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Apparatus development

The method for studying intennediate exchange in NMR is to obtain an excellent equilibrium spectmm of tlie system as a fiinction of temperature. Then the theoretical apparatus developed above can be used to simulate and to fit the experimental data, in order to obtain the rate data. [Pg.2105]

In the late 1980s, Brodie crystalHsers were installed in the United Kingdom and in France for upgrading phthaHc-grade naphthalene to 99% purity or better. This apparatus, developed by Union Carbide Corporation, AustraHa, for separating o- and -dichlorobensene, was adapted for naphthalene refining. The one installed in the United Kingdom, however, has been closed (21) (see Naphthalene). [Pg.341]

Recent innovations [19] have circumvented the heat dissipation and sample stream distortion inherent in most of the previous designs. In one apparatus, developed by R S Technologies, Inc. (Wakefield, RI, USA), Teflon capillary tubes are aligned close to each other in the electrophoretic chamber. Coolant is pumped through the Teflon capillary tubes during the electrophoretic run while the electrophoretic separation is accomplished in the interstitial volume between the Teflon tubes. [Pg.294]

In a different approach, Stalcup and co-workers [25] used sulfated (3-cyclodextrin for the enantioseparation of piperoxan in work directly derived from earlier CE and classical gel results. Their results were obtained using a continuous free flow apparatus developed by R S Technologies, Inc. Processing rates on the order of 4.5 mg h were reported. [Pg.294]

There are several techniques available for SFA to drive a sample along the normal direction and to position it to a specified site. A common feature of these techniques is to employ a multi-stage driving system of increasing sensitivity. The apparatus developed by Israelachivili s team, for example, uses a two-stage screw as the coarse and medium control, which gives positioning accuracy of 1 /rm and 1 nm. [Pg.16]

Method A Agitated Glass Ampoule. The bench scale apparatus developed for these runs consisted of a 12 mm O.D. glass ampoule suspended in a fluidized bed heater (Figure 1). Approximately 1 g of polypropylene pellets (Himont) were placed in the ampoule and preheated for 2 min. at 220°C. A 29 cm long screw with a pitch of 1 mm and a diameter of 6 mm driven at approximately 160 rpm was inserted into the ampoule. The appropriate amount of free-radical initiator, 2,5-dimethyl-2,5-bis(t-butyl peroxy) hexane (Lupersol 101, Lucidol), required for a 0.04 wt% initiator concentration was then injected into the sample... [Pg.510]

These are total systems or even plants made for parallel automated organic synthesis, typically in the liquid phase. In this section, no commercial devices (typically not relying on micro flow processing) are considered, but rather only specialty apparatus developed in the framework of chemical micro processing. [Pg.417]

A schematic of the apparatus developed is shown in Fig. 3. Stirrers mix and push the lighter and heavier phases in each compartment, with the maximum rotation speed governed by the need to maintain the interface steady. Flow deflectors ensure that the phases are circulated in each chamber and that flow near the interface is laminar. The interfacial plate (thickness 2 mm) is rectangular with a hole at its center. The distance from the interface to the flow deflectors is less than 6 mm. The two phases are analyzed by withdrawing small volumes via sampling holes. [Pg.336]

The structure of the review is organized as follows. In Section 6.2, we will address experimental aspects concerning apparatus developments and oxide nanolayer preparation methods, and briefly comment on the interplay between experimental and theoretical results. Section 6.3 constitutes the main body of this chapter, where we present case studies of selected oxide-metal systems. They have been chosen according to their prototypical oxide nanosystem behavior and because of their importance in catalysis. We conclude with a synopsis and a brief outlook speculating on future developments. [Pg.149]

Apparatus, developed in this laboratory for two types of thermochemical measurements—(a) gas-phase ion molecule equilibria and (b) collision-induced dissociation (CID) threshold measurements—will be described. For both purposes, a triple quadrupole mass spectrometer is used. It is only the front end modifications that provide the conditions for (a) or (b). [Pg.273]

An apparatus developed by Rapra for the determination of the scorch and cure... [Pg.71]

