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6.1. Electron ImpactIonization(EI)
▪EI is still used in conjunction with sample introduction either via a direct heated probe or via gas
chromatography (GC):
(i)Thesampleisintroducedintotheinstrumentsourcebyheatingitontheendofaprobeuntilit
evaporates,assistedbythehighvacuumwithintheinstrumentorviaacapillaryGCcolumn.
(ii)Onceinthevapourphase,theanalyteisbombardedwiththeelectronsproducedbyarheniumor
tungstenfilament,whichareacceleratedtowardsapositivetargetwithanenergyof70eV.Theanalyteis
introducedbetweenthefilamentandthetarget,andtheelectronscause
ionisationasfollows:Mþe!Mþ:þ2e.
(iii)Sincetheelectronsusedareofmuchhigherenergythanthe
strengthofthebondswithintheanalyte(4–7eV),extensive
fragmentationoftheanalyteusuallyoccurs.
(iv)Themoleculeanditsfragmentsarepushedoutofthesource
byarepellerplatewhichhasthesamechargeastheions
generated.
Anubhav Gupta
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6.2. Fast Atom Bombardment(FAB)
▪FABisatechniquethatwaspopularinthe80'stoearly90'sbecauseitwasthefirsttechniquethat
allowedionizationofnon-volatilecompoundsthatcouldbedonesimply.
▪Itwasdonebybombardingasampleinavacuumwithabeamofatoms,typicallyArorXe,
acceleratedtoKilovoltenergies.Thesamplewastypicallymixedinamatrix.
▪Thetwomostcommonmatrixeswereglyceroland3Nitro-benzoicacid.Thematrixallowedthe
sampletorefreshitself.
▪TheionsformedbyFABwereadductstothemolecule,wherethe
adductscouldbeprotons,sodiumions,potassiumionsor
ammoniumions.
▪AvariationofFABwasreplacementoftheatombeamwitha
beamofions,typicallycesiumions,whichwascalledsecondary
ionmassspectrometry(SIMS).SIMSspectraweretypically
identicaltoFABspectraandthetermsbecameinterchangeable.
Anubhav Gupta
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7. INSTRUMENTATION
Massspectrometerhasfollowingcomponents:
A. Sample Inlet, through HPLC, GC, Syringe etc.
B.Ionization,canbeachievedby:
1.ElectronImpactionization(EI)
2.FastAtomBombardment(FAB)
3.Electrosprayionization(ESI)
4.AtmosphericPressureChemicalIonization(APCI)
5.MatrixAssistedLaserDesorptionIonization(MALDI)
C. Acceleration&Deflection
D. Analyser,canbe achieved by analysers like :
1.Magnetic sector mass analyser
2.Double focussing analyser
3.Quadrupole mass analyser
4.Time of Flight analyser (TOF)
5.Ion trap analyser
6.Ion cyclotron analyser
E. Detector
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7.1. Sample Inlet
▪Sample stored in large reservoir from which molecules reaches ionization chamber at low
pressure in steady stream by a pinhole called “Molecular leak”.
▪Molecular leak–It is pin-hole restriction (0.01 to 0.05mm diameter) and made up of gold foil. It
is used for metering the sample to ionization chamber.
7.2. Ionization
▪Atoms are ionized by knocking one or more electrons off to give positive ions by bombardment
with a stream of electrons. Most of the positive ions formed will carry charge of +1.
7.3.Acceleration & Deflection
▪Ions are accelerated so that they all have same kinetic energy.
▪Positive ions pass through 3 slits with voltage in decreasing order.
▪Middle slit carries intermediate and finals at zero volts.
▪Ions are deflected by a magnetic field due to difference in their masses.
▪The lighter the mass, more they are deflected.
▪It also depends upon the no. of +ve charge an ion is carrying; the more +ve charge, more it will be
deflected.
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7.4. Analyser
▪A mass analyser is a device that can separate atoms and molecules according to their mass.
▪The five main characteristics for measuring the performance of a mass analyser are
1) The mass range limit or dynamic range
2) The analysis speed [u (m)S-1]
3) The transmission = No. of ion reaching the ions/No. of ions entering mass analyzer
4) The mass accuracy
5) The resolution.
▪Massanalysersusedare:
1.Magnetic sector mass analyser
2.Double focussing analyser
3.Quadrupole mass analyser
4.Time of Flight analyser (TOF)
5.Ion trap analyser
6.Ion cyclotron analyser
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7.4.3. Magnetic Sector Mass Analyzer
▪In a magnetic sector instrument the ions generated are pushed out of the source by a repeller
potential of same charge as the ion itself (most often positive).
▪They are then accelerated in an electric field of ca 3–8 kV and travel through an electrostatic field
region so that they are forced to fall into a narrow range of kinetic energies prior to entering the
field of a circular magnet.
▪They then adopt a flight path through the magnetic field depending on their charge to mass (m/z)
ratio; the large ions are deflected less by the magnetic field:
??????
??????
=
????????????????????????
????????????
where H is the magnetic field strength, r is the
radius of the circular path in which the ion travels,
and V is the accelerating voltage.
Anubhav Gupta