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Lining For reference

Fig. 13.2 Vapor pressures (PV,T) and liquid molar volumes (Vm,T) along the orthobaric LV equilibrium line for reference isotopomer pairs, showing their distinctly different behaviors (schematic). The thicker lines label the heavier isotopomers. The curves begin at the triple points and end at the critical points (except for He which has no triple point under orthobaric conditions). Not to scale, isotopic differences are exaggerated (Reprinted from Van Hook, W. A., Rebelo, L. P. N. and Wolfsberg, M., Fluid Phase Equilib. 257, 35 (2007), copyright 2007, with permission from Elsevier)... Fig. 13.2 Vapor pressures (PV,T) and liquid molar volumes (Vm,T) along the orthobaric LV equilibrium line for reference isotopomer pairs, showing their distinctly different behaviors (schematic). The thicker lines label the heavier isotopomers. The curves begin at the triple points and end at the critical points (except for He which has no triple point under orthobaric conditions). Not to scale, isotopic differences are exaggerated (Reprinted from Van Hook, W. A., Rebelo, L. P. N. and Wolfsberg, M., Fluid Phase Equilib. 257, 35 (2007), copyright 2007, with permission from Elsevier)...
In this laboratory, you will construct a number line for reference electrode conversions, measure the corrosion potentials of several alloys in a salt water solution, construct a galvanic series with two different reference electrodes, and convert the two galvanic series to the NHE scale to determine if they agree (as they should). This lab will demonstrate some of the concepts discussed in Chapter 2. [Pg.361]

Figure 21 Maps of data from Heinrich layer H3. General geology and the Ruddiman (1977) IRD belt are shown, (a) Isopach map with 10 cm contour interval, (b) Sr/ Sr values for siliciclastic detritus in H3. Isopachs are shown in light dashed lines for reference, (c) 25-23 ka 250 mg cm kyr contours dehning the approximately E-W IRD belt (Ruddiman, 1977), contours of 10, 50, and 100 sand-sized ash shards per cm defining the approximately N-S trajectory of currents bringing Icelandic detritus into the North Atlantic (Ruddiman and Glover, 1982), and light... Figure 21 Maps of data from Heinrich layer H3. General geology and the Ruddiman (1977) IRD belt are shown, (a) Isopach map with 10 cm contour interval, (b) Sr/ Sr values for siliciclastic detritus in H3. Isopachs are shown in light dashed lines for reference, (c) 25-23 ka 250 mg cm kyr contours dehning the approximately E-W IRD belt (Ruddiman, 1977), contours of 10, 50, and 100 sand-sized ash shards per cm defining the approximately N-S trajectory of currents bringing Icelandic detritus into the North Atlantic (Ruddiman and Glover, 1982), and light...
Figure 2. (a) A double bend system with bends of the type shown in Fig. 1(a) connected by a waveguide of length =10a and (b) the frequency dependence of the corresponding transmission T (solid line). For reference, the transmission through a single bend is shown (dashed line). [Pg.62]

Figure 8 Spectra of ribonuclease as a function of temperature. Separations were performed as described in the legend to Fig. 7. The spectra at the temperatures for were 35, 50, 55, and 65 C, respectively, and are drawn with a solid line. For reference, the spectrum at 25 C is shown in each panel with a dotted line. Figure 8 Spectra of ribonuclease as a function of temperature. Separations were performed as described in the legend to Fig. 7. The spectra at the temperatures for were 35, 50, 55, and 65 C, respectively, and are drawn with a solid line. For reference, the spectrum at 25 C is shown in each panel with a dotted line.
Fig. 8.2 Snapshots of the squared wavepacket amplitude and Floquet quasienergy surface. Each panel shows the snapshot at the time point which is indicated at the right top. For each panel, the black solid line represent the squared amplitude of the dominant Floquet state, and the gray dashed curve does the corresponding quasienergy surface. Another closely related QES is also plotted with black dotted line for reference. Three panels in each vertical row show snapshots of the dynamics starting from the initial vibrational state and the peak field intensity indicated at the top. We also plotted approximate position of resonant points by gray arrow. The arrow in panel (a-1) shows the 3lo resonance point while that in panel (d-3) shows Itv resonance point. (Reprinted with permission from K. Hanasaki et al., Phys. Rev. A 88, 053426 (2013)). Fig. 8.2 Snapshots of the squared wavepacket amplitude and Floquet quasienergy surface. Each panel shows the snapshot at the time point which is indicated at the right top. For each panel, the black solid line represent the squared amplitude of the dominant Floquet state, and the gray dashed curve does the corresponding quasienergy surface. Another closely related QES is also plotted with black dotted line for reference. Three panels in each vertical row show snapshots of the dynamics starting from the initial vibrational state and the peak field intensity indicated at the top. We also plotted approximate position of resonant points by gray arrow. The arrow in panel (a-1) shows the 3lo resonance point while that in panel (d-3) shows Itv resonance point. (Reprinted with permission from K. Hanasaki et al., Phys. Rev. A 88, 053426 (2013)).
The drag coefficient Cq is then plotted against the equivalent Reynolds number Re to determine the terminal velocity. On a logarithmic scale, Cfq and Cg are superposed as straight lines for reference (Figure 3-7). [Pg.133]

