Mass Ionization 21 01 10

Embed Size (px)

Citation preview

  • 7/28/2019 Mass Ionization 21 01 10

    1/67

    Mass Spectrometry:

    Ionization methods

  • 7/28/2019 Mass Ionization 21 01 10

    2/67

    Mass Spec Principles

    Ionizer

    Sample

    +

    _

    Mass Analyzer Detector

  • 7/28/2019 Mass Ionization 21 01 10

    3/67

    How does a mass spectrometer work?

    Ionization

    method

    MALDI

    Electrospray

    Mass analyzer

    MALDI-TOF

    MW

    Triple Quadrapole AA seq

    MALDI-QqTOF AA seq and MW

    QqTOF AA seq and protein modif.

    Create ions Separate ions Detect ions

    Mass

    spectrum

    Database

    analysis

  • 7/28/2019 Mass Ionization 21 01 10

    4/67

    Ion sources for molecular mass

    spectrometry

  • 7/28/2019 Mass Ionization 21 01 10

    5/67

    Soft Ionization Soft ionization techniques keep the molecule

    of interest fully intact

    Electro-spray ionization first conceived in1960s by Malcolm Dole but put into practice

    in 1980s by John Fenn (Yale)

    MALDI first introduced in 1985 by Franz

    Hillenkamp and Michael Karas (Frankfurt)

    Made it possible to analyze large moleculesvia inexpensive mass analyzers such as

    quadrupole, ion trap and TOF

  • 7/28/2019 Mass Ionization 21 01 10

    6/67

    Soft Ionization Methods

    337 nm UV laser

    MALDI

    cyano-hydroxy

    cinnamic acidGold tip needle

    Fluid (no salt)

    ESI

    +

    _

  • 7/28/2019 Mass Ionization 21 01 10

    7/67

    Soft ion sources little excess energy in

    molecule

    reduced fragmentation

  • 7/28/2019 Mass Ionization 21 01 10

    8/67

    Hard ion sources leave excess energy in

    molecule-extensive fragmentation

  • 7/28/2019 Mass Ionization 21 01 10

    9/67

    Different Ionization Methods

    Electron Impact (EI - Hard method) small molecules, 1-1000 Daltons, structure

    Fast Atom Bombardment (FAB Semi-hard) peptides, sugars, up to 6000 Daltons

    Electrospray Ionization (ESI - Soft)

    peptides, proteins, up to 200,000 Daltons

    Matrix Assisted Laser Desorption (MALDI-Soft) peptides, proteins, DNA, up to 500 kD

  • 7/28/2019 Mass Ionization 21 01 10

    10/67

    Sample introduction/ionization method

    Ionization

    method

    Typical

    Analytes

    Sample

    Introduction

    Mass

    Range

    Method

    Highlights

    Electron Impact (EI)

    Relatively

    small

    volatile

    GC or

    liquid/solid

    probe

    to

    1,000

    Daltons

    Hard method

    versatile

    provides

    structure info

    Chemical Ionization (CI)

    Relatively

    smallvolatile

    GC or

    liquid/solidprobe

    to

    1,000Daltons

    Soft method

    molecular ionpeak [M+H]+

    Electrospray (ESI)

    Peptides

    Proteins

    nonvolatile

    Liquid

    Chromatography

    or syringe

    to

    200,000

    Daltons

    Soft method

    ions often

    multiply

    charged

    Fast Atom Bombardment

    (FAB)

    Carbohydrates

    Organometallics

    Peptides

    nonvolatile

    Sample mixed

    in viscous

    matrix

    to

    6,000

    Daltons

    Soft method

    but harder

    than ESI or

    MALDI

    Matrix Assisted Laser

    Desorption

    (MALDI)

    Peptides

    Proteins

    Nucleotides

    Sample mixed

    in solid

    matrix

    to

    500,000

    Daltons

    Soft method

    very high

    mass

  • 7/28/2019 Mass Ionization 21 01 10

    11/67

    Electron Ionization

    Also called as electron impact ionization

    Oldest and best-characterized of all the ionization

    methods.

    A beam of electrons passes through the gas-phase

    sample. An electron that collides with a neutral analyte

    molecule can knock off another electron, resulting in a

    positively charged ion.

