Page 126 - Academic Press Encyclopedia of Physical Science and Technology 3rd Chemical Engineering
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 Encyclopedia of Physical Science and Technology  EN002G-87  May 19, 2001  20:3






               524                                                                               Catalyst Characterization


                 The measurement of small-angle scattering of neutrons  backscatter line has been used to measure pore sizes in
               provides information similar to that furnished by other  porous materials. The advantage of the technique is that it
               small-angle techniques, such as small-angle X-ray diffrac-  measures smaller pore sizes than can be measured by gas
               tion. Small-angle scattering results from the differences in  adsorption techniques, and it is capable of measuring pore
               neutron scattering length density of pores and particles in  size distributions as a function of depth within the pellet
               the solid matrix of the catalyst. The method does not dis-  by varying the energy of the incoming ion beam.
               tinguish between open and closed pores. A combination
               of the two techniques provides more complete characteri-
                                                                 C. Radioisotope Techniques
               zation of a supported heavy-metal catalyst. A combination
               of neutron and X-ray scattering and gas adsorption on a  This section deals with spectroscopic methods that depend
               supported metal catalyst measures pore size, metal parti-  on nuclear events. Radiotracer techniques that are very
               cle size, and whether metal has been encapsulated in small  valuable in studying the mechanisms of catalytic reactions
               pores by the conditions of its usage.             have been omitted.
                 Inelastic scattering of neutrons yields neutron scattering
               spectra that measure the vibrational energy levels of the
                                                                   1. M¨ossbauer Spectroscopy
               material under study. For example, the chemisorption of
               water on Raney nickel was shown by inelastic scattering  M¨ossbauer spectroscopy depends on low-level nuclear
               both to produce hydroxyl groups and to chemisorb water  transitions that emit or absorb low-energy γ rays. Cou-
               molecules on the surface at less than monolayer coverages.  pling of the nucleus with its electronic surroundings re-
                                                                 sults in changes in the spectrum of the nuclear energy
                                                                 levels. These changes can be interpreted in terms of the
                 2. Ion Diffraction
                                                                 valence state of the M¨ossbauer atom and the electronic and
               Ion scattering spectrometry and secondary ion mass spec-  magnetic surroundings of its environment. The three basic
               trometry are the best-known types of ion-beam-induced  parameters observed in M¨ossbauer spectra are the isomer
               analyses applicable to catalysis. Other ion-beam tech-  shift δ, quadrupole splitting  E q , and magnetic splitting.
               niques have not enjoyed wide use, probably because ac-  The isomer shift is a result of changes in the electron
               celerators are required to produce sufficiently energetic  density at the nucleus, which produce small changes in the
               ion beams.                                        nuclear energy levels. The result is shifts in the centroid
                 The ISS and SIMS techniques are sensitive to less than  of the M¨ossbauer spectrum relative to a standard material.
               monolayer coverages and detect many of the lighter el-  Asymmetry in the electric field surrounding the nucleus
               ements, including hydrogen. Their application to prac-  produces splitting of the energy levels. Additional split-
               tical catalysts is somewhat limited. The sampling area  ting results from a permanent magnetic field surrounding
                       2
               is ∼1mm , and the results obtained from examining the  the nucleus. The benefits of the detailed information on
               surface of a typical catalyst pellet can be very ambiguous.  oxidation state at the atomic level is offset by the limited
                 Other ion-beam techniques applicable to catalysts  number of elements with useful M¨ossbauer isotopes. The
               are proton-induced X-ray emission (PIXE), Rutherford  application of the  57 Fe isotope has been widespread not
               backscattering, and resonance ion-beam backscattering.  only in the characterization of iron catalysts, but also as an
               The proton-induced X-ray emission technique is very sim-  atomic probe in studies of other supported metal catalysts.
               ilar to electron microprobe analysis. Characteristic X-rays  The spectra in Fig. 23 show the effect of the chemisorp-
               are generated by bombardment of the sample with a pro-  tion of NH 3 on the  57 Fe resonance of a highly dispersed
               ton beam. The advantages of PIXE are high sensitivity,  Fe/SiO 2 catalyst. The iron is in the ferrous state following
               particularly for light elements, and a high signal-to-noise  thehydrogenreductionofmicrocrystallineferricoxidede-
               ratio, which allows analysis even of trace elements in a  posits. The addition of NH 3 to the reduced and outgassed
               few minutes.                                      sample has a marked effect on peak 2 of the spectra. Peak 2
                 In Rutherford backscattering the sample is bombarded  decreases in relative area as small doses of NH 3 are added.
               with light ions such as helium ions, and the energy of the  Since peak 2 has been assigned as half of a doublet pro-
               light ions that have been backscattered from the sample  duced by surface ferrous ions, the relative area of this
               is measured. When the ion is reflected back from the sur-  peak is used as a measure of surface sites available for
               face layer the energy lost is inversely proportional to the  chemisorption. There is no noticeable change in the spec-
               atomic number of the scattering species. By measuring  trum with the addition of the first small amounts of ad-
               the energy loss the element can be identified and a sim-  sorbate. However, the relative area under peak 2 begins to
               ple spectrum obtained. The broadening of the resonant  decrease with further addition of NH 3 , starting at ∼2.0 ×
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