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Mass Spectrometry
Presented by,
Ms.Smita P.Shelke,
Assistant Professor
Gokhale Education Society’s
Sir Dr M.S. Gosavi College Of Pharmaceutical Education & Research
Prin.T.A.Kulkarni Vidyanagar, Nashik-422005
India (Maharashtra). Ph No. 0253 2232799.
Mass Spectrometry
Used by Three Ways:-
For structural elucidation of ionic
fragments
 Measurement of relative molecular
mass: molecular formula
 Comparison and identification of
known compounds
Theory of MS
 MS separates individual atoms because of differences
in their masses
consider M is a molecule focused with beam of e-
M + e- M+ + 2e-
ions accelerated with voltage V,
now energy of each particle = kinetic energy
½ mv2 =eV………………………..(1)
• v= Velocity of particle
• m= Mass of particle
• e= Charge on electron
• V= Voltage
Now charge particles enter a magnetic field H, field
attracts the particle and they move in a circle around
it with a force Hev
• However particles have centrifugal force mv2 /r
• When these two forces are equal :molecule start
moving: i.e.
mv2 /r = Hev………………..(2)
• v= Velocity of particle
• m= Mass of particle
• r= Radius of circle
• H= magnetic field
• e= Charge on electron
m/e = H2 r2 / 2V…………..(3)
• m/e= mass to charge ratio is depends on H, V and r
As e, V and H are constant
• m= mass is depends on r
Flow of Ions in Mass Spectroscope
INSTRUMENTATION
OF
MASS SPECTROSCOPY
Classical Mass Spectroscope
Instrument of MS
Schmatics of MS instrument
Basic Components of MS Instrument
 Sample Inlet System
Ion Source / Ionization Chamber
Electrostatic Accelerating System
Ion Seperator / Analyser
Magnetic Field
Ion Collector
Vacuum System
Sample Inlet Systems in MS
 Sample must be in vapour phase
 Less volatile heated before injection in
ampoule.
 Smples with less vapour pressure are with
Probe
IONIZATION METHODS
1. Gas Phase
 Electron Impact
 Chemical Ionization
 Field Ionization
2. Desorption Phase
 Field desorption
 Electro spray Ionization
 MALDI
 FAB
 Thermo spray Ionization
Electron Impact (EI)
A high energy electron beam dislodges an
electron from a
sample molecule to produce a positive ion
M + e → M+. + 2e
M= analyte molecule, M+.= Radical ion
Schematics of EI
Benefits
o well-understood
o can be applied to virtually all volatile
compounds
o reproducible mass spectra
o fragmentation provides structural
information
o libraries of mass spectra can be searched
for EI mass spectral "fingerprint"
Chemical Ionization (CI)
Gaseous atoms of the sample are
bambarded with reagent gas.
Reagent gas- methane gas
All of the primary ions of methane
react rapidly with methane (at virtually
every collision) to give product ions
Mechanism of Methane gas
 Collison of methane to produce ions
CH4
+ + CH4 --> CH5
+ + CH3
CH3
+ + CH4 --> C2H5
+ + H2
 Interaction of ions with molecule M
MH + C2H5
+ --> MH2
+ + C2H4
MH + C2H5
+ --> M+ + C2H6
Field Ionization (FI) Soft Ionization
Emitters of Tungsten wire used on which
microscopic dendrites / emmitters are
formed (by Pyrolysis)
The mechanism of ionisation - when a
molecule is subjected to a very high
electric field, ( > 10*9 volts/metre), a
valence electron tunnels through the
potential barrier and is removed from the
molecule. The resulting ion is therefore a
radical, M+.
carbon emitters and silicon emitters.
Silicon emitters are robust, relatively
inexpensive, and they can handle a higher
current for field desorption.
 Carbon emitters are more expensive, but
they can provide about an order of
magnitude better sensitivity than silicon
emitters.
Carbon Dendrimers
Desorption Field Ionization
Field desorption ionization are soft
ionization methods that tend to
produce mass spectra with little or no
fragment-ion content.