  • 7/28/2019 Mass Ionization 21 01 10

    12/67

    Electron Ionization

    The ionization process can either produce a molecular

    ion which will have the same molecular weight andelemental composition of the starting analyte, or it can

    produce a fragmention which corresponds to a smaller

    piece of the analyte molecule.

    Most mass spectrometers use electrons with anenergy of 70 electron volts (eV) for EI.

    Decreasing the electron energy can reduce

    fragmentation, but it also reduces the number of ionsformed.

  • 7/28/2019 Mass Ionization 21 01 10

    13/67

  • 7/28/2019 Mass Ionization 21 01 10

    14/67

    EI Fragmentation of CH3OH

    CH3OH CH3OH+

    CH3OH CH2O=H+ + H

    CH3OH+ CH3 + OH

    CHO=H+ + HCH2O=H+

    Why wouldnt Electron Impact be suitable

    for analyzing proteins?

  • 7/28/2019 Mass Ionization 21 01 10

    15/67

    Why You Cant Use EI For

    Analyzing Proteins

    EI shatters chemical bonds

    Any given protein contains 20 different

    amino acids

    EI would shatter the protein into not onlyinto amino acids but also amino acid sub-

    fragments and even peptides of 2,3,4amino acids

    Result is 10,000s of different signals from

    a single protein -- too complex to analyze

  • 7/28/2019 Mass Ionization 21 01 10

    16/67

    Electron Ionization

    Sample introduction

    heated batch inlet

    heated direct insertion probe

    gas chromatography

    liquid chromatography (particle-beaminterface)

  • 7/28/2019 Mass Ionization 21 01 10

    17/67

    Some typical reactions in EI

    source

  • 7/28/2019 Mass Ionization 21 01 10

    18/67

    Fragmentation patterns

  • 7/28/2019 Mass Ionization 21 01 10

    19/67

    Fragmentation patterns

  • 7/28/2019 Mass Ionization 21 01 10

    20/67

    Electron Ionization

    Benefits well-understood

    can be applied to virtually all volatile

    compounds reproducible mass spectra

    fragmentation provides structural information

    libraries of mass spectra can be searched forEI mass spectral "fingerprint"

  • 7/28/2019 Mass Ionization 21 01 10

    21/67

    Electron Ionization

    Limitations

    sample must be thermally volatile and

    stable

    the molecular ion may be weak orabsent for many compounds.

    Mass range

    Low Typically less than 1,000 Da.

  • 7/28/2019 Mass Ionization 21 01 10

    22/67

    Electron Ionization

    Advantages of EI: high ion currents - sensitive

    fragmentation aids identification

    Disadvantages of EI:

    weak or absent M+ peak inhibitsdetermination of MW

    molecules must be vaporized (MW < 103 Da)

    molecules must be thermally stable duringvaporization

  • 7/28/2019 Mass Ionization 21 01 10

    23/67

    Chemical Ionization (CI) Chemical ionization uses ion-molecule reactions to

    produce ions from the analyte. The chemical ionization process begins when a

    reagent gas such as methane, isobutane, or

    ammonia is ionized by electron impact.

    A high reagent gas pressure (or long reaction time)

    results in ion-molecule reactions between the

    reagent gas ions and reagent gas neutrals.

    Some of the products of these ion-moleculereactions can react with the analyte molecules to

    produce analyte ions.

  • 7/28/2019 Mass Ionization 21 01 10

    24/67

    Chemical Ionization (CI)Example (R = reagent, S = sample, e = electron, . =

    radical electron , H = hydrogen):R + e ---> R+. + 2e

    R+. + RH ---> RH+ + R.

    RH+ + S ---> SH+ + R(of course, other reactions can occur)

  • 7/28/2019 Mass Ionization 21 01 10

    25/67

    Chemical Ionization (CI)Sample introduction

    heated batch inlet heated direct insertion probe

    gas chromatograph

    liquid chromatograph (particle-beam interface)Benefits

    often gives molecular weight information through

    molecular-like ions such as [M+H]+, even when EIwould not produce a molecular ion.

    simple mass spectra, fragmentation reducedcompared to EI

  • 7/28/2019 Mass Ionization 21 01 10

    26/67

    Chemical Ionization (CI)Limitations

    sample must be thermally volatile and stable less fragmentation than EI, fragment pattern not

    informative or reproducible enough for library

    search results depend on reagent gas type, reagent gas

    pressure or reaction time, and nature of sample.

