Overview Literature on Matrix Assisted Laser Desorption Ionization Mass Spectroscopy (MALDI MS): Basics and Its Applications in Characterizing Polymeric Materials

Overview Literature on Matrix Assisted Laser Desorption Ionization Mass Spectroscopy (MALDI MS): Basics and Its Applications in Characterizing Polymeric Materials

Bull. Mater. Sci., Vol. 28, No. 6, October 2005, pp. 515–528. © Indian Academy of Sciences. Overview literature on matrix assisted laser desorption ionization mass spectroscopy (MALDI MS): basics and its applications in characterizing polymeric materials R N JAGTAP* and A H AMBRE Polymer Engineering and Technology Department, University of Mumbai, Institute of Chemical Technology, Mumbai 400 019, India MS received 30 December 2004; revised 11 April 2005 Abstract. Matrix assisted laser desorption ionization mass spectroscopy (MALDI MS) is a technique which allows the measurement of molecular mass > 200,000 Daltons by ionization and vapourization without degra- dation. This technique is useful for the mass analysis of synthetic polymers, which have very low volatility. The basic principles of and its applications for polymer characterization have been discussed in this paper. In addition, the possibilities of combining MALDI MS with chromatographic and other analytical techniques have also been discussed. Keywords. MALDI; mass spectroscopy; gel permeation chromatography (GPC); ion fragmentation; copoly- mer analysis. 1. Introduction The use of lasers for generating ions began from the early 1960s. These ions were used for analysis in MS The chemical structures of polymers are characterized (Vastola et al 1970). Researchers have used a wide variety typically by determining the repeat units i.e. monomers, of lasers of different wavelengths and pulse widths and end-groups that cap the polymer chains and the molecu- tried to combine them with various spectrometers. The lar weight distribution. Polymer characterization with mass first systematic attempt to generate ions from organic spectroscopy, MS, is not possible as MS requires gas- molecules began from the early 1970s (Posthumus et al phase ions for a successful analysis and polymers are 1978; Kupka et al 1980). Numerous systematic observa- composed of large, entangled chains that are not easily tions led to two general principles. First, efficient and converted to gas phase ions. Traditional mass spectro- controllable energy transfer to the matrix, lasers emitting scopic techniques developed for polymer analysis, like in the far ultraviolet which can couple to electronic states, pyrolysis gas chromatography use thermal energy to va- or far-infrared, give the best results. Second, to avoid ther- pourize non volatile samples like polymers. Although mal decomposition of the thermally labile molecules, the thermal energy also decomposed polymers into constituent energy must be transferred in a very short time. Usually, parts leading to fragmentation, the full chemical structure lasers with pulse widths in the range of 1–100 ns are information used to be lost during vapourization. used. These lasers can be easily focused on small spot A new technique has been developed to measure this sizes that are comparatively smaller than the other di- aspect of polymer sample. This new technique is known mensions of the ion source and hence are essentially gene- as matrix assisted laser desorption ionization mass spec- rated at a point source in space and time. This makes troscopy (MALDI MS). It is perhaps the most important these lasers easily compatible with time of flight (TOF) mass spectroscopy method used to analyse polymer sys- mass spectrometers. tems. It is a special case of MS, using specific sample Early experiments on laser desorption of organic ions preparation methods and low fluence laser desorption to revealed that there was an upper limit on the size of the create the analyte ions. It was invented by Tanaka and his molecules that can be desorbed as intact ions. This limit was co-workers (Karas and Hillenkamp 1988; Tanaka et al dependent on the molecular structure and was 1000 Da 1988; Bahr et al 1992). MALDI MS has rapidly grown in for biopolymers and 9000 Da for synthetic polymers and applications ranging from sequencing peptides to measuring laser parameters. These limitations were due to the reso- the average molecular weights of complex synthetic nant excitation of the analyte molecules, necessary for polymer materials. the controllable non-explosive energy transfer and also put energy into the photo dissociation channels. In non- *Author for correspondence resonant desorption experiments, the necessary irradia- (jagtap–[email protected], [email protected]) tions are very close to the onset of plasma generation, 515 516 R N Jagtap and A H Ambre which destroyed the large organic molecules. An impor- In the linear time of flight (TOF) analyser, the distribu- tant breakthrough towards the higher mass organic mole- tion of molecules emanating from a sample is imparted to cules was achieved by Karas et al (1987) who observed identical translational kinetic energies after being sub- that the use of matrix could avoid this problem. Thus, the jected to the same electrical potential energy difference. concept of MALDI MS came