometry
3Overview Fundamentals of ICP-MS What we will
cover
- Overview and Fundamentals
- ICP-MS Theory
- Interferences
- Reports
4EPA 200.8ICP-MS Definition
- An analytical technique to determine Elements
using Mass Spectrometry from Ions generated by an
Inductively Coupled Plasma. - Mass Spectroscopy
- Separation and measurement of the mass of
individual atoms making up a given material
5EPA 200.8Analytical Benefits of ICP-MS
- Rapid multi-element quantitative analysis
- Very low detection limits
- Rapid semi-quantitative analysis
- Wide dynamic range
- Isotopic analysis
- Spectral simplicity
- Speciation (with HPLC)
6EPA 200.8Isotopes and Mass Spectra
- Isotopes of an element differ in the number of
neutrons in the nucleus - U Atomic Number 92
- 234U has 142 neutrons
- 235U has 143 neutrons
- 238U has 146 neutrons
7EPA Method 200.8U Isotope Abundance
- Isotope Half Life Natural Specific
- Years Abundance Activity (pCi/ug)
- 234U 246,000 0.0055 6208.2
- 235U 700 million 0.72 2.17
- 238U 4.47 billion 99.27 0.336
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8EPA Method 200.8 Isotopes and Mass Spectra
- The Isotopic abundance of most elements is
constant - Pb may differ slightly based on the source of the
Pb - Pb is analyzed as the sum
- 206 Pb
- 207 Pb
- 208 Pb
9EPA Method 200.8 Ions and Mass Spectra
- Positive ions are produced by the energy in the
plasma - In order to utilize a mass spectrometer an ion is
necessary - ICP-MS analyze isotopic ions
- The ions are steered throughout the ion path of
the spectrometer.
10EPA Method 200.8 ICP-MS Spectrum
- A series of peaks that correspond to mass to
charge ratio (m/z) - Peaks could be the sum of different isotopes of
different elements - Doubly charged ions will appear ½ its mass
- 138Ba double charges will appear at 138/2 69
11EPA Method 200.8 Isobaric Spectral Overlaps
- Signal at given amu is the summation of all the
isotopes at that amu - It is best to avoid potential overlaps by
monitoring a clean mass - Overlaps are correctable in software
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14EPA Method 200.8 Isobaric Spectral Overlaps
- Several factors must be considered when selection
an isotope - Concentration of analyte
- Concentration of interferences
- Abundances of isotopes at the given mass
15EPA Method 200.8 Molecular Overlaps
- Polyatomic or molecular ions will occur
- Common ones are Ar, O, and H based
- Be aware of molecular overlaps that are
formed - Plasma (Ar)
- Solvents (O, H, Cl, N)
- Samples (C, Cl, S)
16EPA Method 200.8 Molecular Overlaps
- Elements in the ICP do not fully break apart and
recombination of highly concentrated elements
will occur - Example
- 56Fe and 40Ar16O
- Background spectral features have been well
characterized
17EPA Method 200.8 Factors Affecting Ion
Intensities
- Isotopic Abundance Intensity
- Intensity of an isotope is proportional to its
natural abundance - The sum of the signals from all isotopes of an
element are compared to the signal from a
mono-isotopic element, the signals ideally should
be equal - Example Element Percent Relative
- Isotope Abundance Intensity
- 55Mn 100.0 100.0
- 234U 0.0055 0.0055
- 235U 0.7200 0.7200
- 238U 99.2745 99.7245
18EPA Method 200.8 Factors Affecting Ion
Intensities
- Percent Ionization
- Element Ionized
- Na 100
- As 50
- Se 34
- F 0.001
- Most elements are ionized greater than 90.
19EPA Method 200.8 ICP-MS System
Courtesy Perkin Elmer
20EPA Method 200.8 Spray Chamber and Nebulizer
21 EPA Method 200.8 ICP-MS Ion Source Region
- Plasma creates ions from the components in the
sample. - Heat from 6,000K-10,000K dries, aerosol, then
atomize, and ionize components of the sample.