    Mass range

    Low Typically less than 1,000 Da.

  • 7/28/2019 Mass Ionization 21 01 10

    27/67

    Field Desorption (FD)

    The sample is deposited onto the emitter and the emitter is

    biased to a high potential (several kilovolts) and a current is

    passed through the emitter to heat up the filament.

    Mass spectra are acquired as the emitter current is

    gradually increased and the sample is evaporated from the

    emitter into the gas phase.

    The analyte molecules are ionized by electron tunneling atthe tip of the emitter 'whiskers'.

    Characteristic positive ions produced are radical molecular

    ions and cation attached species such as [M+Na]+ and [M-

    Na]+. The latter are probably produced during desorption by the

    attachment of trace alkali metal ions present in the analyte.

  • 7/28/2019 Mass Ionization 21 01 10

    28/67

    Field Desorption (FD)

    Sample introduction

    Direct insertion probe. The sample is deposited onto the tip of the emitter

    by

    . dipping the emitter into an analyte solution

    . depositing the dissolved or suspended sample

    onto the emitter with a microsyringe

  • 7/28/2019 Mass Ionization 21 01 10

    29/67

    Field Desorption (FD)

    Benefits

    simple mass spectra, typically one molecular ormolecular-like ionic species per compound.

    little or no chemical background

    works well for small organic molecules, manyorganometallics, low molecular weight polymersand some petrochemical fractions

  • 7/28/2019 Mass Ionization 21 01 10

    30/67

    Field Desorption (FD)

    Limitations

    sensitive to alkali metal contamination and sampleoverloading

    emitter is relatively fragile

    relatively slow analysis as the emitter current is

    increased the sample must be thermally volatile to some

    extent to be desorbed

    Mass range Low-moderate, depends on the sample. Typically

    less than about 2,000 to 3,000 Da.

    some examples have been recorded from ions withmasses beyond 10,000 Da.

    Fi ld I i ti (FI)

  • 7/28/2019 Mass Ionization 21 01 10

    31/67

    Field Ionization (FI)

    The sample is evaporated from a direct insertion probe,gas chromatograph, or gas inlet.

    As the gas molecules pass near the emitter, they areionized by electron tunneling.

    Sample introduction heated direct insertion probe

    gas inlet

    gas chromatograph

    i i i

  • 7/28/2019 Mass Ionization 21 01 10

    32/67

    Field Ionization (FI)

    Benefits

    simple mass spectra, typically one molecular ormolecular-like ionic species per compound.

    little or no chemical background

    works well for small organic molecules and somepetrochemical fractions

    Fi ld I i i (FI)

  • 7/28/2019 Mass Ionization 21 01 10

    33/67

    Field Ionization (FI)

    Limitations

    The sample must be thermally volatile.

    Samples are introduced in the same way as forelectron ionization (EI).

    Mass range

    Low Typically less than 1000 Da.

    F t At B b d t (FAB)

  • 7/28/2019 Mass Ionization 21 01 10

    34/67

    Fast Atom Bombardment (FAB)

    The analyte is dissolved in a liquid matrix such as

    glycerol, thioglycerol,m-nitrobenzyl alcohol,

    ordiethanolamine and a small amount (about 1microliter) is placed on a target.

    The target is bombarded with a fast atom beam

    (for example, 6 keV xenon atoms) that desorbmolecular-like ions and fragments from theanalyte.

    Cluster ions from the liquid matrix are alsodesorbed and produce a chemical background thatvaries with the matrix used.

    F t At B b d t (FAB)

  • 7/28/2019 Mass Ionization 21 01 10

    35/67

    Fast Atom Bombardment (FAB)

    Sample introduction

    direct insertion probe LC/MS (frit FAB or continuous-flow FAB).

