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Surface region measurements

It is generally believed that EG cleave p-1,4 bonds randomly on the surface of cellulose, and CBH cleave P-1,4 bonds in a processive manner from either the reducing or non-reducing end of a cellulose chain (2,11,13,15). It is not clear, however, whether different cellulases, belonging to either the same or different functional group/family, adsorb initially at the same cellulose surface region. Measuring for individual and mixed cellulases would address this question. [Pg.158]

Figure 2. PDMS concentration in the surface region measured by ESCA for three copolymers. The distance between the horizontal bar and the top of the column represents one standard deviation. Data series A, PDMS2.4K-IP-B2 B, PDMS10K-IP-B2 and C, PDMS27K-IP-B2. Figure 2. PDMS concentration in the surface region measured by ESCA for three copolymers. The distance between the horizontal bar and the top of the column represents one standard deviation. Data series A, PDMS2.4K-IP-B2 B, PDMS10K-IP-B2 and C, PDMS27K-IP-B2.
The most widely used experimental method for determining surface excess quantities at the liquid-vapor interface makes use of radioactive tracers. The solute to be studied is labeled with a radioisotope that emits weak beta radiation, such as H, C, or One places a detector close to the surface of the solution and measures the intensity of beta radiation. Since the penetration range of such beta emitters is small (a ut 30 mg/cm for C, with most of the adsorption occurring in the first two-tenths of the range), the measured radioactivity corresponds to the surface region plus only a thin layer of solution (about 0.06 mm for C and even less for H). [Pg.77]

Photoelectron spectroscopy provides a direct measure of the filled density of states of a solid. The kinetic energy distribution of the electrons that are emitted via the photoelectric effect when a sample is exposed to a monocluomatic ultraviolet (UV) or x-ray beam yields a photoelectron spectrum. Photoelectron spectroscopy not only provides the atomic composition, but also infonnation conceming the chemical enviromnent of the atoms in the near-surface region. Thus, it is probably the most popular and usefiil surface analysis teclmique. There are a number of fonus of photoelectron spectroscopy in conuuon use. [Pg.307]

The strong point of AES is that it provides a quick measurement of elements in the surface region of conducting samples. For elements having Auger electrons with energies hr the range of 100-300 eV where the mean free path of the electrons is close to its minimum, AES is considerably more surface sensitive than XPS. [Pg.1859]

MOKE measurements can be made using relatively simple and inexpensive apparatus, compared to most other surface magnedc probes and surface analytical techniques. MOKE is usefid for the mj netic characterizadon of films of one to several monolayers, thin films, or the near-surface regions of bulk materials. MOKE has... [Pg.733]

Electron spectroscopic techniques require vacuums of the order of 10 Pa for their operation. This requirement arises from the extreme surface-specificity of these techniques, mentioned above. With sampling depths of only a few atomic layers, and elemental sensitivities down to 10 atom layers (i. e., one atom of a particular element in 10 other atoms in an atomic layer), the techniques are clearly very sensitive to surface contamination, most of which comes from the residual gases in the vacuum system. According to gas kinetic theory, to have enough time to make a surface-analytical measurement on a surface that has just been prepared or exposed, before contamination from the gas phase interferes, the base pressure should be 10 Pa or lower, that is, in the region of ultrahigh vacuum (UHV). [Pg.9]

Isothermal a—time curves for the decomposition of U02(CH3C02)2 in air (513—573 K) [1018] showed two approximately linear regions, 0.0 < a < 0.2 and 0.2 < a < 0.9, for which the values of E were 107 and 165 kJ mole-1, respectively. In nitrogen, the earlier portion of the curve was not linear and E = 151 kJ mole-1 for the later interval. The zero-order kinetic behaviour was explained by growth of nuclei in thin, plate-like crystals, which were shown by microscopic and surface area measurements to fragment when a > 0.85. The proposed initial step in the decomposition was fission of bonds between the U02+ and the (OCO CH3) species [1018]. [Pg.217]

The decrease in 0 implies a negative value of SxM or measured value. What we can say is that the modifications occurring in the surface regions of the two phases are such as to decrease 0 and that even larger modifications are observed with other metals, always in the negative direction. Since x ... [Pg.16]

In general one requires that gas and surface be equilibrated, such that they are at the same temperature. This may be a problem at loiv pressures, ivhere the gas molecules collide more often ivith the walls of the vacuum vessel than with the surface under study. Reducing the volume and increasing the pressure to the millibar regime by adding an inert gas helps to establish a region around the crystal where the gas is in thermal equilibrium with the surface. Such measurements are commonly referred to as bulb experiments. [Pg.271]

RBS is based on collisions between atomic nuclei, and it involves measuring the number and energy of ions in a beam which backscatter after colliding with atoms in the near-surface region of a sample. The use of scattering as an analysis tool led to the first in situ chemical analysis of the lunar surface during the landing of Surveyor V. The use of particle accelerators as an a-source was the next powerful step made in Chalk River (Canada) and Arus (Denmark). [Pg.83]


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Measurement surface

Surface region

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