Molecular Mass Spectrometry

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Molecular Mass Spectrometry Mass Spectrometry: capable of providing information about (1) Elemental composition of samples of matter: atomic mass (2) Structures of inorganic, organic, and biological molecules (3) Qualitative and quantitative composition of complex mixtures (4) Structure and composition of solid surfaces (SIMS) (5) Isotope ratios of atoms in samples

Applications of Mass Spectrometry

History of Mass Spectrometer The first general application of mass spec for routine chemical analysis: - the early 1940s in petroleum industry - quantitative analysis of hydrocarbon mixtures produced in catalytic crackings Commercial mass spec: the early 1950s 1980s: development of various ionization methods (nonvolatile or thermal labile compounds) 1990s: explosive growth in the area of biological mass spec. Nowadays: can be used for the determination of the structure of polypeptides, proteins, and other high-molecular-weight biopolymers

Molecular Mass Spectra Analyte vapor (e.g. ethyl benzene) is bombarded with a stream of electrons Loss of electron and formation of molecular ion (M + ) M + : radical ion and the same MW as the analyte molecule : largest peak Further fragments possible

How Does a Mass Spectrometer Work? Ionization/ desorption Mass Sorting Detection + Source Form ions (charged molecules) Analyzer Sort Ions by Weight (m/z) Ion Detection Detect ions Inlet Solid Liquid Vapor 100 75 50 25 0 1330 1340 1350 Sample Introduction Method to vaporize sample Mass Spectrum Data Analysis

Reason for Vacuum in MS 10-6 to mid 10-5 Torr Avoid ion-molecule reactions Collision free ion trajectories Increase sensitivity Avoid background interference

Sample Introduction Techniques Batch Inlet Systems Classical and simplest Gaseous or liquid samples (b.p. up to 500 o C) Sample is volatilized externally allowed to leak into the evacuated ionization region Direct Probe Inlet Solid and nonvolatile liquids Small sample amounts are needed

Sample Introduction Techniques Batch Inlet Direct Probe/Metal Targets Sample put onto the end of long probe and inserted into the MS Sample spotted with matrix onto a metal plate Gas chromatography: EI, CI, NCI - Sample must be volatile, thermally stable Liquid chromatography: FAB, ESI & APCI - Most widely used separation technique in the pharmaceutical industry - LC/MS applicable to thermally labile, high MW compounds - LC/MS suitable for proteins & peptides - On-line technique

Transducer for Mass Spectrometry Electron Multiplier - Rugged Energetic ions - reliable - high current gains - nanosecond response time Highly enegetic Cu/Be Discrete-dynode e.m. (similar to PMT) : 20 dynodes (G = 10 7 ) Continuous-dynode e.m. - A potential of 1.8 ~ 2KV is applied across the length of the transducer - Gain: 10 5-10 8

Ion Sources in Mass Spectrometer Starting point for a mass spec analysis: formation of gaseous analyte ions Determine the Scope and utility of a mass spec method Determine the Appearance of mass spectra for a given molecule Ionization Techniques Electron Impact (EI) Hard Ionization Fragments Chemical Ionization (CI) Fast Atom Bombardment (FAB) ESI MALDI Soft Ionization Intact

Gas Phase Sources The sample is first vaporized and then ionized Applicable to thermally stable compounds (b.p < 500 o C, MW < 1000) Desorption Sources The sample in a solid or liquid state is converted directly into gaseous ions Applicable to nonvolatile and thermally unstable compounds (MW up to 10 5 ) Do not require volatilization of analyte molecules

Ion Sources in Mass Spectrometer: continued Hard Sources --- Electron Impact (EI) Sufficient energy to cause large fragment of ions Useful information about the structure and functional groups Soft Sources --- Chemical Ionization (CI) Cause little fragmentation of ions Useful information about the MW of the analyte

Electron-Impact Ion Sources Major ion source Historically, ions for mass spectrometry were produced by electron impact Sample is brought into a temperature high enough to produce molecular vapor collision with energetic electrons (70 V: 6.7x10 3 kj/mol, typical bond: 200-600 kj/mol) ionization Positive ions are accelerated into slit W, Re filament (heated): electrons are emitted (-5V) Collision of molecules and e- ionization + 70V 10 3 V for magnetic sector