    Benefits rapid

    simple

    relatively tolerant of variations in sampling

    good for a large variety of compounds

    strong ion currents -- good for high-resolutionmeasurements

    F t At B b d t (FAB)

  • 7/28/2019 Mass Ionization 21 01 10

    36/67

    Fast Atom Bombardment (FAB)

    Limitations

    high chemical background defines detection limits

    may be difficult to distinguish low-molecular-weightcompounds from chemical background

    analyte must be soluble in the liquid matrix

    no good for multiply charged compounds with morethan 2 charges

    Mass range

    Moderate Typically ~300 Da to about 6000 Da.

    Secondar Ion Mass Spectrometr (SIMS)

  • 7/28/2019 Mass Ionization 21 01 10

    37/67

    Secondary Ion Mass Spectrometry (SIMS)

    Dynamic SIMS is nearly identical to FAB except

    that the primary particle beam is an ion beam(usually cesium ions) rather than a neutral beam.

    The ions can be focused and accelerated to higher

    kinetic energies than are possible for neutralbeams, and sensitivity is improved for highermasses.

    The use of SIMS for moderate-size (3000-13,000Da) proteins and peptides has largely beensupplanted by electrospray ionization.

    S d I M S t t (SIMS)

  • 7/28/2019 Mass Ionization 21 01 10

    38/67

    Secondary Ion Mass Spectrometry (SIMS)

    Sample introduction

    Same as for FAB

    Benefits

    Same as for FAB, except sensitivity is improved forhigher masses (3000 to 13,000 Da).

    S d I M S t t (SIMS)

  • 7/28/2019 Mass Ionization 21 01 10

    39/67

    Secondary Ion Mass Spectrometry (SIMS)

    Limitations

    Same as for FAB except

    target can get hotter than in FAB due to moreenergetic primary beam

    high-voltage arcs more common than FAB

    ion source usually requires more maintenance thanFAB

    Mass range Moderate Typically 300 to 13,000 Da.

    Electrospray Ionization (ESI)

  • 7/28/2019 Mass Ionization 21 01 10

    40/67

    Electrospray Ionization (ESI)

    Sample dissolved in polar, volatile buffer (no salts)

    and pumped through a stainless steel capillary (70

    - 150 mm) at a rate of 10-100 mL/min

    Strong voltage (3-4 kV) applied at tip along with

    flow of nebulizing gas causes the sample tonebulize or aerosolize

    Aerosol is directed through regions of highervacuum until droplets evaporate to near atomic

    size (still carrying charges)

  • 7/28/2019 Mass Ionization 21 01 10

    41/67

    Electrospray Ionization (ESI)

    El t I i ti (ESI)

  • 7/28/2019 Mass Ionization 21 01 10

    42/67

    Electrospray Ionization (ESI)

    Can be modified to nanospray system

    with flow < 1mL/min

    Very sensitive technique, requires lessthan a picomole of material

    Strongly affected by salts & detergents

    Positive ion mode measures (M + H)+ (addformic acid to solvent)

    Negative ion mode measures (M - H)- (add

    ammonia to solvent)

  • 7/28/2019 Mass Ionization 21 01 10

    43/67

    Positive or Negative Ion Mode?

    If the sample has functional groups thatreadily accept H+ (such as amide andamino groups found in peptides andproteins) then positive ion detection isused-PROTEINS

    If a sample has functional groups that

    readily lose a proton (such as carboxylicacids and hydroxyls as found in nucleicacids and sugars) then negative iondetection is used-DNA

    Electrospray Ionization (ESI)

  • 7/28/2019 Mass Ionization 21 01 10

    44/67

    Electrospray Ionization (ESI)

    Sample introduction

    flow injection LC/MS

    typical flow rates are less than 1 microliter perminute up to about a milliliter per minute

    Electrospray Ionization (ESI)

  • 7/28/2019 Mass Ionization 21 01 10

    45/67

    Electrospray Ionization (ESI)

    Benefits

    good for charged, polar or basic compounds permits the detection of high-mass compounds at

    mass-to-charge ratios that are easily determined

    by most mass spectrometers (m/z typically less

    than 2000 to 3000). best method for analyzing multiply charged

    compounds

    very low chemical background leads to excellentdetection limits

    can control presence or absence of fragmentation

    by controlling the interface lens potentials

    compatible with MS/MS methods

    Electrospray Ionization (ESI)