Figure 5.6 Morphology-induced dependence of the crystallization temperature (Tf) of the EO block on total polybutadiene (PB) concentration in binary blends of a polybutadiene homopolymer and a B-EO diblock copol5uner. Data obtained from a poly(ethylene oxide) homopolymer are included (dashed line) for reference. (Reprinted with permission from Chen, H.-L., Hsiao, S.-C., Lin, T.-L., Yamauchi, K., Hasegawa, H. and Hashimoto, T. Macromolecules 34 671, (2001). Copyright 2001 American Chemical Society.)... Figure 5.6 Morphology-induced dependence of the crystallization temperature (Tf) of the EO block on total polybutadiene (PB) concentration in binary blends of a polybutadiene homopolymer and a B-EO diblock copol5uner. Data obtained from a poly(ethylene oxide) homopolymer are included (dashed line) for reference. (Reprinted with permission from Chen, H.-L., Hsiao, S.-C., Lin, T.-L., Yamauchi, K., Hasegawa, H. and Hashimoto, T. Macromolecules 34 671, (2001). Copyright 2001 American Chemical Society.)...
Figure C2.17.10. Optical absorjDtion spectra of nanocrystalline CdSe. The spectra of several different samples in the visible and near-UV are measured at low temperature, to minimize the effects of line broadening from lattice vibrations. In these samples, grown as described in [84], the lowest exciton state shifts dramatically to higher energy with decreasing particle size. Higher-lying exciton states are also visible in several of these spectra. For reference, the band gap of bulk CdSe is 1.85 eV. Figure C2.17.10. Optical absorjDtion spectra of nanocrystalline CdSe. The spectra of several different samples in the visible and near-UV are measured at low temperature, to minimize the effects of line broadening from lattice vibrations. In these samples, grown as described in [84], the lowest exciton state shifts dramatically to higher energy with decreasing particle size. Higher-lying exciton states are also visible in several of these spectra. For reference, the band gap of bulk CdSe is 1.85 eV.
NOTE. It is not expected that a student xvill attempt to memorise all the colour tests given in Part III. He might for example be expected to know the Phthalein Reaction for phenol itself (p. 339). Details of the divergence from the standard result are recorded primarily for reference, so that a student will not be diverted from his line of investigation if he observes that a suspected phenol does not respond exactly to the standard colour changes. [Pg.319]

A typical arrangement for a voltammetric electrochemical cell is shown in Figure 11.28. Besides the working, reference, and auxiliary electrodes, the cell also includes a N2 purge line for removing dissolved O2 and an optional stir bar. Electrochemical cells are available in a variety of sizes, allowing for the analysis of solution volumes ranging from more than 100 mL to as small as 50 )+L. [Pg.510]

Extensive design and optimization studies have been carried out for this sequence (108). The principal optimization variables, ie, the design variables that have the largest impact on the economics of the process, are the redux ratio in the azeo-column the position of the tie-line for the mixture in the decanter, determined by the temperature and overall composition of the mixture in the decanter the position of the decanter composition on the decanter tie-line (see Reference 104 for a discussion of the importance of these variables) and the distillate composition from the entrainer recovery column. [Pg.196]

For apphcation to distiUation (a nearly isobaric process), as shown in Figs. 13-8 to 13-13, binary-mixture data are frequently plotted, for a fixed pressure, as y versus x, with a line of 45° slope included for reference, and as T versus y and x. In most binary systems, one of the components is more volatile than the other over the entire composition range. This is the case in Figs. 13-8 and 13-9 for the benzene-toluene system at pressures of both 101.3 and 202.6 kPa (1 and 2 atm), where benzene is more volatile than toluene. [Pg.1248]