Electron-Impact Ion Sources Molecular ion Daughter ions (lower mass ions Characteristics of E.I. convenient to use high ion currents good sensitivity extensive fragmentation good for the identification of analytes but disappearance of M + need to volatilize the sample

Electron-Impact Ion Sources Mass spectrometry for biotechnology by Gary Siuzdak, Academic Press, 1996

Electron-Impact Mass Spectra Isotope peaks 12 CH2 35 Cl2 (m = 84) 13 CH2 35 Cl2 (m = 85) 12 CH2 35 Cl 37 Cl (m = 86) 13 CH2 35 Cl 37 Cl (m = 87) 1-pentanol; MW = 88

Electron-Impact Mass Spectra (%)

Chemical Ionization Sources Gaseous sample are ionized by collisions with ions produced by electron bombardment of an excess of a reagent gas (concentration ratio of reagent to sample: 10 3-10 4 ) Reagent gases: CH 4 : most common, other reagents: propane, isobutane, or ammonia) CH 4 reacts with high-energy electrons to give several ions such as CH 4+, CH 3+, and CH 2 + CH 4+,+ CH 4 CH 5+ + CH 3 CH 3+ + CH 4 C 2 H 5+ + H 2 Collision between the sample molecule RH and CH 5+ or C 2 H 5+ are highly reactive Proton or hydride transfer occurs CH 5+ + RH RH 2 + + CH 4 : (M+1) proton transfer (high proton affinity of sample) C 2 H 5+ + RH RH 2 + + C 2 H 4 : (M+1) proton transfer C 2 H 5+ + RH R + + C 2 H 6 : (M-1) hydride transfer (low proton affinity) Most modern mass spectrometer can use E.I and C.I interchangeably

Sample Ionization 1. proton transfer: higher proton affinity than that of reagent CH + + 5 + RH ------ CH 4 + RH 2 (M+H) + C 2 H + + 5 + RH ------- C 2 H 4 + RH 2 (M+H) + 2. alkyl addition: C 2 H + + 5 + RH ------- RH C 2 H 5 (M+29) + C 3 H + + 5 + RH ------- RH C 3 H 5 (M+41) + 3. hydride abstraction : lower PA molecules (M-1) + CH + 5 + RH ------- CH 4 + H 2 + R + C 2 H + 5 + RH -------C 2 H 6 + R +

Electron Impact Sources Chemical Ionization Sources Chemical Ionization Sources

Chemical Ionization Sources Advantages of Chemical Ionization 1. Large (M+H) + ion identifies molecular weight (M) 2. Sensitivity is enhanced by - simple fragmentations (fewer peaks of higher abundance) 3. CI spectra compliment EI spectra Disadvantages of Chemical Ionization 1. Simple fragmentation gives little structural information 2. Ion source contamination 3. Control reagent gas flow

EI versus PICI for Pesticides EI Spectrum of Heptachlor PICI Spectrum of Heptachlor Intensity is low for any single m/z ion. Intensity is concentrated in [M+H] + ion. Spectrum is simpler.

Field Ionization Sources - Ions are formed under the influence of a large electric field (10 8 V/cm) by applying high voltages (10-20 kv) to specially formed emitters with diameter less than 1 m oxidation of analytes at the tip -The gaseous sample from a batch inlet system is allowed to diffuse into the high-field area around the microtips of anode - The spectrum is simple: (M+1) + peak - Low sensitivity (one order lower than E.I) Developed in 1969

Desorption Sources - Applicable to nonvolatile or thermally labile compounds (biomolecules, even MW> 10 5 Da) - Energy in various forms is introduced into the solid or liquid samples to cause direct formation of gaseous ions - Simple spectra (M + or M+1 + ) - Field desorption, FAB, MALDI, and ESI Field Desorption - Electrode (emitter) is mounted on a probe that is coated with a solution of sample - After the probe is inserted into sample compartment, ionization takes place by applying a high voltage to the electrode - Spectrum is even simpler than that of field ionization

Fast Atom Bombardment (FAB) Ionization Applicable to polar high-molecular-weight species (thermally unstable compounds; biochemical compounds) Samples in a condensed state (often in glycerol or m-nitrobenzyl alcohol) are ionized by bombardment with energetic (several kev) Xe, Ar or Cs atoms FAB provides rapid heating reduce sample fragment provides molecular ions

FAB Ionization Sources FAB source also called liquid secondary-ion source -A beam of fast atom is obtained by passing accelerated argon or xenon ions from an ion source, or gun through a chamber containing argon or xenon atoms at a pressure of about 10-5 torr. - The high-velocity ions undergo a resonant electronexchange with the atoms without substantial loss of translational energy.

