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Capillary slit cells

Figure II.6.6 shows two possible designs of capillary slit cells. The second type of cell has the added advantage of being suitable also for in situ ESR spectroelec-trochemical experiments. Capillary slit cells permit fast electrochemical conversion... Figure II.6.6 shows two possible designs of capillary slit cells. The second type of cell has the added advantage of being suitable also for in situ ESR spectroelec-trochemical experiments. Capillary slit cells permit fast electrochemical conversion...
Unfortunately, even when capillary slit cells are used in the experiment, the spectra of the different species are still superimposed. Therefore, it is necessary to separate or to deconvolute the superimposed spectra in order to obtain information about the reaction kinetics of individual species. In the literature, techniques have been proposed for the deconvolution of the superimposed spectra [68, 69]. Data processing and deconvolution may be achieved with spreadsheet software on a suitable computer system. As soon as the time dependence of the concentration of each component is known, the absorbance-time curves and the charge-time curves calculated from the current passing the electrode can be used to determine rate or equilibrium constants for the chemical system under smdy. [Pg.192]

Figure II.6.6 shows two possible designs of capillary slit cells. The second type of cell has the added advantage of being suitable also for in situ ESR spectro-electrochemical experiments. Capillary slit cells permit fast electrochemical conversion of the starting material into unstable radical intermediates, which may be followed in time during follow-up chemical reaction steps. The thickness of the capillary slit, together with the diffusion coefficient D of the reactant, determine the approximate conversion time raiffusion (Eq. II.6.5). Figure II.6.6 shows two possible designs of capillary slit cells. The second type of cell has the added advantage of being suitable also for in situ ESR spectro-electrochemical experiments. Capillary slit cells permit fast electrochemical conversion of the starting material into unstable radical intermediates, which may be followed in time during follow-up chemical reaction steps. The thickness of the capillary slit, together with the diffusion coefficient D of the reactant, determine the approximate conversion time raiffusion (Eq. II.6.5).
In the glomerular capillaries, a portion of the plasma water is forced through a filter that has three basic components fenestrated capillary endothelial cells, a basement membrane lying just beneath the endothelial cells, and the filtration slit diaphragms formed by the epithelial cells that cover the basement membrane on its urinary space side. Solutes of small size flow with filtered water (solvent drag) into the urinary (Bowman s) space, whereas formed elements and macromolecules are retained by the filtration barrier. [Pg.477]

Fig. II.6.9 In situ UV/Vis/NIR spectroelectrochemical long path length cell based on a nontransparent band electrode in a capillary slit and a light beam focused through the diffusion layer... Fig. II.6.9 In situ UV/Vis/NIR spectroelectrochemical long path length cell based on a nontransparent band electrode in a capillary slit and a light beam focused through the diffusion layer...
Fig. 11.6.6 a, b. Capillary slit in situ UV/Vis/NIR spectroelectrochemical cells with an optically transparent electrode prepared from a metal mesh, grid or gauze in a left cuvette cell and in a right flat cell with outlet allowing the solution to flow through the slit... [Pg.180]

In l02) the authors describe the design of an experimental plant for studies of acoustic cavitation in flowable high polymers with the help of optic methods the plant employs a flat-slit transprent-wall capillary acoustic treatment of a polymer was carried out at a frequency of 17.8 kHz, and amplitude of vibration between 0 and 15 mcm. The study was conducted on 1,2 polybutadienes of narrow molecular-mass distribution tests were arranged at room temperature. It has been demonstrated that static mechanical stresses occur in a stationary (non-flowing) polymer under the action of acoustic treatment isochrome lines in the viscosimetric tank form a cellular structure with cell size of about 1-3 mm, and in the capillary the isochromes are observed in form of longitudinal strips (Fig. 19). The authors have also found that acoustic... [Pg.73]

In order to get a Raman spectrum, a sample is located in the sample cell. Then, a laser light is focused on the sample using a lens. Usually, the sample cell is a capillary tube, normally made of Pyrex glass, where liquids and solids are sampled in [57], Or another appropriate sample holder system where is given the possibility that the light scattered during its interaction with the sample is accumulated using an additional lens and is then focused at the entry slit of the monochromator [32,62],... [Pg.167]