22EPA Method 200.8 ICP-MS Ion Source Region
(Plasma)
- Plasma is formed by a stream of argon gas flowing
between to quartz tubes. - Radio frequency (RF) power is applied through the
coil, and an oscillating magnetic field is
formed. - An electrical discharge creates seed electrons
and ions.
23EPA Method 200.8 ICP-MS Ion Source Region
(Plasma)
- Inside the induced magnetic field, the charged
particles are forced to flow in a closed annular
path. - As they meet resistance, heating takes place and
additional ionization occurs.
24EPA Method 200.8 Reaction Cell
- Pressurized with a reactive gas
- Convert isobar to a different ion which does not
interfere - Convert analyte to polyatomic ion which is not
interfered - The specific chemistry is dependent on
- Nature and density of the reactive gas
- Electrical fields within the cell
25EPA Method 200.8 ICP-MS Ion Source Region (Lens)
- Before sampler cone 760 torr
- Before skimmer cone 3 torr
- After skimmer cone 1e-3 torr
26EPA Method 200.8 ICP-MS Ion Source Region (Lens)
- Material extracted from the plasma are composed
of a mixture of the following - Neutral atoms (Ar) Molecules (O2)
- Positively charged atomic and molecular ions
(Ar, O2) - Reactive metastable atoms and ions
- Negatively charged atomic and molecular ions
- Photons
- Electrons
27EPA Method 200.8 ICP-MS Ion Source Region (Lens)
- The lens captures and guides the positively
charged ions to the quadrupole. - By applying a positive potential to the lens, the
ions will be focused to the center of the lens. - Small ions are optimized at lower voltages. As
the voltage is increased, higher mass ions are
better focused. - If the voltage is to high the ions are repelled.
28EPA Method 200.8 Reaction Cell or Collision Cell
- A reaction gas is introduced into the cell. The
reaction of the gas with the interfering species
is set up to remove these interferences from the
path.
29EPA Method 200.8 Quadrupole
Courtesy Perkin Elmer
- Mass Filtering System
- Separates on type of element (ion) from another
with an electromagnetic field. - Only one mass (m/z) will make it through at a
time. Many masses enter, only one makes it out.
30EPA Method 200.8 Perkin Elmer Optimization
- After initiating the plasma, allow the instrument
to warm up while aspirating a blank solution for
at least 15 minutes. - Mass Calibration Tune
- DRC II Tuning Solution
- (1 ppb Mg, In, Ce,Ba,Pb, U) and check for
responses and RSDs. Generate and evaluate a tune
report.
31Perkin Elmer DRC II Optimization Suggestions
- Suggested guidelines for an acceptable tune for
method 200.8 - Sensitivity
- Mg gt 8,000 cts/0.1 sec/10 ppb
- In gt40,000 cts/0.1 sec/10 ppb
- U gt30,000 cts/0.1 sec/10 ppb
- Precision
- Mg lt 5 RSD (0.1 sec integration time)
- In lt 5 RSD ()
- U lt 5 RSD ()
- Oxides lt 3.0
- Ba/Ba lt 3.0
- Background
- Mass 220 lt 2 cps
- Mass Accuracy /- 0.05 AMU
32EPA Method 200.8 Daily Performance Check
- Sensitivity
- Nebulizer
- Autolens
- x-y adjustment
- Detector Optimization
- Oxides to High
- Reduce nebulizer flow (plasma temperature
increases) - Dirt cones
- Reduce peristaltic pump speed
- Increase RF power
- Double Charged ions too high
- Decreased RF power
- Increase nebulizer flow
- Check skimmer 0-ring
- Poor precision
- Check entire sample introduction system
- Check the nebulizer
- Check that the correct method is used
- Perform a visual check of the plasma! Is it
stable?
33EPA Method 200.8 Isobaric Correction
- Counts at mass 114 114Cd 114Sn
- 114Cd mass 114 - 114Sn
- We cannot measure the counts of Sn at mass 114
directly since 114Cd can also be present.