Matrix for FAB Ionization

FAB Ionization Sources

Matrix-Assisted Laser Desorption/Ionization (MALDI) -Ionization method for accurate MW information about polar bioploymers -A low concentration of the analyte is uniformly dispersed in a solid or liquid matrix on the end of a stainless steel probe or placed on a metal plate. - The plate is then placed in a vacuum chamber and a laser beam is focused onto the sample - The MALDI matrix must strongly absorb the laser radiation. - The matrix and analyte are then desorbed and ionized, creating an ion plume.

MALDI

MALDI Matrix Ratio of analyte to matrix is 1:10 3 to 1:10 5 Nitrogen laser (337 nm) Nd-YAG (266 and 355 nm) Excimer (308 nm)

MALDI Spectrum -The most common type of mass analyzer used with MALDI is the time-of-flight (TOF). - low background noise - no fragment - multiply charged ions, dimer, and trimer species trimer dimer

Matrix-Assisted Laser Desorption/Ionization

MALDI/TOF 1. Sample is mixed with matrix & dried on target Ions are accelerated by an electrical field to the same kinetic energy, and they drift (or fly) down a field free flight tube where they are separated in space 20-30 kv Flight tube 5. Ions strike the detector at different times, depending on the mass to charge ratio of the ion. 2. Target is introduced into high vacuum of MS High vacuum High voltage 3. Sample spot is irradiated with laser, desorbing ions into the gas phase and starting the clock measuring the time of flight. Pulsed laser Tim e 6. A data system controls all instrument parameters, acquires the signal vs. time, and permits data processing.

Electrospray Ionization ESI takes places under atmospheric pressures and temperatures Sample is pumped through a SS capillary needle at a rate of few ml/min The needle is maintained at ~ kv against a cylindrical electrode that surround the needle Charged spray of fine droplet pass through a desolvating capillary evaporation of solvent and formation of charged analyte SS capillary needle (~kv) 2002 Nobel Prize: John B. Fenn

Electrospray Ionization

Electrospray Ionization

Electrospray Ionization

LC-MS CE-MS Electrospray Ionization

Mechanism of Ionization

Transfer of charged molecule into the gas phase Mechanism of Ionization

Mechanism of Ionization 5. Electron ejection Halogenated compounds

Mass Analyzers All analyzers sort ions based on their mass-to-charge ratios (m/z) Magnetic Sector 1970s/80s TOF Q-TOF 1950s/60s 1980s/90s 1990s- 2000s- Quadrupoles Ion Traps

Mass Analyzers

In order to resolve peaks at m/z of 400.0 and 400.1 R of 4000 is needed Most common MS: R < 2000 High-resolution MS: R ~ 10 5

General Comparison of Mass Analyzers Mass analyzer mass range and resolution Advantages Disadvantages Quadrupole Range m/z 3000 Resolution 2000 Ease of switching between positive/negative ion Small size Relatively low cost Small size Medium resolution Mass range limited to about 3000 m/z Poor adaptability to MALDI Ion trap Range m/z 2000 Resolution 1500 Simple design, low cost Well-suited for tandem mass spectrometry (MS n, n 4) Easy for positive/negative ions Limited mass range of current commercial versions;however, progress is being made in their development Magnetic sector Range m/z 20,000 Resolution 10,000 Capable of high resolution Capable of exact mass Medium mass range Can be very reliable, manufacturer dependent Not tolerant of high pressure Expensive Instrumentation is massive Relatively slow scanning Time-of-flight (TOF) Range m/z Resolution 350 Highest mass range Very fast scan speed Simple design, low cost Ease of adaptation to MALDI Low resolution Difficulty of adaptation to electrospray Time-of-flight refrectron Range m/z Resolution 1500 Good resolution Very fast scan speed Simple design,low cost Good resolving power has limited m/z range Lower sensitivity than TOF Fourier transform-mass spectrometry (FT-MS) Range m/z 10,000 Resolution 30,000 High resolution Well-suited for tandom mass spectrometry (MS n, n 4) High vacuum (<10-7 Torr) required Superconducting magnet required, expensive Instrumentation massive