The Carman-Kozeny equation relates the drop in pressure through a bed to the specific surface of the material and can therefore be used as a means of calculating S from measurements of the drop in pressure. This method is strictly only suitable for beds of uniformly packed particles and it is not a suitable method for measuring the size distribution of particles in the subsieve range. A convenient form of apparatus developed by Lea and Nurse 22 1 is shown diagrammatically in Figure 4.4. In this apparatus, air or another suitable gas flows through the bed contained in a cell (25 mm diameter, 87 mm deep), and the pressure drop is obtained from hi and the gas flowrate from h2. [Pg.203]

Until recently, previous studies for continuous monitoring of hepatic function with ICG utilized the absorption mode. However, new studies demonstrate that the highly sensitive fluorescence technique can equally be used [148-150]. In addition to high sensitivity, in-depth analysis of the emission, excitation and polarization properties of fluorescence spectroscopy furnishes additional functional information about the dye molecule. In this system, the fluorescence profile emanating from the clearance of injected biocompatible dye is monitored with a small photodetector. Fig. 8 shows the in vivo fluorescence detection apparatus developed for continuous monitoring of organ functions [147,148]. [Pg.48]

The apparatus developed for yb measurements of BLM deserves brief comment since it can be used not only to examine the effects of various substances on BLM but is readily adaptable for studying other types of interfacial films and related adsorption phenomena at either air-water or oil-water interfaces (and bifaces). Unlike both the Wil-helmy plate and film balance methods, the present technique measures 7i directly. From the description of the apparatus and procedure that the present method relies on the ability to measure the very small pressure difference across an interface (or biface). For certain BLM s, the pressure heads measured are only fractions of a millimeter of water. Therefore, the method described here has been possible only as a result of developing pressure transducers of high sensitivity. [Pg.119]

Fig. 6.1. Representation of the optical alignment of the apparatus developed at the Central Laboratory TNO... Fig. 6.1. Representation of the optical alignment of the apparatus developed at the Central Laboratory TNO...
THERMAL PRECIPITATION. Sinclair (13D, Chap. 8) describes an apparatus developed to test the theory of thermal precipitation. An aerosol particle will move in a temperature gradient from a hot body toward a colder body with a velocity proportional to the temperature gradient. [Pg.146]

The apparatus developed above is rigorous with respect to the calculation of the ZFS but suffers from transparency. On its output we get the numbers, but it might be difficult to control and tune them. It would be helpful to have a set of formulae as simple as possible that, even with a limited applicability, could provide a better understanding of the crucial factors that determine the ZFS and other MPs. Considerable work has been done so far in this respect however, no comprehensive review of this approach exists. [Pg.46]

Fig. 3.15. Schematic illustration of the crossed-beam apparatus developed by Hyder et al. (1986) for the measurement of positron elastic differential scattering cross sections. Reprinted from Physical Review Letters 57, Hyder et al, Positron differential elastic scattering cross section measurements for argon, 2252-2255, copyright 1986 by the American Physical Society. Fig. 3.15. Schematic illustration of the crossed-beam apparatus developed by Hyder et al. (1986) for the measurement of positron elastic differential scattering cross sections. Reprinted from Physical Review Letters 57, Hyder et al, Positron differential elastic scattering cross section measurements for argon, 2252-2255, copyright 1986 by the American Physical Society.
Fig. 4.12. Schematic of the apparatus developed by Fornari, Diana and Coleman (1983) for studies of positronium formation. Reprinted from Physical Review Letters 51, Fornari et al., Positronium formation in collisions of positrons with He, Ar and H2, 2276-2279, copyright by the American Physical Society. Fig. 4.12. Schematic of the apparatus developed by Fornari, Diana and Coleman (1983) for studies of positronium formation. Reprinted from Physical Review Letters 51, Fornari et al., Positronium formation in collisions of positrons with He, Ar and H2, 2276-2279, copyright by the American Physical Society.
Fig. 4.15. Illustration of the apparatus developed by Zhou et al. (1994b) for studies of positronium formation in positron-alkali metal collisions. Fig. 4.15. Illustration of the apparatus developed by Zhou et al. (1994b) for studies of positronium formation in positron-alkali metal collisions.
Fig. 5.18. Schematic illustration of the apparatus developed by Kover and coworkers for studies of positron-impact differential ionization cross sections. Reprinted from Journal of Physics B26, Kover, Laricchia and Charlton, Ionization by positrons and electrons at 0°, L575-L580, copyright 1993, with permission from IOP Publishing. Fig. 5.18. Schematic illustration of the apparatus developed by Kover and coworkers for studies of positron-impact differential ionization cross sections. Reprinted from Journal of Physics B26, Kover, Laricchia and Charlton, Ionization by positrons and electrons at 0°, L575-L580, copyright 1993, with permission from IOP Publishing.
Thermalization in N2 gas has also been studied using the positron-trap apparatus developed by Surko and coworkers and described in subsection 6.2.2. By storing positrons in the trap at a known pressure for various lengths of time before ejecting them and measuring their mean... [Pg.285]