into existence. The ions travel the same distance down an evacuated field free drift tube. The smaller ions arrive at the detec- tor in a shorter time than the more massive ions. Sepa- 2. Principle of MALDI MS rated ion fractions at the end of the drift tube are detected by an appropriate recorder that produces a signal upon MALDI is a soft ionization technique in which the en- impact of each ion group. The digitized data generated from ergy from the laser is spent in volatilizing the matrix successive laser shots are added up yielding a TOF mass rather than degrading the polymer. Figure 1 elucidates spectrum. The TOF mass spectrum is a recording of the the principle of this technique. signal as a function of time. The time of flight (TOF) for This technique is based upon an ultraviolet absorbing a molecule of mass, m, and charge, z, to travel this dis- matrix. The matrix and the polymer are mixed at a mole- tance is proportional to (m/z)1/2. This relationship can be cular level in an appropriate solvent. The solvent helps used to calculate mass of the ions. Through calculation of prevent aggregation of the polymer. The sample–matrix mass of the ions, conversion of TOF mass spectrum to a mixture is placed on the sample probe tip, under vacuum conventional mass spectrum of mass to charge axis can conditions; the solvent is removed, leaving co-crystal- be achieved as shown in figure 2. lized polymer molecules homogenously dispersed within matrix molecules. When the pulsed laser beam is tuned to the appropriate frequency, the energy is transferred to the 3. Advantages of MALDI MS matrix which is partially vapourized, carrying intact polymer into the vapour phase and charging the polymer (I) One of the key advantages of MALDI MS is that the chains. absolute molecular weights of oligomers can be deter- Figure 1. Principle of MALDI. Figure 2. Conversion of TOF spectrum to mass spectrum. Overview literature on MALDI MS 517 mined as opposed to obtaining relative molecular weights (II) Some polymers such as teflon, polyimide and poly- by chromatographic techniques. MALDI MS does not urethane still cannot be characterized by MALDI MS require polymer standards to assign molecular weights to (Analytical Chemistry News and Features 1998). oligomers, and the technique permits accurate determina- (III) It is difficult to analyse complex mixtures of surfac- tion of molecular weights from narrowly distributed tants. Quantization of mixtures is quite difficult (Hanston polymers with polydispersity < 1×2 (Kuang and Odom 2004). 1998). (IV) MALDI MS is also challenged by chemistry that has (II) The speed and information obtained by MALDI MS too little functionality to stabilize a cation in the gas phase. are significantly more than that obtained with other con- For example, saturated hydrocarbons like polyethylene and ventional molecular weight determination techniques. polypropylene are difficult to analyse by MALDI (Analy- (III) MALDI MS can determine molecular weight inde- tical Chemistry News and Features 1998; Hanston 2004). pendent of the polymer structure. For example, rigid rod polymers such as tetrahydropyrene are very difficult to 5. Sample preparation analyse by conventional analysis technique such as gel permeation chromatography because these polymers have The sample preparation for polymer MALDI must ac- stick-like geometry. Most polymers have flexible back- complish five different roles (Analytical Chemistry News bones that form random coil conformations in solution. and Features 1998; Hanston 2004), one for the solvent These polymers are readily analysed by GPC methods, and four for the matrix. The roles are as follows which are based on relating the hydrodynamic volume of · The solvent must effectively separate the polymer the coiled polymer chains with molecular weight. How- molecules. We need to minimize the interactions bet- ever, the hydrodynamic volume of the rigid rod polymers ween the polymer molecules and generate individual does not correlate with molecular weight. Hence molecu- molecules for the MALDI experiment to analyse. lar weights determined by gel permeation chromatogra- · Isolate the oligomers: The matrix must maintain the phy often deviate from the true values for such polymers. separation of the oligomers obtained by dissolving the (IV) MALDI MS can be used to analyse materials that polymer in a good solvent. are difficult to characterize by GPC methods, because of · Absorb energy: The matrix must absorb energy deli- either solvent or column incompatibilities. Moreover, vered to the sample, usually wavelength of 337 nm of GPC does not perform well in low-molecular-weight re- the laser. gions (masses < 20 kDa), whereas MALDI MS works very · Desorb the analyte: The matrix must convert the en- effectively in this mass range. Polymer characteristics ergy delivered by the laser to eject the molecules in that can readily be determined by MALDI MS include the gas phase. molecular weight averages (including the number [M ] n · Ionize the analyte: The matrix must provide an ioniza- and weight [M ] averaged molecular weights), polydis- w tion path for the analyte molecules. persity, mass of repeat units, and end-group mass struc- ture.

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