Overview of Mass Spectrometry - PowerPoint PPT Presentation

1 / 63
About This Presentation
Title:

Overview of Mass Spectrometry

Description:

fax = ( 2qVtrap/md2)1/2. d = distance between trapping plates (1% term) ... SIMS: Secondary Ion Mass Spec. Ion beams: easy to create, but charges the ... – PowerPoint PPT presentation

Number of Views:510
Avg rating:3.0/5.0
Slides: 64
Provided by: johnba93
Category:

less

Transcript and Presenter's Notes

Title: Overview of Mass Spectrometry


1
Overview of Mass Spectrometry
Instrumentation and Methods Chem 553
Spring 2009
2
  • Mass Spectrometry
  • Unlike other spectroscopies!
  • Others
  • radiation in, modified radiation out
  • infer structure from difference in
  • intensity as function of frequency
  • MS
  • Weigh molecules and their pieces
  • Vaporize
  • Ionize (can be conjoint with 1.)
  • Mass Sort
  • Detect
  • Interpret

3
  • Vaporize
  • (1) Thermal
  • Background vacuum typically 10-6 torr
  • need sample at 10-3 torr vapor pressure.
  • If you can get it through a GC, it's okay
  • T lt250 C typically
  • (organics pyrolize at gt250 C)
  • Gas/GC/ Solid probe
  • Sputter with beam (photon, ion, neutral)
  • from solid or liquid matrix
  • (3) Spray (LC, Electrospray)

4
2. Ionize Electron ionization M
energetic e- ? M. e- ( original e-)
Universal, cheap 1 milliAmp/1 year 0.03
typically 70 V electron acceleration Thermodynam
ics Ionization Energy (IE) ?E0K
Radical cations higher in energy than
isostructural neutral Range of IEs 4-24 eV
1 eV 23.06 kcal 98.5 kJ
5
Ionization Energy IE (thermodynamics)
(formerly Ionization Potential IP) Cs
3.89 CH4 12.5 tBu
6.58 H2 15.4 PhCH2 7.6
Ne 21.6 benzene 9.2
He 24.6 MeOH 10.8 Tables NIST
Webbook http//webbook.nist.gov/chemistry -
Recombination energy M. e- ? M - Vertical
vs. adiabatic (next slide) - Appearance Energy
(of fragment) AE - Plateau region
6
M.
IEv
IEad
M0
EDEv
M-.
EAad
7
Fragmentation ABC ? ABC. ? AB C.
? A BC.
? A B C
? AC B.  (Rearrangements)
Mechanism of Ionization not billiard ball
70 eV 1614 kcal/mol 2 of c gt C, H, CH
- electric field of fast near-miss electron
yields electronic excited state. - If
excited state in continuum, can lose electron or
fragment with excess energy.
8
(No Transcript)
9
Formation of Anions by EI much rarer (usually
1-3 of amount of cations generated, if
any at all) Reason anion will detach electron
if higher in energy than neutral
(negative electron affinity) if seen, more
stable than neutral EA 0 to 10 eV
(most organic anions are 0 to 4 eV EA) but if
stable anion A e- ?(A-.) ?
A e- electron attachment yields excited
anion, which can detach the electron.
10
M.
IEv
IEad
M0
EDEv
M-.
EAad
11
  • Electron Ionization Practical Aspects
  • hot filament (wire or ribbon) emits electrons,
    due
  • to low work function (Re, W, ThO2 )
  • why is rhenium important to UT Chemistry?
  • - filament current few amps (yellow hot)
  • - electron beam current nanoamps to microamps
  • - Often a small magnet to collimate beam
  • - Continuous

12
(No Transcript)
13
Analyzers Magnetic sector
14
Mass Selection F zq(v x B) Lorentz
equation centrifugal
force F mv2/r centripetal force
mv/z q.r.B Momentum spectrometer!
15
Thermal energy of ions or neutrals
vave (8kT/pm)1/2 145 (TK/mamu)1/2
m/s 250 m/s for mass 100 at
298K 630 m/s for mass 16
79 m/s for mass 1000
(55 mph 25 m/s) Boltzman
distribution
16
(No Transcript)
17
(No Transcript)
18