Figure 3.23 Schematic of the apparatus developed by Ward et al. [52] to prepare water-cast composite membranes. Reprinted from J. Membr. Sci., 1, W.J. Ward, HI, W.R. Browall and R.M. Salemme, Ultrathin Silicone Rubber Membranes for Gas Separations, p. 99, Copyright 1976, with permission from Elsevier... Figure 3.23 Schematic of the apparatus developed by Ward et al. [52] to prepare water-cast composite membranes. Reprinted from J. Membr. Sci., 1, W.J. Ward, HI, W.R. Browall and R.M. Salemme, Ultrathin Silicone Rubber Membranes for Gas Separations, p. 99, Copyright 1976, with permission from Elsevier...
Ref 34 and pamphlets which can be obtained from the firm). An apparatus developed during WWII by the National Research Council of Canada under the name of Ottawa Chronograph was also used in US. Its description is given in Ref 30a, pp 28-34 In addn to Potter Co, the following US firms are engaged in manuf of counter chronographs a) Berkeley Division of Beckman Instruments, Inc, Richmond, Calif b) Hewlett-Packard Co, Palo Alto, Calif c) Computer Measurements Co, San Fernando, Calif d) The Detectron Corp, North Hollywood, Calif and e) Lavoie Laboratories, Inc, Motganville, NJ There are probably other firms, but we have no info on their products... [Pg.92]

DTA(2) data were obtained with a Model DT-40 DTA apparatus (Shimadzu Co., Ltd.) at Yoshida laboratory. Since the DSC apparatus developed problems frequently, an attempt was made to use a DTA apparatus in screening tests for the hazards of reactive substances. The sample cell used was the same as in DSC(l). Qdta(2) was determined by using the apparatus constant, k, at each temperature as obtained in the DTA evaluation of the standard substances listed above. The DTA curve was stored on a floppy disk by a Model PC-9801 personal computer (NEC), and the values of Tdta and peak area were determined with the base line leveled. The peak area was calculated as the product of output voltages ( V) times temperature (0 C) and, by multiplying the resulting peak area by the apparatus constant, Qdta(2) was determined. [Pg.81]

The experimental apparatus developed for citrus oil processing is shown in Figure 4. The empty column was equipped before the adsorption column in order to dissolve the raw oil completely in SC-C02 and to avoid the adsorption of waxes and pigments, where they were removed easily due to the small solubility in SC-C02. A pair of 0.5 m long and 9 mm i.d. columns packed with silica gel were used for adsorber. [Pg.305]


See other pages where Apparatus development is mentioned: [Pg.366]    [Pg.14]    [Pg.154]    [Pg.284]    [Pg.350]    [Pg.149]    [Pg.298]    [Pg.351]    [Pg.10]    [Pg.368]    [Pg.81]    [Pg.189]    [Pg.341]    [Pg.225]    [Pg.490]    [Pg.555]    [Pg.119]    [Pg.93]    [Pg.327]    [Pg.338]    [Pg.235]    [Pg.43]   


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