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Schematic experimental system

Figure 1. Key elements of the TAP reactor (A) and high pressure fixed bed reactor (B) experimental systems. The TAP reactor schematic shows the heated valve manifold and reactor with the elevated pressure attachment located in the main high vacuum chamber. The fixed bed reactor shows the feed system, liquid vaporizer, oxygen disperser, reactor, and waste recovery system. Figure 1. Key elements of the TAP reactor (A) and high pressure fixed bed reactor (B) experimental systems. The TAP reactor schematic shows the heated valve manifold and reactor with the elevated pressure attachment located in the main high vacuum chamber. The fixed bed reactor shows the feed system, liquid vaporizer, oxygen disperser, reactor, and waste recovery system.
A schematic representation of the experimental system is shown in Figure 11.23. The modules comprising this system are discussed below. [Pg.361]

Figure 17. Experimental system for the measurement of surface pressure-molecular area (n-A) isotherms and the horizontal touch cyclic voltammetry/ and schematic representations for the control of permeabilities through oriented monolayers formed at low and high applied surface pressures. Figure 17. Experimental system for the measurement of surface pressure-molecular area (n-A) isotherms and the horizontal touch cyclic voltammetry/ and schematic representations for the control of permeabilities through oriented monolayers formed at low and high applied surface pressures.
Several experimental systems can be set up corresponding to different initial component distributions as schematically shown in Fig. 3 we shall confine our considerations to the transport arising from relaxation of the concentration gradients of only one or both solute components in a system. System A one of the components is initially present at uniform concentration throughout the system while the other component is maintained at a non-zero concentration gradient. This system has been a focus of major study in our laboratory and will be discussed in Section 3.3... [Pg.120]

Fiq. 13. Schematic diagram of experimental system used to study the adsorption of nitrogen on tungsten. [Pg.161]

Figure 4.9 Schematic of the experimental system (Zhang et al., 2007a). Figure 4.9 Schematic of the experimental system (Zhang et al., 2007a).
A schematic of the experimental system is shown in Fig. 1. One liter of culture liquid was added to a 2.8-L cylindrical glass column reactor, and 300 mL of cylindrical carrier was packed with rock wool. All of the tubing connections, stoppers, and seals in the column were made of butyl rubber. To prevent photodecomposition of vitamin B12, the outside of the whole device was covered with a vinyl sheet to shut out light. The digestion was carried out at 55°C and 20 d of hydraulic retention time (HRT). [Pg.1034]

The UMR process was studied in a pilot scale experimental system. A simplified schematic of the pilot scale system is shown in Figure 5. The pilot scale system consists of two packed bed reactors. The system was designed to produce 100 standard liters per minute of hydrogen, which is sufficient to generate 10 kW of electricity using a PEM fuel cell. [Pg.39]

Figure 12 Combination of dielectrophoretic field cage (DFC) and optical tweezers (OT) for the measurement of bead-cell adhesion (A) 4.1-(xm polystyrene particle trapped with laser tweezers (right) in contact with T-lymphoma cell ( — 1 5 pm in diameter). Cell and bead were brought into contact. The time for stable adhesion was measured. (B) Schematic representation of the experimental system used to measure the adhesion forces between bead and cell with the cell trapped in a DFC and the bead trapped in the laser focus of the OT. (C) Probing different surface regions of the cell for bead-cell adhesion (five beads are attached to a single cell). (Reprinted from Ref. 91 with permission.)... Figure 12 Combination of dielectrophoretic field cage (DFC) and optical tweezers (OT) for the measurement of bead-cell adhesion (A) 4.1-(xm polystyrene particle trapped with laser tweezers (right) in contact with T-lymphoma cell ( — 1 5 pm in diameter). Cell and bead were brought into contact. The time for stable adhesion was measured. (B) Schematic representation of the experimental system used to measure the adhesion forces between bead and cell with the cell trapped in a DFC and the bead trapped in the laser focus of the OT. (C) Probing different surface regions of the cell for bead-cell adhesion (five beads are attached to a single cell). (Reprinted from Ref. 91 with permission.)...
The experimental system has been described previously (1,2, 7,8) and is shown schematically in Figure 1. It consists of a 325-mesh stainless steel screen on which a thin layer of coal particles and a thermocouple are heated at rates of between 100° and 10,000°C/sec to temperatures as high as 1100°C, and held there for times up to 30 sec. The sample is contained within a pressure vacuum vessel of large volume such that the dispersion of evolving volatiles is great. Only the screen and sample are heated, and the volatiles are rapidly quenched as they mix with cold gas or condense on cold surfaces. [Pg.243]