  • 7/28/2019 Mass Ionization 21 01 10

    46/67

    Electrospray Ionization (ESI)

    Limitations

    multiply charged species require interpretation andmathematical transformation (can sometimes bedifficult)

    complementary to APCI. No good for uncharged,

    non-basic, low-polarity compounds (e.g.steroids) very sensitive to contaminants such as alkali

    metals or basic compounds

    relatively low ion currents relatively complex hardware compared to other ion

    sources

    Mass range

    Low-hi h T icall less than 200 000 Da.

    Atmospheric Pressure Chemical Ionization

  • 7/28/2019 Mass Ionization 21 01 10

    47/67

    Atmospheric Pressure Chemical Ionization

    (APCI)

    Similar interface to that used for ESI.

    In APCI, a corona discharge is used to ionize theanalyte in the atmospheric pressure region.

    The gas-phase ionization in APCI is more effective

    than ESI for analyzing less-polar species.

    ESI and APCI are complementary methods.

    Atmospheric Pressure Chemical Ionization

  • 7/28/2019 Mass Ionization 21 01 10

    48/67

    Atmospheric Pressure Chemical Ionization

    (APCI)

    Sample introduction

    same as for electrospray ionization

    Benefits

    good for less-polar compounds

    excellent LC/MS interface

    compatible with MS/MS methods

    Atmospheric Pressure Chemical Ionization

  • 7/28/2019 Mass Ionization 21 01 10

    49/67

    Atmospheric Pressure Chemical Ionization

    (APCI)

    Limitations

    complementary to ESI

    Mass range

    Low-moderate Typically less than 2000 Da.

    Matrix-Assisted Laser Desorption

  • 7/28/2019 Mass Ionization 21 01 10

    50/67

    Matrix-Assisted Laser Desorption

    Ionization (MALDI)

    The analyte is dissolved in a solution containing anexcess of a matrix such as sinapinic acid ordihydroxybenzoic acid that has a chromophorethat absorbs at the laser wavelength.

    A small amount of this solution is placed on thelaser target.

    The matrix absorbs the energy from the laserpulse and produces a plasma that results invaporization and ionization of the analyte.

  • 7/28/2019 Mass Ionization 21 01 10

    51/67

    MALDI Ionization

    ++

    +

    +

    -

    --

    ++

    +

    +

    -

    ---++

    Analyte

    Matrix

    Laser

    +

    ++

    Absorption of UV radiationby chromophoric matrix andionization of matrix

    Dissociation of matrix,phase change to super-compressed gas, chargetransfer to analyte molecule

    Expansion of matrix atsupersonic velocity, analytetrapped in expanding matrixplume (explosion/popping)

    +

    +

    +

    MALDI

  • 7/28/2019 Mass Ionization 21 01 10

    52/67

    MALDI

    Unlike ESI, MALDI generates spectra that have just

    a singly charged ion

    Positive mode generates ions of M + H

    Negative mode generates ions of M - H

    Generally more robust that ESI (tolerates salts and

    nonvolatile components) Easier to use and maintain, capable of higher

    throughput

    Requires 10 mL of 1 pmol/mL sample

    P i i l f MALDI TOF MASS

  • 7/28/2019 Mass Ionization 21 01 10

    53/67

    Principal for MALDI-TOF MASS

    +

    +

    +++

    +

    +

    +

    +

    +

    pulsedUV or IR laser(3-4 ns)

    detector

    vacuum

    strong

    electricfield

    Time Of Flight tube

    peptide mixture

    embedded inlight absorbingchemicals (matrix)

    cloud ofprotonatedpeptide moleculesacc

    V

    P i i l f MALDI TOF MASS

  • 7/28/2019 Mass Ionization 21 01 10

    54/67

    Principal for MALDI-TOF MASS

    Linear Time Of Flight tube

    Reflector Time Of Flight tube

    detector

    reflector

    ion source

    ion source

    detector

    time of flight

    time of flight

    Matrix-Assisted Laser Desorption

  • 7/28/2019 Mass Ionization 21 01 10

    55/67

    Matrix Assisted Laser Desorption

    Ionization (MALDI)

