Peak cleaning procedure

Spectra for a series of Cu-Ni alloys have been obtained (91) and these are reproduced in Fig. 11. Because of overlapping of peaks from the component metals, separate indications of each element are only obtained from the 925 eV Cu peak and the 718 eV Ni peak. The results have only qualitative significance because the quoted nickel concentrations are bulk values. Nevertheless, they do suggest that for these particular samples of Cu-Ni alloys, the surface composition varies smoothly from pure copper to pure nickel. Auger spectroscopy has subsequently shown that the surface composition of the (110) face of a 55% Cu-Ni crystal was identical with the bulk composition (95a). Ono et al. (95b) have used the technique to study cleaning procedures argon ion bombardment caused nickel enrichment of... 

Alkaline-cleaned substrate. After alkaline cleaning, the steel substrate was completely devoid of aliphatic fatty acids, as was verified by TOFSIMS. The freshly cleaned substrate was immediately immersed in the 1% silane solution and analyzed. The wettability of the cleaned steel by the solution was considerably improved by the alkaline cleaning procedure. The spectra obtained with a film deposited from a pH 10.5 solution are shown in Fig. 7. A rigorous peak identification procedure was applied here. The masses of all major peaks could be... 

On the other hand, the intensity of TSD (1 peaks is proportional to the volume concentration of ether groups in the polymer. Peak cleaning and partial heating procedures allow us to separate the (32 process from the total TSD spectrum. Probably, one of the (3 peaks corresponds to crankshaft-type motion. 

Kazimierczuk and co-workers apphed their semi-automatic CLEAN procedure to suppress artifacts in a randomly sampled N-labeled NOESY-HSQC spectrum of ubiquitin [60]. It was demonstrated that the process does not systematically influence relative peak amplitudes, and is therefore applicable to NOESY spectra. Similar conclusions were later drawn by Stanek and Kozmihski [85], and by Werner-AUen and co-workers [84], who compared their reconstructions with conventionally sampled three-dimensional spectra of the same spectral resolution. The algorithm proposed by Kazimierczuk and co-workers was later also applied to higher-dimensional experiments [80]. 

If we inject manually, the syringe, the syringe needle or the injector seal can be contaminated and cause the occurrence of the extra peak. Simply interchanging different syringes can help pinpoint the source of the problem. In an automated injector, the same parts can be causing the problem. Cleaning procedures for these parts should be investigated. 

With correct experimental procedure TDS is straightforward to use and has been applied extensively in basic experiments concerned with the nature of reactions between pure gases and clean solid surfaces. Most of these applications have been catalysis-related (i. e. performed on surfaces acting as models for catalysts) and TDS has always been used with other techniques, e.g. UPS, ELS, AES, and LEED. To a certain extent it is quantifiable, in that the area under a desorption peak is proportional to the number of ions of that species desorbed in that temperature range, but measurement of the area is not always easy if several processes overlap. 

Procedure Dissolve accurately 22.5 mg of /ram-clomiphene citrate and 52.5 mg of cis-clomiphene citrate (approx. 1 2.3) into 10 ml of DW in a clean 50 ml separating funnel. Add to it 1 ml solution of sodium hydroxide (5% w/v in DW). In the alkaline medium the base is liberated which is extracted successively with 3 portions of solvent ether (10 ml each). The combined ethereal layer is washed with two portions of DW (10 ml each). The resulting ethereal fraction is dried over anhydrous sodium sulphate, filter, evaporate to diyness carefully over an electric water-bath and dissolve the residue in 1 ml of CS2. Now, record the absorption curve in a 0.2 mm cell over the range 12.50 to 14.00 pm. Calculate the absorbance for the peaks at 13.16 and 13.51 pm respectively by employing the base-line method (see section 3. l. B in this chapter) between the minima at 12.66 and 13.89 pm. 

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