Figure 1. Schematic diagram of experimental system 1- tank-separator, 2- pump, 3- working section. Figure 1. Schematic diagram of experimental system 1- tank-separator, 2- pump, 3- working section.
Fig. 9.6. Schematic diagram of the experimental system for laser ablation-assisted radio-frequency atomization excitation. (I) Sample holder, (2) tantalum lid, (3) graphite cup, (4) graphite disc, (5) rf power source, (6) different types of sample holder for sintered ceramics, (7) NdiYAG laser, (8) laser beam-focusing lens, (9) spectrometer, (10) quartz window for laser irradiation, (11) central electrode, (12) discharge chamber, (13) quartz window for optical observation. (Reproduced with permission of the Royal Society of Chemistry.)... Fig. 9.6. Schematic diagram of the experimental system for laser ablation-assisted radio-frequency atomization excitation. (I) Sample holder, (2) tantalum lid, (3) graphite cup, (4) graphite disc, (5) rf power source, (6) different types of sample holder for sintered ceramics, (7) NdiYAG laser, (8) laser beam-focusing lens, (9) spectrometer, (10) quartz window for laser irradiation, (11) central electrode, (12) discharge chamber, (13) quartz window for optical observation. (Reproduced with permission of the Royal Society of Chemistry.)...
Lasers have been used as a source of energy for pyrolysis, and several experimental systems were described in Section 4.5. The main use of lasers in mass spectral analysis is associated with several desorption techniques where the pyrolysis is an undesired process. However, laser pyrolysis is also used in direct coupling with an MS system, and a schematic diagram of a laser Py-MS system is shown in Figure 5.4.5. [Pg.151]

When a system has a positive Liapunov exponent, there is a time horizon beyond which prediction breaks down, as shown schematically in Figure 9.3.6. (See Lighthill 1986 fora nice discussion.) Suppose we measure the initial conditions of an experimental system very accurately. Of course, no measurement is perfect— there is always some error <5fl between our estimate and the true initial state. [Pg.322]

A schematic description of the experimental system is shown in Figure 1. The annular bed was formed by two concentric Poral type porous stainless steel tubes 0.60 meters long. The external tube O.D. was 50 mm with a wall thickness of 3 mm and limiting pore size of 35 microns. The internal tube O.D. was 20 mm with a wall thickness of 1 mm and limiting pore size of 20 microns. The concentric tubes were housed in a stainless steel tube of 75 mm O.D. The adsorption unit was immersed in an oil circulation thermostat,... [Pg.422]

Figure 7.3.4 Schematic experimental arrangement for tast polarography. Staircase voltammetry is carried out at a stationary electrode with the same system except the drop knocker. Figure 7.3.4 Schematic experimental arrangement for tast polarography. Staircase voltammetry is carried out at a stationary electrode with the same system except the drop knocker.
Schematic concentration profiles for the general case are shown in Figure 14.4.6. The limiting current with all of the processes contributing can be obtained only by numerical solution of the differential equations governing the system. However, in most experimental systems only one or two of the processes will be important. Which limiting case or subcase applies (i.e., which factors are rate-determining) is determined by the relative magnitudes of the characteristic currents, or more explicitly, by the ratios / // and ip/i, ... Schematic concentration profiles for the general case are shown in Figure 14.4.6. The limiting current with all of the processes contributing can be obtained only by numerical solution of the differential equations governing the system. However, in most experimental systems only one or two of the processes will be important. Which limiting case or subcase applies (i.e., which factors are rate-determining) is determined by the relative magnitudes of the characteristic currents, or more explicitly, by the ratios / // and ip/i, ...
Figure 4. A schematic diagram of the static experimental system. Figure 4. A schematic diagram of the static experimental system.
The catalytic wood gasification experiments were carried out in a 2.8-inch I.D. pressurized continuous reactor system. The experimental system is shown schematically in Figure I and consists of the following sections. [Pg.352]

Figure 6 shows a schematic diagram of the experimental system nsed for measnring m/n valnes for the... [Pg.199]


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Experimental schematic

Experimental system

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