Mass spectrometry (MS) is an analytical technique that measures the mass-to-charge ratio of charged particles. It is used for determining masses of particles, for determining the elemental composition of a sample or molecule. The MS principle consists of ionizing chemical compounds to generate charged molecules or molecule fragments and measurement of their mass-to-charge ratios by using the one of a variety of techniques (e.g EI/CI/ESI/APCI/MALDI).
A) Brief introduction to Electron Ionization (EI) technique
EI is the most appropriate technique for relatively small (m.w.<600) neutral organic molecules which can easily be promoted to the gas phase without decomposition, i.e. volatile. Since EI samples are thermally desorbed to the gas phase and subjected to the high energy of EI, analytes must be thermally stable. The gas phase molecules enter into the ion source where they are bombarded with free electrons emitted from a filament (Figure 1). The electrons bombard the molecules causing a hard ionization that fragments the molecule, and turn into positively charged particles called ions. This is important because the particles must be charged to pass through the analyser.
As the ions continue from the source, they travel through an analyser (electromagnetic/quadrupole/the ion trap) that filters the ions based on mass to charge ratio. The filter continuously scans through the range of masses as the stream of ions come from the ion source. A detector counts the number of ions with a specific mass. This information is sent to a computer and a mass spectrum is created. The mass spectrum is a graph of the number of ions with different masses that traveled through the analyser.
Figure 1. Schematic diagram of EIMS
B) Chemical Ionization (CI) technique
CI technique is especially useful when no molecular ion is observed in EI mass spectrum of a compound, and also in the case of confirming the molecular weight of a compound. CI technique uses nearly the same ion source device as in EI, except, CI uses tight ion source, and a reagent gas (Figure 2).
Figure 2. Schematic diagram of CI interface
Reagent gas (e.g. methane, iso-butane and ammonia) is first subjected to electron impact to yield reagent gas ions. These initial reagent gas ions further undergo ion-molecule reactions with neutral reagent molecules (G) to yield reagent selective ions (reagent plasma, e.g., GH+). When sample is introduced, the sample molecules (M) undergo ion-molecule reactions with reagent plasma to produce sample ions. In general, reagent gas molecules are present in the ratio of about 100:1 with respect to sample molecules. Pseudo-molecular ions, [M+H]+ (positive ion mode) or [M-H]- (negative ion mode) are often observed. Unlike in EI method, the CI process is soft ionization and yields abundant quasi-molecular ions, with less fragment ions.
Positive ion mode: GH+ + M ------> MH+ + G
Negative ion mode: [G-H]- + M ------> [M-H]- + G
The fragmentation pattern of protonated molecules obtained under CI conditions may be different from that of the molecular ions observed under EI conditions. In CI mass spectrometry the molecules of a vaporized sample are ionized by a set of reagent ions (reagent plasma) in a series of ion-molecule reactions. The energy transferred by these reactions is lower than the energy imparted by electrons in EI source, and therefore fragmentation of the sample molecules is greatly decreased. For this reason CI mass spectrometry has been finding increasing use as a tool for the molecular weight confirmation and for elucidation of structure of variety of organic compounds including differentiation of isomeric compounds. Generally hydrogen (H2), methane (CH4), isobutane (iso-C4H10) and ammonia (NH3) are used as reagent gases in CI mass spectrometry; with all these CI gases the compounds form protonated molecule ion in their CI spectra.
C) Electrospray Ionization (ESI) technique
ESI technique involves spraying of a solution of the sample through a highly charged needle so-called capillary which is at atmospheric pressure (Figure 3). The spraying process can be streamlined by using a nebulizing gas. The charged droplets are produced in which the positive or negative ions are solvated with solvent molecules. Heat gas or a dry gas, usually called as desolvation gas is applied to the charged droplets to cause solvent evaporation. The desolvation process decreases the droplet size, leads to the columbic repulsion between the charges present in the droplet and further the droplet fission leads to the formation of individual gas phase analyte ions (that critical point known as the Rayleigh limit), that are guided through ion optics into the mass analyzer.