 Benefits
simple mass spectra, typically one
molecular or molecular-like ionic
species per compound.
little or no chemical background
works well for small organic molecules,
many organometallics, low molecules -
polymers and some petrochemical
fractions
Limitations
sensitive to alkali metal contamination and
sample overloading
emitter is relatively fragile
 relatively slow analysis as the emit
the sample must be thermally volatile
Electrospray Ionization
The sample solution is sprayed across a
high potential difference (a few kilovolts)
from a needle into an orifice in the
interface. Heat and gas flows are used to
desolvate the ions existing in the sample
solution.
Electrospray Ionization
Advantages of ESI
• good for charged, polar or basic
compounds
• permits the detection of high-mass
compounds at mass-to-charge ratios that
are easily
• best method for analyzing multiply
charged compound
• very low chemical background leads to
excellent detection limits
• compatible with MS/MS methods
Matrix Assisted Laser Desorption
Ionization (MALDI)
The analyte is dissolved in a solution
containing an excess of a matrix such as
sinapinic acid or dihydroxybenzoic acid
that has a chromophore that absorbs at
the laser wavelength.
Matrix Assisted Laser Desorption
Ionization (MALDI)
The matrix absorbs the energy from the
laser pulse and produces a plasma that
results in vaporization and ionization of the
analyte.
Matrix Assisted Laser Desorption
Ionization (MALDI)
Advantages of MALDI
 rapid and convenient molecular weight
determination
Limitations of MALDI
MS/MS difficult
requires a mass analyzer that is
compatible with pulsed ionization
techniques
not easily compatible with LC/MS
Fast Atom Bombardment (FAB)
The analyte is dissolved in a liquid matrix
such as glycerol, thioglycerol, m-
nitrobenzyl alcohol, or diethanolamine and
a small amount (about 1 microliter) is
placed on a target.
Fast Atom Bombardment (FAB)
The target is bombarded with a fast atom
beam (for example, 6 keV xenon atoms)
that desorb molecular-like ions and
fragments from the analyte.
 Cluster ions from the liquid matrix are also
desorbed and produce a chemical
background that varies with the matrix
used.
Fast Atom Bombardment (FAB)
Mass analyzers
OR
Separators
Mass analyzers / Seperators
1.Sector analysers
Single focusing
Double focusing
2. Quadrupole analyser
Mass filter
Ion trap/ Ion storage
3. Time of Flight (TOF)
4. FT-Ion Cyclotron Resonance (FT-ICR)
Mass analyzers / Seperators
1. Sector analysers:
 uses an electric and/or magnetic field to affect
the path and/or velocity of the charged particles .
 bend the trajectories of the ions as they pass
through the mass analyzer, according to their
mass-to-charge ratios.
 deflecting the more charged and faster-moving,
lighter ions more.
1.1 Single Focusing Sector Analyser
1.2 Double Focusing
Mass spectrometer that incorporates a
magnetic sector and an electric sector
connected in series in such a way that
ions with the same m/z but with
distributions in both the direction.
1.2 Double Focusing
2.1 Quadrupole analyser : Mass filter
A quadrupole mass filter consists of four
parallel metal rods
Two opposite rods have an applied
potential
The applied voltages affect the trajectory
of ions traveling between the four rods.
only ions of a certain mass-to-charge ratio
pass through the quadrupole filter.
Quadrupole analyser : Mass filter
Quadrupole analyser : Ion Trap
an ion trap uses constant DC and radio
frequency (RF) oscillating AC electric
fields to trap ions.
It is commonly used as a component of
a mass spectrometer.
Quadrupole analyser : Ion Trap
3. Time Of Flight (TOF)
 an ion's mass-to-charge ratio is
determined via a time measurement.
Ions are accelerated by an electric field of
known strength.
This acceleration results in an ion having
the same kinetic energy.
The velocity of the ion depends on the
mass-to-charge ratio.
The time that it takes for the particle to
reach a detector at a known distance is
measured.
3. Time Of Flight (TOF)
3. FT-Ion Cyclotron resonance (FT-ICR)
 the mass-to-charge ratio (m/z) of ions
based on the cyclotron frequency of the
ions in a fixed magnetic field.
 The ions are trapped in a Penning trap (a
magnetic field with electric trapping plates)
where they are excited by rf
After the excitation field is removed, the
ions are rotating at their cyclotron
frequency in phase (as a "packet" of ions).