Fig. 19-4. Vertical expansion of continuous plumes related to vertical temperature structure, The dashed lines correspond to the dry adiabatic lapse rate for reference. Fig. 19-4. Vertical expansion of continuous plumes related to vertical temperature structure, The dashed lines correspond to the dry adiabatic lapse rate for reference.
Step 4. A straight line between the point on the reference line 2 and the point on the pressure line for 1 atmosphere absolute will cross the line for gas dissolved at 1,500 parts per million by weight. [Pg.366]

Another variation is to use a pyramid-shaped tank at grade level with an inclined dewatering screw feeder. Refer to Figure 38 for an example. Tank materials are usually constructed from carbons steel, stainless steel, stainless clad, resin or epoxy-lined for those situations where iron contamination in the product is a concern, or if corrosion by the adsorbate in the carbon is possible. [Pg.312]

Solution We ll construct the Z-matrix for the RR form first. We ll use the Cl-C-C-Cl plane as our major reference. Here are the lines for the carbons and chlorines ... [Pg.291]

All the alkali metals have characteristic flame colorations due to the ready excitation of the outermost electron, and this is the basis of their analytical determination by flame photometry or atomic absorption spectroscopy. The colours and principal emission (or absorption) wavelengths, X, are given below but it should be noted that these lines do not all refer to the same transition for example, the Na D-line doublet at 589.0, 589.6 nm arises from the 3s — 3p transition in Na atoms formed by reduction of Na+ in the flame, whereas the red line for lithium is associated with the short-lived species LiOH. [Pg.75]

Fig. 2. Geometries calculated (solid lines) and observed (bold dashed lines) for 1-propanol in its a-cyclodextrin adduct. G3 and G6 denote the numbers of glucopyranose units of a-cyclodextrin. H3 and H5 refer to the hydrogen atoms located inside of the cyclodextrin cavity. The hydrogen atoms for the observed geometry of 1-propanol are not shown, since their atomic coordinates have not been determined. The observed 1-propanol is twofold disordered, with site a occupied 80%, site b 20%. Interatomic distances are shown in bold italics on fine dashed lines (nm). Reproduced with permission from the Chemical Society of Japan... Fig. 2. Geometries calculated (solid lines) and observed (bold dashed lines) for 1-propanol in its a-cyclodextrin adduct. G3 and G6 denote the numbers of glucopyranose units of a-cyclodextrin. H3 and H5 refer to the hydrogen atoms located inside of the cyclodextrin cavity. The hydrogen atoms for the observed geometry of 1-propanol are not shown, since their atomic coordinates have not been determined. The observed 1-propanol is twofold disordered, with site a occupied 80%, site b 20%. Interatomic distances are shown in bold italics on fine dashed lines (nm). Reproduced with permission from the Chemical Society of Japan...
Processing line downtime Refers to equipment that cannot be operate when it should be operating. Reason for downtime could be equipment being inoperative, shortage of material, electric power problem, operators not available, and so on. Regardless of reason, downtime is costly. [Pg.641]

The (vapor + liquid) equilibrium line for a substance ends abruptly at a point called the critical point. The critical point is a unique feature of (vapor + liquid) equilibrium where a number of interesting phenomena occur, and it deserves a detailed description. The temperature, pressure, and volume at this point are referred to as the critical temperature, Tc. critical pressure, pc, and critical volume, Vc, respectively. For COi, the critical point is point a in Figure 8.1. As we will see shortly, properties of the critical state make it difficult to study experimentally. [Pg.392]


See other pages where Lining For reference is mentioned: [Pg.1604]    [Pg.25]    [Pg.39]    [Pg.253]    [Pg.137]    [Pg.1604]    [Pg.25]    [Pg.39]    [Pg.253]    [Pg.137]    [Pg.102]    [Pg.117]    [Pg.73]    [Pg.309]    [Pg.409]    [Pg.81]    [Pg.240]    [Pg.124]    [Pg.358]    [Pg.391]    [Pg.265]    [Pg.175]    [Pg.177]    [Pg.369]    [Pg.147]    [Pg.120]    [Pg.134]    [Pg.15]    [Pg.33]    [Pg.185]    [Pg.120]    [Pg.134]    [Pg.227]   


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