Magnetic Sector Analyzer 70 ev ~ 400 ev ½ mv 2 = zev v = (2zeV/m) 1/2 -- (1) mv 2 /r = ZeVB => v = zebr/m (centripetal force) (magnetic force) (2) (1) = (2) => m/z = er 2 B 2 /2V r = circular path of radius B: magnetic filed (variable) V; accelerating voltage Fig 22-2

Magnetic Sector Analyzer ½ mv 2 = zev v = (2zeV/m) 1/2 -- (1) r = circular path of radius mv 2 /r = ZeVB => v = zebr/m (centripetal force) (magnetic force) (2) (1) = (2) => m/z = er 2 B 2 /2V B: magnetic filed (variable) V; accelerating voltage

Double Focusing Magnetic sector analyzer: single focusing High-resolution MS: R = 10 5 Inhomogeneous electric field in ion source To focus a beam of ions having a narrow band of kinetic energy Ions with different mass but constant KE are separated by their trajectories in magnetic field Variation of kinetic energy of ions emerging from ion source => Limit the resolving power of magnetic sector analyzer

Double Focusing

Mass Analyzer for Mass Spectrometry Quadrupole Mass -More compact, more rugged, less inexpensive than magnetic sector mass spec - high scan rate (less than 100 ms) Ions are accelerated into the space between rod by a potential of 5-10 V Only ions having a limited range of m/z reach the detector It is difficult to deflect heavier ion than a lighter ion

Tim-of-Flight Mass Analyzer Ions are accelerated by an electric field 10 3-10 4 V KE = qv = zev = ½ mv 2, v = L/t Time of flight, t = L [(m/e)(1/2v)] 1/2 Heavier ions slower v longer flight time

Tandem Mass Spectrometry Tandem Mass: Coupling of one mass spec to a second: good for the analysis of mixture The first: isolate the molecular ions of various components of a mixture The second: molecular ions are further fragmented

Tandem Mass Spectrometer Soft ionization He is pumped; Further ionization occurs as a consequence of collision of the rapidly moving parent ions with the resident He atoms

Tandem Mass Spectrometry Analysis of isomers (ABCD and BCDA) in mixture (UKL, UMN, and others) (1) Soft ionization in the first MS : set to transmit ions with an m/z values corresponding to ABCD + and BCDA + (2) Further fragments in the second MS. -AB +, CD +, BC +, DA + - Identification of isomers MW=278 MW=278

GC-Mass Spectrometer Mass spectrometer is a powerful detector for both qualitative and quantitative analysis of analyte in gas or liquid chromatography Analyte: ionized Ionized analyte: separated according to mass Ions: detected

GC-Mass Spectrometer Remove most of carrier gas 50% of analyte molecules goes to skimmer

GC-Mass Spectrometer CH 3 CH 2 CH 2 CH 2 OH + Br - CH 3 CH 2 CH 2 CH 2 Br + OH - 1-butanol 1-bromobutane <Total ion current> <peak 1> <peak 2>

LC/MS(/MS) Application Areas Pharmaceutical Drug Discovery Clinical Trials Drug Production (QA/QC) Biomolecules Forensic and Doping Environmental Medical diagnostics The MS detector for HPLC

Incompatibilities between HPLC and MS Two most dominant ionization methods in LC-MS : pneumatically assisted electrospray and atmospheric pressure chemical ionizaion (APCI)

APCI in LC-Mass - APCI uses heat and a coaxial flow of N 2 to convert eluate into a fine aerosol mist from which solvent and analyte evaporate - Like C.I., APCI creates molecular ions (MH + ) from gas phase reactions between ions and molecules Nebulizing gas (N 2 ) -100V -140V

APCI in LC-Mass From Harris book, 6 th edition, Quantitative Chemical Analysis -Protonated MH + can be formed in the following manner. N 2 + e- N 2+ + 2 e- N 2+ + 2N 2 N 4+ + N 2 N 4+ + H 2 O H 2 O + + 2N 2 H 2 O + + H 2 O H 3 O + + OH H 3 O + + nh 2 O H 3 O + (nh 2 O) n H 3 O + (nh 2 O) n + M MH + + (n+1)h 2 O Analyte M might also form a negative ion by electron capture: M + e M - A molecule X-Y can produce negative ions by reaction such as X-Y + e- X + Y - The species Y - could abstract a proton form a weakly acidic analytes: AH + + Y - A - + HY