ESI can produce singly or multiply charged ions. The number of charges retained by a particular analyte depends on several factors such as the size, chemical composition, and higher order structure of the analyte molecule, the solvent composition, the presence of co-solutes, and the instrument parameters. For small molecules (< 2000 Da) ESI typically generates singly, doubly, or triply charged ions, while for large molecules (> 2000 Da) ESI can produce a series of multiply charged ions.
Figure 3. Schematic diagram of a typical ESIMS source phenomenon operating in positive mode
ESI is very suitable for a wide range of biochemical compounds including peptides and proteins, lipids, oligosaccharides, oligonucleotides, bio-inorganic compounds, synthetic polymers, and intact non-covalent complexes.
D) Atmospheric pressure chemical ionization (APCI) technique
APCI has also become an important ionization source because it generates ions directly from solution and it is capable of analyzing relatively non-polar compounds. Similar to electrospray, the liquid effluent of APCI (Figure 4) is introduced directly into the ionization source. The droplets are not charged and the APCI source contains a heated vaporizer, which facilitates rapid desolvation/vaporization of the droplets. Vaporized sample molecules are carried through an ion-molecule reaction region at atmospheric pressure. APCI ionization originates from the solvent being excited or ionized from the corona discharge. Because the solvent ions are present at atmospheric pressure conditions, chemical ionization of analyte molecules is very efficient; at atmospheric pressure analyte molecules collide with the reagent ions frequently.
Figure 4. Schematic diagram of APCI interface
In general, proton transfer occurs in the positive mode to yield [M+H]+ ions. In the negative ion mode, either electron transfer or proton loss occurs to yield M- . or [M-H]- ions, respectively. The moderating influence of the solvent clusters on the reagent ions, and of the high gas pressure, reduces fragmentation during ionization and results in primarily intact quasi-molecular ions. Multiple charging is typically not observed presumably because the ionization process is more energetic than ESI.
E) MALDI technique
Matrix-assisted laser desorption/ionization (MALDI) is a technique to allows the high molecular weight compounds such as organic macro molecules and labile bimolecular into the gas phase as intact ions. MALDI is one of the recent developments of soft ionization techniques in the field of mass spectrometry. It can desorb intact analyte molecular ions with relative masses up to 300KDa. In MALDI-MS analysis, the analyte is first co-crystallized with a larger excess of a matrix compound (CHCA, DBA, Sinapic acid etc), after which, on laser radiation of this matrix-analyte preparation results in desorption of the matrix as a plume, which carries the analyte along with it into gas phase (Figure 5). Thus the matrix plays a key role by strongly absorbing the laser light energy and causing, indirectly, the analyte to vaporize. The matrix also serves as a proton donor and acceptor, acting to ionize analyte in both positive and negative ionization modes, respectively. The TOF analyzers are typically used with the MALDI ionization source.
Figure 5. Schematic diagram of MALDI source
F) Tandem Mass spectrometry/Collision induced dissociation (CID)
The general approach of CID mass spectrometry (MS/MS), in modern terms known as product ion scanning using a triple quadrupole mass spectrometer is shown in Figure 6, and it is routinely used for primary structure determination. The first mass analyzer (MS1) is used to select ion of interest specifically from those transmitted by the ionization source. The precursor ion is passed into the collision cell where it undergoes low-energy collisions with an inert gas (argon or nitrogen) to induce fragmentation. The second mass analyser (MS2) acquires the m/z ratio for all the ions exiting the collision cell. For an MS/MS experiment performed using a triple-quadrupole equipped with an ESI source, a quadrupole/hexapole mass analyzer acts as the collision cell. Using the second quadrupole as a collision cell enables the re-focusing of scattered ions following fragmentation. Similarly, for MS/MS experiments using a quadrupole-time of flight (TOF) mass spectrometer, the precursor is selected using a quadrupole analyzer and the product ions that are formed in the collision cell are analyzed by TOF (Figure 7).
Precursor ion scanning is used to confirm the identity of compounds from a mixture that result in a common daughter ion. For precursor ion scanning, the second mass analyzer (MS2) is fixed to only monitor and transmit product ions of a specific m/z ratio. The first mass analyzer (MS1) is set to scan the whole mass range that includes all the precursor ions whose fragmentation would result in the selected daughter ion.
Figure 6. Schematic of a triple quadrupole mass spectrometer
Figure 7. Schematic of a quadrupole-TOF mass spectrometer