Time atomic mass spectrometry

See also Archaeometry and Antique Analysis Dating of Artifacts Metaiiic and Ceramic Objects. Atomic Absorption Spectrometry Principles and Instrumentation. Atomic Mass Spectrometry Inductively Coupled Plasma. Gas Chromatography Mass Spectrometry. Mass Spectrometry Time-of-Flight Stable Isotope Ratio Clinical Applications Environmental Applications Food Applications Forensic Applications. 

See also Atomic Mass Spectrometry Laser Microprobe. Mass Spectrometry Time-of-Flight. Nitric Oxide. Surface Anaiysis Secondary ion Mass Spectrometry of Polymers Secondary Neutral Mass Spectrometry. 

Meyer, R.T. (1968) Flash Photolysis and Time-resolved Mass Spectrometry. 2. Decomposition of Methyl Iodide and Reactivity of I( Pi/2) atoms. J. Phys. Chem. 72 1583-1591. 

A mass spectrometer is an instrument that produces ions and separates them according to their mass-to-charge ratios, m/z. Most of the ions we will discuss are singly charged so that the ratio is simply equal to the mass number of the ion. Several types of mass spectrometers are currently available from instrument manufacturers. In this chapter, we describe the three types that are used in atomic mass spectrometry the quadru-pole mass spectrometer, the time-of-flight mass spectrometer, and the double-focusing mass spectrometer. Other types of mass spectrometers are considered in Chapter 20, which is devoted to molecular mass spectrometry. The first column in Table 11-1 indicates the types of atomic mass spectrometry in which each of the three types of mass spectrometer is usually applied. 

Direct atomic absorption spectrometry (AAS) analysis of increasing (e 0,10 g) mass of solid samples is the great practical interest since in a number of cases it allows to eliminate a long-time and labor consuming pretreatment dissolution procedure of materials and preconcentration of elements to be determined. Nevertheless at prevalent analytical practice iS iO based materials direct AAS are not practically used. 

In looking for the mechanism, many intermediates are assumed. Some of these are stable molecules in pure form but very active in reacting systems. Other intermediates are in very low concentration and can be identified only by special analytical methods, like mass spectrometry (the atomic species of hydrogen and halogens, for example). These are at times referred to as active centers. Others are in transition states that the reacting cheimicals form with atoms or radicals these rarely can be isolated. In heterogeneous catalytic reaction, the absorbed reactant can... 

In Laser Ionization Mass Spectrometry (LIMS, also LAMMA, LAMMS, and LIMA), a vacuum-compatible solid sample is irradiated with short pulses ("10 ns) of ultraviolet laser light. The laser pulse vaporizes a microvolume of material, and a fraction of the vaporized species are ionized and accelerated into a time-of-flight mass spectrometer which measures the signal intensity of the mass-separated ions. The instrument acquires a complete mass spectrum, typically covering the range 0— 250 atomic mass units (amu), with each laser pulse. A survey analysis of the material is performed in this way. The relative intensities of the signals can be converted to concentrations with the use of appropriate standards, and quantitative or semi-quantitative analyses are possible with the use of such standards. 

Electrothermal vaporization can be used for 5-100 )iL sample solution volumes or for small amounts of some solids. A graphite furnace similar to those used for graphite-furnace atomic absorption spectrometry can be used to vaporize the sample. Other devices including boats, ribbons, rods, and filaments, also can be used. The chosen device is heated in a series of steps to temperatures as high as 3000 K to produce a dry vapor and an aerosol, which are transported into the center of the plasma. A transient signal is produced due to matrix and element-dependent volatilization, so the detection system must be capable of time resolution better than 0.25 s. Concentration detection limits are typically 1-2 orders of magnitude better than those obtained via nebulization. Mass detection limits are typically in the range of tens of pg to ng, with a precision of 10% to 15%. 

The total number of protons and neutrons in a nucleus is called the mass number, A, of the atom. A nucleus of mass number A is about A times as heavy as a hydrogen atom, which has a nucleus that consists of a single proton. Therefore, if we know that an atom is a certain number of times as heavy as a hydrogen atom, then we can infer the mass number of the atom. For example, because mass spectrometry shows that the three varieties of neon atoms are 20, 21, and 22 times as heavy as a hydrogen atom, we know that the mass numbers of the three types of neon atoms are 20, 21, and 22. Because for each of them Z = 10, these neon atoms must contain 10, 11, and 12 neutrons, respectively (Fig. B.7). 

Here small amounts of CO and O atoms were adsorbed at relatively low temperature, after which the surface was heated linearly in time, and the CO2 formation monitored by mass spectrometry. The reaction sequence for this process is... 

In modern times, most analyses are performed on an analytical instrument for, e.g., gas chromatography (GC), high-performance liquid chromatography (HPLC), ultra-violet/visible (UV) or infrared (IR) spectrophotometry, atomic absorption spectrometry, inductively coupled plasma mass spectrometry (ICP-MS), mass spectrometry. Each of these instruments has a limitation on the amount of an analyte that they can detect. This limitation can be expressed as the IDL, which may be defined as the smallest amount of an analyte that can be reliably detected or differentiated from the background on an instrument. 

Montaudo and co-workers have used direct pyrolysis mass spectrometry (DPMS) to analyse the high-temperature (>500°C) pyrolysis compounds evolved from several condensation polymers, including poly(bisphenol-A-carbonate) [69], poly(ether sulfone) (PES) and poly(phenylene oxide) (PPO) [72] and poly(phenylene sulfide) (PPS) [73]. Additionally, in order to obtain data on the involatile charred residue formed during the isothermal pyrolysis process, the pyrolysis residue was subjected to aminolysis, and then the aminolyzed residue analysed using fast atom bombardment (FAB) MS. During the DPMS measurements, EI-MS scans were made every 3 s continuously over the mass range 10-1,000 Da with an interscan time of 3 s. 

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