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I Advantages and Disadvantages of Rh

I Advantages and disadvantages of target- and ligand-based NMR screening methods

I Advantages of FTIR

I Advantages of Organonetallies Directly Deposited on Refractory Supports

I Age-Standardized Mortality Ratios for Selected Causes of Death Among 25,000 White California Adventists, 1960-1980

I Aggregation pheromone for I. typographus

I ai tial List of ASTM Standards for Forensic Science

I Air drying of the carrot variety Bauer s Kieler Rote Air temperature

I Airborne Amine and Nltrosamlne Concentrations in a Tire Factory Concentrations in yg m

I Aldehydes fbom 2-Lithio-1,3,5-Tb.ithiane and Alkyl Halides

I Aldehydes from 2-Lithio-1,3,5-Tbithiane and Alkyl Halides

I Algorithm with balanced energy dissipation.

I Alkane Content of Hydrocarbon Minerals and Other Sediments

I Alloy Environment Systems Exhibiting Stress Corrosion Cracking

I Alloy Test Form and condition Composition, Grain size, ASTM Hardness, Rh

I also compares the heat stabilities of 60- and 120-mil plaques at 140 C. The relative order of stabilities has changed slightly. The stability of Resin A in the thicker sections has equalled or surpassed the stability of the long term heat aging Resin B. Resins E, C, and H have improved their position, displacing I, the most stable resin in the 25-mil sheets, which is now third best in the 60-mil plaques and only fourth best in the 120-mil plaques.

I also contains an analysis of the orbital character of these five energy levels. These were determined from the four-component spinors by neglecting the two lower, small, components, and by assuming that the radial functions depend only upon , i.e. that the radial functions for pi 2 and p3 2 or for da 2 and ds 2 are the same. The orbitals may then be written in Pauli form as products of .

I also demonstrates the difference in partitioning for different classes of hydrocarbons shown in Figure 2. Although the classes partition approximately the same, they all show an increase with increase in molecular weight. This happens because the water solubilities decrease more rapidly than the vapor pressures.

I also gives the charge transfer associated with the hydrogen bonded complexes in millielectrons transfered from the AMP or AMS to the substituent. Both AMP and AMS donate approximately the same fraction of electrons to each compound. There is no obvious correlation between the extent of charge transfer and stability of the complex formed.

I also gives the neutron multiplicatibiis obtainable for pure fissionable microspheres at the maximum theoretical density. Here it is seen that a pellet of Cm must have a radius of only about a quarter of that required for Pu to achieve a comjarable neutron multiplication. Additional calculations were run, however, which take into account the diction of the fissionable material with time. These show that, because of depletion, neutron multiplication reaches u. maximum of only 5 X10 at about 3 X10 sec, and then steadily decreases. For the Cm pellet of 0.021-cm radius, a maximum of about 3 x 10 is obtained at about 2.4 x 10 sec.

I also gives the value of u for the triangular and fee lattices. These behave less regularly than C , and take longer to settle down to asymptotic form

I also Illustrates the effect of adding 0.60 of Milube N-32 to a low grade, low micronaire and high trash content cotton. The histograms and cumulative distribution curves of the control and treated cottons are shown in Figures 7 and 8. The results are similar to those found for the other cottons containing additives in that there is a drop of 74.7 in particle count and of 90.8 in dust concentration. The presence of the additive lowers d from 1.62 to 1.09 un over a ramge including 99.95 of the particles and that of the additive-treated cotton is bimodal. The smaller

I also includes a summary of four methods for recovering the hydrocarbon values without mining the oil sand. Three involve combustion as part of the displacement technology. The fourth uses a steam drive to emulsify the oil in water.

I also indicates a noticeable difference in the heat required to maintain a given temperature difference between specimen and liquid bath for the different gases in the gas chamber. This would be expected not only from the different heat transfer characteristics of the various gases, but also because the lower liquid temperatures allow more heat to enter through the tension linkage which extends through the bottom of the cryostat.

I also lists response time as an important performance characteristic of optical sensors. This characteristic is particularly relevant in defining the range and scope of the utility of the sensor that is, the faster the response, the more widespread its applicability. At present, the response of most sensors is limited by the slow diffuslonal mass transport of analyte through an Impermeable polymeric support. Recent studies have shown, however, that response times can be dramatically decreased by the construction of sensors from porous polymeric materials that minimize barriers to the mass transport of an analyte .



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