FT-Ion Cyclotron resonance (FT-ICR)
These ions induce a charge on a pair of
electrodes as the packets of ions pass
close to them.
The resulting signal is called a free
induction decay (FID), transient or
interferogram that consists of a
superposition of sine waves.
The useful signal is extracted from this
data by performing a Fourier transform
ION CYCLOTRON
FT-Ion Cyclotron resonance (FT-ICR)
Tandem Mass Spectroscopy MS-MS
Multiple stages of mass analysis separation
can be accomplished with individual mass
spectrometer.
Elements separated in space or using a
single mass spectrometer with the MS
steps separator.
Tandem Mass Spectroscopy MS-MS
Methods of Ion Detection / Ion
detectiors
Mass analysis - i.e. the separation of
bunches or streams of ions according to
their individual mass-to-charge (m/z) ratio.
The most common types of ion detector
used in modern instruments:
1. The Faraday Cup or Cylinder
2. The Electron Multiplier
3. The Photomultiplier or
Scintillation Counter.
1. The Faraday Cup or Cylinder
The basic principle is that the incident ion
strikes the dynode surface, which emits
electrons and induces a current which is
amplified and recorded.
The dynode electrode is made of a
secondary emitting material like CsSb,
GaP or BeO.
The Faraday cup is very robust.
1. The Faraday Cup or Cylinder
2. The Electron Multiplier
 A Faraday cup uses one dynode, it has
series of dynodes maintained at increasing
potentials resulting in a series of
amplifications.
Their are two types of electron multiplier
2. The Electron Multiplier
3. The Photomultiplier or
Scintillation Counter.
The ions initially strike a dynode which
results in electron emission.
These electrons then strike a phosphorous
screen which in turn releases a burst of
photons.
The photons then pass into the multiplier
where amplification occurs in a cascade
3. The Photomultiplier or
Scintillation Counter.
Interpretation of MS Spectrum
The mass spectrum produced will usually
be presented as a vertical bar graph, in
which each bar represents an ion having a
specific mass-to-charge ratio (m/z) and the
length of the bar indicates the relative
abundance of the ion.
Presentation on mass spectroscopy
Sector Analyser
QUADRUPOLE
and 27.9949 Daltons, respectively2.
Time of Flight
Types of Ion in MS / Interpertation
Mass Spectrum
Gas Chromatograph with MS
Applications of Mass Spectroscopy
Presentation on mass spectroscopy
Presentation on mass spectroscopy
Presentation on mass spectroscopy
Presentation on mass spectroscopy

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Presentation on mass spectroscopy

  • 1. Mass Spectrometry Presented by, Ms.Smita P.Shelke, Assistant Professor Gokhale Education Society’s Sir Dr M.S. Gosavi College Of Pharmaceutical Education & Research Prin.T.A.Kulkarni Vidyanagar, Nashik-422005 India (Maharashtra). Ph No. 0253 2232799.
  • 2. Mass Spectrometry Used by Three Ways:- For structural elucidation of ionic fragments  Measurement of relative molecular mass: molecular formula  Comparison and identification of known compounds
  • 3. Theory of MS  MS separates individual atoms because of differences in their masses consider M is a molecule focused with beam of e- M + e- M+ + 2e- ions accelerated with voltage V, now energy of each particle = kinetic energy ½ mv2 =eV………………………..(1) • v= Velocity of particle • m= Mass of particle • e= Charge on electron • V= Voltage
  • 4. Now charge particles enter a magnetic field H, field attracts the particle and they move in a circle around it with a force Hev • However particles have centrifugal force mv2 /r • When these two forces are equal :molecule start moving: i.e. mv2 /r = Hev………………..(2) • v= Velocity of particle • m= Mass of particle • r= Radius of circle • H= magnetic field • e= Charge on electron
  • 5. m/e = H2 r2 / 2V…………..(3) • m/e= mass to charge ratio is depends on H, V and r As e, V and H are constant • m= mass is depends on r
  • 6. Flow of Ions in Mass Spectroscope
  • 10. Schmatics of MS instrument
  • 11. Basic Components of MS Instrument  Sample Inlet System Ion Source / Ionization Chamber Electrostatic Accelerating System Ion Seperator / Analyser Magnetic Field Ion Collector Vacuum System