However, we can measure another isotope of Sn
(118) that is free from overlap by Cd. Therefore - 114Cd mass 114 (a114Sn/a118Sn)(118Sn)
34EPA Method 200.8 Isobaric Correction
- The abundance ratio (a114Sn/a118Sn) of these two
isotopes is (0.65/24.23) and is reasonably
constant. Therefore - 114Cd mass 114 (0.65/24.23)(118Sn)
- Correction -(0.0268)(118Sn)
- 114Cd mass 114 (a114Sn/a118Sn)(118Sn)
35EPA Method 200.8 Polyatomic Correction
- Interference of Chloride on Arsenic
- High concentrations of chloride react with argon
in the plasma to form the following - 40Ar35Cl interfering on 75As
- 40Ar37Cl interfering on 77Se
- As has only one isotope at mass 75
- 40Ar35Cl can cause isobaric overlap
- Erroneously high results
- Must measure 40Ar35Cl contribution and subtract
it from the total counts at mass 75 - Total counts mass 75 counts from 75As plus
counts from 40Ar35Cl - 75As mass 75- 40Ar35Cl
36EPA Method 200.8 Polyatomic Correction
- We cannot measure the ArCl contribution at mass
75, however, we can measure the ArCl contribution
from 40Ar37Cl at mass 77 - The equation then becomes
- 75As mass 75- (a40Ar35Cl/a40Ar37cl)(40Ar37Cl)
- The relative intensities of 40Ar35Cl and 40Ar37Cl
are determined by the isotopic ratio of 35Cl to
37Cl. - 75.77/24.233.127
- 75As mass 75-3.217(40Ar37Cl)
- Correction -3.127 77Se
37EPA Method 200.8 Polyatomic Correction
- If Se is present in the sample, the correction
becomes more complicated. 77Se will contribute
intensity counts to mass 77. - Therefore, measure Se at mass 82 and multiply
the result by the ratio of 77Se to 82Se. - 75As mass 75-3.127(mass77-77Se)
- 75As mass 75-3.127(mass77-(a77Se/a82Se)82Se
- 75As mass 75-3.127(mass77-0.87482Se
- Correction -3.12777Se2.733 82Se
38EPA Method 200.8 Types of Methods Measuring
Uranium
- Total concentration method 200.8
- Uranium analysis by ICP-MS
- Results reported as ug/L
- Not very labor intensive
- Limitations
- Can not detect 234U and 235U isotope
- Conversion is accurate if isotopes are present in
natural abundance - Bias radioactivity concentration low
39EPA Method 200.8 Uranium Calculation
- Uranium radioactivity
- A (pCi/L) U (ug/L) 0.67 (pCi/ug)
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- Where A activity of uranium
- U uranium concentration
- 0.67 conversion factor
- 40 CFR part 141.25 Analytical methods for
radioactivity. - Footnote 12
40EPA Method 200.8 Types of Methods Measuring
Uranium
- Total activity method 908.0
- Uranium chemically separated
- Analyzed on alpha-beta proportional counter
- Total activity of all three uranium isotopes
- Reported as pCi/L
- Limitations
- Can not distinguish isotope
- Conversion is accurate if isotopes are present in
natural abundance - Bias mass concentration high
- Labor intensive
41EPA Method 200.8 Types of Methods Measuring
Uranium
- Isotopic activity method
- Uranium chemically separated
- Similar to total activity
- Alpha spectrometer
- Able to distinguish uranium isotope
- Results can be reported as pCi/L or ug/L
- Limitations
- Labor intensive
42EPA Method 200.8U Isotope Abundance
- Isotope 234U 235U 238U
- Half Life (years) 246,000 700 million 4.47
billion - Natural Abundance 0.0055 0.72 99.27
- Specific Activity (pCi/ug) 6,208 2.17 0.336
- Relative Intensity 0.0055 0.72 99.27
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