    Sample introduction

    direct insertion probe

    continuous-flow introduction

    Benefits

    rapid and convenient molecular weightdetermination

    Matrix-Assisted Laser Desorption

  • 7/28/2019 Mass Ionization 21 01 10

    56/67

    Matrix Assisted Laser Desorption

    Ionization (MALDI)

    Limitations

    MS/MS difficult

    requires a mass analyzer that is compatible withpulsed ionization techniques

    not easily compatible with LC/MS

    Mass range

    Very high Typically less than 500,000 Da.

  • 7/28/2019 Mass Ionization 21 01 10

    57/67

  • 7/28/2019 Mass Ionization 21 01 10

    58/67

  • 7/28/2019 Mass Ionization 21 01 10

    59/67

  • 7/28/2019 Mass Ionization 21 01 10

    60/67

  • 7/28/2019 Mass Ionization 21 01 10

    61/67

    How is the sample introduced into the

  • 7/28/2019 Mass Ionization 21 01 10

    62/67

    Mass Spectrometer?

    For EI and CI there are four main options Heated reservoir septum inlet for pure gases or

    volatile liquids. Basically this is a heated reservoir

    (~200oC) with a small restriction bleed into the ion

    source. Sample is injected into the reservoir

    through a septum.

    Direct insertion probe for volatile solids. Sample isloaded into a quartz tube at the end of a probe and

    inserted directly into the ion source. The end of the

    probe can then be heated, if required, up to

    temperatures in excess 400oC.

  • 7/28/2019 Mass Ionization 21 01 10

    63/67

    How is the sample introduced into the

  • 7/28/2019 Mass Ionization 21 01 10

    64/67

    Mass Spectrometer?

    For EI and CI there are four main options Particle Beam interface for semi-volatile compounds that

    are amenable to EI and CI.

    Samples are dissolved in a suitable solvent and the solution

    is introduced into the mass spectrometer using a suitable(e.g. HPLC) pump.

    The liquid is nebulised with helium gas to form an aerosol of

    solvent droplets. The stream of liquid droplets passes

    through a desolvation chamber and then a series of nozzles

    and skimmers that remove the solvent and helium, allowing

    a stream of solid particles (the sample) to enter the EI/CI ion

    source.

    How is the sample introduced into the

  • 7/28/2019 Mass Ionization 21 01 10

    65/67

    Mass Spectrometer?

    For FAB / LSIMS Sample can be dissolved directly into the matrix on thetarget or applied dissolved in a miscible solvent. The probeis then inserted in to the mass spectrometer. A dynamicversion of FAB exists, often referred to as continuous flowFAB. Here, the sample, in matrix, is introduced from outsidethe instrument and is then pumped to the target via a lengthof fused silica tubing. Interfacing chromatographictechniques such as HLPC and CZE has been successfully

    achieved with this option, although practical difficulties areoften encountered. Dynamic FAB has largely beensuperseded by ESI, which is a more robust technique.

    How is the sample introduced into the

  • 7/28/2019 Mass Ionization 21 01 10

    66/67

    Mass Spectrometer?

    FOR MALDI:The sample is dissolved in matrix, spotted onto the

    target, allowed to crystallise and then inserted intothe instrument

    How is the sample introduced into the

  • 7/28/2019 Mass Ionization 21 01 10

    67/67

    Mass Spectrometer?

    For ESI For pure samples dissolved in the mobile phase, a directinjection loop can be used. The technique really comes intoits own however, when interfaced to chromatographicprocedures such as CZE, CEC and in particular HPLC.Historically, mass spectrometry and HPLC have beenunhappy bedfellows. ESI has changed all that and the twoare now routinely and reliably interfaced together. Also, withsmaller columns and ever decreasing flow rates being used,

    the amount of sample required for successful analyses isalso reduced, thus effectively increasing the sensitivity of thetechnique dramatically. With CEC being coupled to ananospray (e.g. 50nl/min) ESI interface, attomole detection