Solution Accelerate ions through several
kilovolts! v ( 2qzVaccel/m)1/2 100
amu 124 km/sec at 8 kV (
500 thermal v) m/z qB2r2/(2Vaccel)
thermal ?v now a tiny fraction of total v.
Flight time (1 m) ca. 1 to 10 µsec B 1
Tesla means r 0.5 m For m 100 amu, If
V 1000 volts 8000 volts vaccel
44,000 m/s 124,500 m/s vthermal 0.6
0.2
19
(No Transcript)
20
(No Transcript)
21


r (2Vm/zqB2)1/2 If B 1
Tesla and V 8 kV Then r 12.877 cm for m
100 amu 12.813 cm for m
99 amu or 6.4 mm away.
Can focus mass with either B or V.
22
Detection Spatial spread  
Photoplate (original) today photoarray
detector (Fellgett
advantage) Time spread B or V sweep
in time, sequential detect at one point
Faraday cup, to electrometer. measure
current to neutralize impacting ion.
Good down to a picoamp. Picoamp 107
ions/sec
23
E
E
Electron multiplier 105 - 106 amplification
24
Double focusing high resolution! Single
magnetic sector m/?m ca. 2000 Due to (1)
energy, spatial spread of ions emerging
from source Answer electrostatic and magnetic
fields. High resolution (20,000 to 250,000
m/?m). "Exact mass" (to 1 ppm) ? molecular
formula.  
25
Velocity/energy focusing (?v) Electrostatic
sector
26
Spatial focusing
27
Other analyzers - Quadrupole mass filter
AC and DC fields (100's of volts at 1 MHz) are
high mass/low mass filters.
Cheap, lt2000 Da, lt1000 resolution. - Ion
Trap (J. Am. Soc Mass Spectrom. 2002 13(6).) -
Time of Flight (TOF) Rapid Commun. Mass
Spectrom. 1997 951 - Fourier Transform Ion
Cyclotron Resonance (FT-ICR)
Marshall, A.G. Accounts Chem. Res. 1985 18, 316.
Mass Spectrom. Rev.
1998 17, 1-35. Whole Issue Acc. Chem. Res. 1997
27(11) - Orbitrap J. Mass Spectrom. 2005 40,
430-43.
28
Quadrupole analyser ca.. 90 of MSs in the world
Quattro HP GC/MS
29
AC high pass filter. DC Low pass filter. AC
ca. 1 MHz and 100-200v
30
Quads - Small - High Transmission - Insensitive
to spread in initial ion kinetic
energy Increased rod diameter increase in
transmission
increase in resolution
decrease in mass range Increase
in rod length increase in resolution
31
Previous methods (magnetic sector, quadrupole)
are continuous ion beams. Now time-resolved
analysers
32
Quadrupole Ion trap Time resolved (msec) He at
milliTorr to help trap ions Ion
accumulation Ion/neutral chemistry Selective ion
ejection Used in Varian GC/MS in BU 665
Used in Varian
33
Time-of-flight (TOF) Time resolved
(pulsed) Resolution lt1000
34
Reflectron TOF Used in DART, Voyager MALDI

35
Ion Cyclotron Resonance (ICR) Mass
Spectrometry Fourier Transform Mass Spectrometry
(FTMS) FT-ICR MS Pulsed/time resolved Inherently
highest mass resolution known Trapped ions (msec
to sec to minutes) bimolecular ion-molecule
chemistry Parallels to nmr!
36
FT-ICR Cell, trapping and detection
Ion made in magnetic field Ions not accelerated
37
Frequencies in an ICR cell   Cyclotron  
fcyc qB/2?m   1535.7 BT
/mamu   Axial (due to trapping plates)   fax
( 2qVtrap/md2)1/2   d distance between
trapping plates (1 term)   Net f
(qB/2?m)2 - qVtrap/?md21/2
38
FT-ICR Signal FID
39
FT-ICR resolution as a function of transient
length
Record resolution 32,000,000,000 at Mass 3
40
e- mass 0.5 mmu
41
  • FT-ICR Performance
  • Resolution (mass x resolution const record
    30x109)
  • Mass Accuracy
  • Mass range
  • Dynamic Range more limited than others
  • Sensitivity 1 ion (remeasurement!)
  • positive/negative switching near-instant
  • Magnetic field higher the better
  • - Background Pressure lower the better
  • Acquisition time msec
  • Signal averaging remeasurement of same ions