  • 12. Sample Inlet Systems in MS  Sample must be in vapour phase  Less volatile heated before injection in ampoule.  Smples with less vapour pressure are with Probe
  • 13. IONIZATION METHODS 1. Gas Phase  Electron Impact  Chemical Ionization  Field Ionization 2. Desorption Phase  Field desorption  Electro spray Ionization  MALDI  FAB  Thermo spray Ionization
  • 14. Electron Impact (EI) A high energy electron beam dislodges an electron from a sample molecule to produce a positive ion M + e → M+. + 2e M= analyte molecule, M+.= Radical ion
  • 16. Benefits o well-understood o can be applied to virtually all volatile compounds o reproducible mass spectra o fragmentation provides structural information o libraries of mass spectra can be searched for EI mass spectral "fingerprint"
  • 17. Chemical Ionization (CI) Gaseous atoms of the sample are bambarded with reagent gas. Reagent gas- methane gas All of the primary ions of methane react rapidly with methane (at virtually every collision) to give product ions
  • 18. Mechanism of Methane gas  Collison of methane to produce ions CH4 + + CH4 --> CH5 + + CH3 CH3 + + CH4 --> C2H5 + + H2  Interaction of ions with molecule M MH + C2H5 + --> MH2 + + C2H4 MH + C2H5 + --> M+ + C2H6
  • 19. Field Ionization (FI) Soft Ionization Emitters of Tungsten wire used on which microscopic dendrites / emmitters are formed (by Pyrolysis) The mechanism of ionisation - when a molecule is subjected to a very high electric field, ( > 10*9 volts/metre), a valence electron tunnels through the potential barrier and is removed from the molecule. The resulting ion is therefore a radical, M+.
  • 20. carbon emitters and silicon emitters. Silicon emitters are robust, relatively inexpensive, and they can handle a higher current for field desorption.  Carbon emitters are more expensive, but they can provide about an order of magnitude better sensitivity than silicon emitters.
  • 22. Desorption Field Ionization Field desorption ionization are soft ionization methods that tend to produce mass spectra with little or no fragment-ion content.  Benefits simple mass spectra, typically one molecular or molecular-like ionic species per compound.
  • 23. little or no chemical background works well for small organic molecules, many organometallics, low molecules - polymers and some petrochemical fractions Limitations sensitive to alkali metal contamination and sample overloading emitter is relatively fragile  relatively slow analysis as the emit the sample must be thermally volatile
  • 24. Electrospray Ionization The sample solution is sprayed across a high potential difference (a few kilovolts) from a needle into an orifice in the interface. Heat and gas flows are used to desolvate the ions existing in the sample solution.
  • 26. Advantages of ESI • good for charged, polar or basic compounds • permits the detection of high-mass compounds at mass-to-charge ratios that are easily • best method for analyzing multiply charged compound • very low chemical background leads to excellent detection limits • compatible with MS/MS methods
  • 27. Matrix Assisted Laser Desorption Ionization (MALDI) The analyte is dissolved in a solution containing an excess of a matrix such as sinapinic acid or dihydroxybenzoic acid that has a chromophore that absorbs at the laser wavelength.
  • 28. Matrix Assisted Laser Desorption Ionization (MALDI) The matrix absorbs the energy from the laser pulse and produces a plasma that results in vaporization and ionization of the analyte.
  • 29. Matrix Assisted Laser Desorption Ionization (MALDI)
  • 30. Advantages of MALDI  rapid and convenient molecular weight determination Limitations of MALDI MS/MS difficult requires a mass analyzer that is compatible with pulsed ionization techniques not easily compatible with LC/MS
  • 31. Fast Atom Bombardment (FAB) The analyte is dissolved in a liquid matrix such as glycerol, thioglycerol, m- nitrobenzyl alcohol, or diethanolamine and a small amount (about 1 microliter) is placed on a target.
  • 32. Fast Atom Bombardment (FAB) The target is bombarded with a fast atom beam (for example, 6 keV xenon atoms) that desorb molecular-like ions and fragments from the analyte.  Cluster ions from the liquid matrix are also desorbed and produce a chemical background that varies with the matrix used.
