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Atomic Mass Spectrometry

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Presentation on theme: "Atomic Mass Spectrometry"— Presentation transcript:

1 Atomic Mass Spectrometry
Chap 11 Advantages: very low detection limits (0.02 – 0.1 ppb) spectra that are relatively simple and easy to interpret ability to measure isotopic ratios

2 General Features: Steps in the analysis Atomization Ionization of analyte atoms Separation of ions by mass-to-charge ratio (m/z) e.g., For Pb+, m/z = For Pb2+, m/z = 104 Counting or measuring ions of each m/z Units: amu or Daltons to 3 or 4 decimal places (5) Data plotted as relative intensity vs. m/z

3 Mass Spectrum Showing Natural Isotopes of Pb
Observed as an Impurity in Brass Variability in isotopic abundances in Pb from natural sources creates a large uncertainty in the atomic mass (207.2 ± 0.1).

4 Bromine 35 Br 79.904(1) Several definitions of “mass”
Atomic mass ≡ weighted avg. of masses of isotopes of an element Units: 1 amu = 1 Dalton = 1 u = 1/12 mass of 12C e.g., % 79Br with a mass = Da 49.31% 81Br with a mass = Da Gives: (1) Da for Br Bromine 35 Br (1)

5 Exact mass ≡ mass of a particular isotope of an element
e.g., 13C with an exact mass = Da Nominal mass ≡ integer mass of the species e.g., 13C with a nominal mass = 13 Da Mass-to-charge ratio (m/z) ≡ “mass” for all singly charged ions

6 Components of a Mass Spectrometer
Fig. 11-1 P = 10-5 to 10-8 torr

7 Types of Atomic Mass Spectrometers
(Distinguished by type of mass analyzer) Quadrupole MS Time-of-flight (TOF) MS Double-focusing MS Ion trap MS (covered in Chap 20)

8 Discrete dynode Fig. 11-2 (a)
Transducers for MS Electron Multipliers Discrete dynode Fig (a) dynodes Typical gain ~ 107

9 Continuous Dynode Fig. 11-2 (b)
Transducers for MS Electron Multipliers Continuous Dynode Fig (b) 1.8 – 2.0 kV Typical gain ~ 105 – 108

10 Faraday Cup Detector Fig. 11-3 The accelerated particles are stopped inside cup The accumulated electric charge is detected as a corresponding electric current.

11 Faraday Cup Detector Ion beam

12 Types of Atomic Mass Spectrometers
Quadrupole MS Time-of-flight (TOF) MS Double-focusing MS Ion trap MS (covered in Chap 20)

13 Most common type of mass analyzer for atomic MS
Quadrupole MS Fig. 11-6 Most common type of mass analyzer for atomic MS Rugged, compact, high scan rates ~ 100 ms

14 The “Mass Filter” Fig. 11-7 Constant (DC) voltage and
alternating (AC) voltage applied to rods At a particular DC voltage: Large ions tend to drift into wall Small ions spiral, travel farther, then annihilate on wall “Right size” ions spiral, are pulled back by AC, and complete the path

15 Quadrupole Mass Analyzer
Fig. 11-8 Different ions have different stability regions. As DC is ramped, ions are selected. high pass mass filter low pass mass filter both mass filters in operation

16 Voltage Relationships During a Mass Scan
Fig. 11-9

17 Types of Atomic Mass Spectrometers
Quadrupole MS Time-of-flight (TOF) MS Double-focusing MS Ion trap MS (covered in Chap 20)

18 Schematic of TOF Mass Spectrometer
Fig 11-10 Ions formed by bombardment E-field pulse accelerates ions: KE = ½ mv2 Ions then “drift” down tube (~1 ms) according to mass

19 Time-of-Flight Mass Analyzer
KE = 1/2mv2 Heavier ions in later Light ions in first

20 Schematic of ICP-MS Fig 11-10


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