42
Orbitrap MS Makarov, A. J. Mass Spectrom. 40
(2005) 430
43
(No Transcript)
44
Other Sources and Hyphenated combinations!
45
GC/MS open-split interface
46
LC/MS Micro LC into 1 torr vacuum Differential
pumping EI etc. after desolvation
47
  • Chemical Ionization soft ionization
  • 1 torr CH4 in source (high pressure)
  • plus analyte at 10-3 torr or so
  • CH4 e- ? CH4.
  • CH4 . CH4 ? CH5 CH3. self-ionization
  • CH5 B ? BH CH4
  • less exothermic ionization (0-4 eV) means little
    fragmentation,
  • often just quasi-molecular ion BH
  • Other reagent gases, specific for functional
    groups
  • Negative ions (electron attachment or
    deprotonation)

48
Negative Ions Electron attachment e- ArX
? ArX-. selective for Ar-EWG Dissociative
Attachment XY e- ? X. Y- NF3 ?
F- N2O ? O-. ( RH ? HO-) NH3 ?
NH2- Ac2O ? AcO-
49
Tandem MS, or MS/MS the structure of ions
triple quadrupole MS
Also multiple magnetic sector instruments,
FT-ICR, Ion Trap
50
iBuC(O)Et MW 114
51
Sputtering Methods
Energetic Beam onto surface SIMS Secondary Ion
Mass Spec Ion beams easy to create, but
charges the sample, with degradation of
signal
FAB Fast Atom Bombardment 8 kV neutral Xe or
Ar beam, onto glycerol (liquid in vacuum!)
drop with dissolved analyte
MALDI matrix assisted Laser Desoprtion and
Ionization photon beam (neutral and easy!)
52
MALDI Matrix Assisted Laser Desorption/Ionization
Typical matrix substituted cinnamic acid,
ArCHCHCOOH Absorbs at laser wavelength
53
(No Transcript)
54
External Sources Atmospheric Pressure
Ionization Differential pumping Ion guides
55
Electrospray Ionization (ESI) from LC, but
ionization is in liquid phase
56
One molecule, variously charged peptides 2
of 20 AA side chains are basic and
positively charged ca. 10 charges/10,000 amu
57
MW 5727 nominal 5730.6 (3.6) exact 5733.6
(6.6) ave C254H377N65O75S6
58
Tetramer Mass 147,550 daltons
59
Calibration Perfluorokerosene (CF2 50 C2F4
100) PFTBA N(C4F9)3 671 PEG H(OCH2CH2)nOH
steps of 44 Ultramark (1621) perfluoroalkylphosph
azene
60
DART Direct Analysis in Real Time
61
DART Chemistry
He discharge ? He. (filtered out) e-
He
metastable ca. 19 eV Cations He H2O ?
H2O. e- H2O. H2O ? H3O HO. H3O
B ? BH H2O Anions e- O2 ?
O2-. O2-. B ? (B-H)- HOO.
62
APCI Atmospheric Pressure Chemical Ionization
LC source, gas phase ionization
APPI Atmospheric Pressure Photoionization
63
DESI Desorption Electrospray Ionization Atmosphe
ric pressure Electrospray beam onto open
surface from wand Desorbed material sucked
into vacuum orifice
Handheld Startrek Tricorder! (for chemicals,
not biologicals)
Write a Comment
User Comments (0)
About PowerShow.com