Chem 454
March 30, 2001
Mass Spectrometry
- Goal is to separate molecules by mass
- generally to identify a species
- fragmentation pattern provides useful hints
- parent ion, if present, tells molecular weight
- at high resolution (+0.01 amu) there's more information
- a major use is as a detector for GC and LC
- MS pattern can uniquely identify each peak
- works nicely with automated data systems
- as a rule, MS needs a pure sample
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- Also find instruments called RGA
- residual gas analyzers
- limited to gases (N2, O2, NO, CO, CO2, H2O, low hydrocarbons)
- perhaps to mass 150
- specialized mass spectrometers
- helium leak detector
- only looks for Helium
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- How to
create the ions?
- First, convert to isolated ions
- typically sample is a gas/vapor
- might need vapor pressure of 1-5 torr
- sample ionized by electron impact
- at 40-90 eV, can ionize and fragment the species
- ions are accelerated and focused by electrical fields
- most work is done with + ions (all we will consider here)
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Vacuum Conditions
- Ion must travel a path of 2-200 cm
- any collisions would alter the path in unpredictable manner
- want low pressure (10-5 - 10-7 torr) to reduce collisions
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- Detecting the ions
- simplest is just a sheet of metal
- charged negatively
- collects + ions
- measure the electrical current
- really very tiny currents
- in some simpler devices (RGA, He) that's OK
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- Most use Electron Multipliers
- act like photomultiplier
- except first stage accelerates ions to produce electron
- dynodes multiply electron current
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- Heart of a Mass Spectrometer is separation of ions
- by their mass
- (usually really by mass/charge ratio)
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Several Major Schemes
- Magnetic Sectors
charged particle moving in magnetic field
- experiences force perpendicular to motion
- will follow curve (circular) path
- radius is fixed by mass
- affected by (charge, magnetic field strength, ion velocity)
- magnetic region usually smaller than the circular path
- one style is 60o (one sixth of a circle)
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- oldest forms (Aston 1910 ?)
- detect on film or a phosphor screen
- image shows all masses at different positions
- (Analogy: spectrograph or diode array spectrometer)
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- more commonly, fixed exit slit
- reject all ions except one mass
- scan to look at all the masses
- (analogy, scanning spectrometer)
Time of Flight mass Spectrometers
- create ions in a very short pulse
- accelerate the ions down a tube (drift tube)
- determine when ions arrive
- force on all +1 ions same (e x Voltage)
- kinetic energy of ions the same
- velocity proportional to 1/ m1/2
- see H+, H2+, He+, N+, O+, N2+, O2+ ...then heavier ions
Quadrupole Mass Spectrometer
- ions sent into an analyzer region
- analyzer has four parallel metal rods
- typically like four half length wood pencils
- space down the center a little larger than a similar pencil
- apply a mixed DC and AC electrical field to the rods
- ion in the field accelerated up/down/right/left by AC field
- most ions follow paths of increasing amplitude
- ions are lost, never make it through the tube
- one narrow range of masses form stable trajectories
- ion gets through and gets detected
- we vary the frequency (RF) or voltages to select the mass
- can sweep mass range in under a second or over a few seconds
- useful in GC-MS (peak may last 10 sec, need a fast MS)
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Quadrapole Mass Trap
3D analog of Quarupole Mass Filter
ions get trapped inside
- only one mass stays (others hit walls, lost)
- can store for minutes if desired
- like CCD light detector, accumulates signals
- quick voltage change and ions all hit the wall
- measure that current
- can do this rapidly (millisec.) so good GC detector
- detector is smaller, simpler, less costly than Quad Rod Assembly
- can accumulate to detect weaker samples
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Fourier Transform Mass Spectrometer
- older name Ion Cyclotron Trap
- traps all ions in circular paths
- quickly change parameters
- ions travel to detector
- detect which ions arrive when (similar to TOF)
- complex signal reversed by Fourier Transform
- not widely used except in research applications
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Comparisons
- Magnetic Sector
- Traditional (1930's to 1970's)
- Typically an electromagnet
- Magnet might weigh 1 ton, but 10-20" across
- need current of 100 amps, cooling water
- could go 10-4000 amu, + 0.01 amu perhaps
- scan time varies with resolution
- some sweep magnetic field, others vary the accelrating voltage
- typically scan a full spectrum in 1-5 minutes
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Miniature versions exist
lower mass range, lower resolution
- smaller, lighter
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- Quadrupole (1975 and beyond)
- smaller and lighter
- needed to wait on low cost RF electronics
- cheaper once the electronics evolved
- initially low mass range, modest resolution
- gradually replaced most magnetic instruments
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Quad Ion Trap (1985 and beyond)
analyzer more compact, cheaper than quad
- poorer resolution
- gradually taking over on GC-MS and LC-MS