Capillary structure Capillary structure varies widely in terms of the fraction of the basement membrane that is exposed by slit (tight) junctions between endothelial cells. In the brain, the capillary structure is continuous, and there are no slit junctions (Figure 1.8). This contrasts with the liver and spleen, where a large part of the basement membrane is exposed due to large discontinuous capillaries, through which large plasma proteins can pass. [Pg.19]

Q1 The glomerulus is a ball of capillaries which is part of the renal corpuscle the other portion of this structure is Bowman s capsule, which forms the start of the nephron. The wall of Bowman s capsule is composed of a layer of specialized epithelial cells with extensions or foot processes which are in contact with the glomerulus and are called podocytes. The gaps between the foot processes are known as slit pores. These pores allow small molecules to pass through the epithelial layer into the nephron tubules. Below the epithelium is a basement membrane which prevents the passage of large proteins and whole cells into the renal tubules. [Pg.227]

The detector time constant and detector cell volume are both involved. The slit width along the length of S the capillary is proportional to the latter. A value of ... [Pg.209]

Fig. 18. Schematic diagram of the optical arrangement for single-crystal work. A, tungsten lamp B1 and B2, Polaroids C, focusing lens, D, light-collection lens E, capillary cell showing lens (1), solid phase (ice, s), liquid phase (solution, w), interface (i), and laser beam (b) F, filler tube G, monochromator slits and H, analyzer. Coordinate system is as indicated. Cold air flow is along the X direction. From Tomimatsu et al. (1976), reproduced with permission. Fig. 18. Schematic diagram of the optical arrangement for single-crystal work. A, tungsten lamp B1 and B2, Polaroids C, focusing lens, D, light-collection lens E, capillary cell showing lens (1), solid phase (ice, s), liquid phase (solution, w), interface (i), and laser beam (b) F, filler tube G, monochromator slits and H, analyzer. Coordinate system is as indicated. Cold air flow is along the X direction. From Tomimatsu et al. (1976), reproduced with permission.
Fig. 1-6. A sketch illustrating liquid-vapor interfacial configurations during transition Imm adsorption to capillary-dominated imbibition in the proposed unit cell () spontaneous slit fill up (capillary condensation), (c) pore snap-off, and < /) full unit cell. Fig. 1-6. A sketch illustrating liquid-vapor interfacial configurations during transition Imm adsorption to capillary-dominated imbibition in the proposed unit cell (</) liquid films adsorbed on pore and slit walls and liquid held in corners due to capillary forces at low matric potentials, (/>) spontaneous slit fill up (capillary condensation), (c) pore snap-off, and < /) full unit cell.
Fig. 1. Raman spectra of four waters, HjO, H2 0, D2O, and Di left) as ice at 77 K with a liquid N2 cell (see Fig. 6), 135° backscattering directly off the ice surface, laser power 250 mW, spectral slit width 6 cm and right) as neat liquid at room temperature with a capillary tube, 90° scattering, laser power 250 mW, spectral slit width 10 cm". Exciting radiation (488.0 nm) for all RR spectra was provided by a Coherent Innova 90-6 Ar ion laser. The scattered light was dispersed by a SPEX 1403 double monochromator equipped with 1800 grooves/mm holographic gratings and detected by a cooled Hamamatsu 928 photomultiplier tube under the control of a SPEX DM3000 data station as described elsewhere. ... Fig. 1. Raman spectra of four waters, HjO, H2 0, D2O, and Di left) as ice at 77 K with a liquid N2 cell (see Fig. 6), 135° backscattering directly off the ice surface, laser power 250 mW, spectral slit width 6 cm and right) as neat liquid at room temperature with a capillary tube, 90° scattering, laser power 250 mW, spectral slit width 10 cm". Exciting radiation (488.0 nm) for all RR spectra was provided by a Coherent Innova 90-6 Ar ion laser. The scattered light was dispersed by a SPEX 1403 double monochromator equipped with 1800 grooves/mm holographic gratings and detected by a cooled Hamamatsu 928 photomultiplier tube under the control of a SPEX DM3000 data station as described elsewhere. ...

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See also in sourсe #XX -- [ Pg.189 , Pg.190 , Pg.192 ]




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