  • 35. Mass analyzers / Seperators 1.Sector analysers Single focusing Double focusing 2. Quadrupole analyser Mass filter Ion trap/ Ion storage 3. Time of Flight (TOF) 4. FT-Ion Cyclotron Resonance (FT-ICR)
  • 36. Mass analyzers / Seperators 1. Sector analysers:  uses an electric and/or magnetic field to affect the path and/or velocity of the charged particles .  bend the trajectories of the ions as they pass through the mass analyzer, according to their mass-to-charge ratios.  deflecting the more charged and faster-moving, lighter ions more.
  • 37. 1.1 Single Focusing Sector Analyser
  • 38. 1.2 Double Focusing Mass spectrometer that incorporates a magnetic sector and an electric sector connected in series in such a way that ions with the same m/z but with distributions in both the direction.
  • 40. 2.1 Quadrupole analyser : Mass filter A quadrupole mass filter consists of four parallel metal rods Two opposite rods have an applied potential The applied voltages affect the trajectory of ions traveling between the four rods. only ions of a certain mass-to-charge ratio pass through the quadrupole filter.
  • 41. Quadrupole analyser : Mass filter
  • 42. Quadrupole analyser : Ion Trap an ion trap uses constant DC and radio frequency (RF) oscillating AC electric fields to trap ions. It is commonly used as a component of a mass spectrometer.
  • 44. 3. Time Of Flight (TOF)  an ion's mass-to-charge ratio is determined via a time measurement. Ions are accelerated by an electric field of known strength. This acceleration results in an ion having the same kinetic energy. The velocity of the ion depends on the mass-to-charge ratio. The time that it takes for the particle to reach a detector at a known distance is measured.
  • 45. 3. Time Of Flight (TOF)
  • 46. 3. FT-Ion Cyclotron resonance (FT-ICR)  the mass-to-charge ratio (m/z) of ions based on the cyclotron frequency of the ions in a fixed magnetic field.  The ions are trapped in a Penning trap (a magnetic field with electric trapping plates) where they are excited by rf After the excitation field is removed, the ions are rotating at their cyclotron frequency in phase (as a "packet" of ions).
  • 47. FT-Ion Cyclotron resonance (FT-ICR) These ions induce a charge on a pair of electrodes as the packets of ions pass close to them. The resulting signal is called a free induction decay (FID), transient or interferogram that consists of a superposition of sine waves. The useful signal is extracted from this data by performing a Fourier transform
  • 50. Tandem Mass Spectroscopy MS-MS Multiple stages of mass analysis separation can be accomplished with individual mass spectrometer. Elements separated in space or using a single mass spectrometer with the MS steps separator.
  • 52. Methods of Ion Detection / Ion detectiors Mass analysis - i.e. the separation of bunches or streams of ions according to their individual mass-to-charge (m/z) ratio. The most common types of ion detector used in modern instruments: 1. The Faraday Cup or Cylinder 2. The Electron Multiplier 3. The Photomultiplier or Scintillation Counter.
  • 53. 1. The Faraday Cup or Cylinder The basic principle is that the incident ion strikes the dynode surface, which emits electrons and induces a current which is amplified and recorded. The dynode electrode is made of a secondary emitting material like CsSb, GaP or BeO. The Faraday cup is very robust.
  • 54. 1. The Faraday Cup or Cylinder
  • 55. 2. The Electron Multiplier  A Faraday cup uses one dynode, it has series of dynodes maintained at increasing potentials resulting in a series of amplifications. Their are two types of electron multiplier
  • 56. 2. The Electron Multiplier
  • 57. 3. The Photomultiplier or Scintillation Counter. The ions initially strike a dynode which results in electron emission. These electrons then strike a phosphorous screen which in turn releases a burst of photons. The photons then pass into the multiplier where amplification occurs in a cascade
  • 58. 3. The Photomultiplier or Scintillation Counter.
  • 59. Interpretation of MS Spectrum The mass spectrum produced will usually be presented as a vertical bar graph, in which each bar represents an ion having a specific mass-to-charge ratio (m/z) and the length of the bar indicates the relative abundance of the ion.
  • 64. Types of Ion in MS / Interpertation Mass Spectrum
  • 66. Applications of Mass Spectroscopy