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Starting Situation

These crematoria are entirely comparable in size, equipment, and manner of construction to other similar installations built in the Third Reich at that time, as well as with those built today.176 In this connec- [Pg.88]

Answer As supervising engineer, I inspected the Huta Corporation and dealt with the Zentralhauleitung of the SS. I also audited the invoices of our firm. [Pg.89]

One could walk everywhere without hindrance on the streets of the camp and was only stopped by the guards upon entering and leaving the camp. [Pg.89]

But lines of inmates in a relatively poor general condition could be seen on the streets of the camp. [Pg.89]

Among other things, crematoria II and III with the large morgues. [Pg.89]


Several studies have been performed to investigate the compatibalizing effect of blockcopolymers [67,158, 188,196-200], It is generally shown that the diblock copolymer concentration is enhanced at the interface between incompatible components when suitable materials are chosen. Micell formation and extremely slow kinetics make these studies difficult and specific non-equilibrium starting situations are sometimes used. Diblock copolymers are tethered to the interface and this aspect is reviewed in another article in this book [14]. [Pg.391]

The starting situation is partially defined by the state of the following valves ... [Pg.82]

Fig. 4.10. The left side of the scheme represents the starting situation of pure Zeeman splitting, as described by (4.48) and shown before in Fig. 4.9. In this example, the field B = (0,0,B), which defines the quantization axis, is chosen as the z-direction. The additional quadrupole interaction, as shown on the right side of Fig. 4.10, leads to a pair-wise shift of the Zeeman states with mj = 3/2 and mi = 1/2 up- and down-wards in opposite sense. In first order, all lines are shifted by the same energy as expected from the m/-dependence of the electric... Fig. 4.10. The left side of the scheme represents the starting situation of pure Zeeman splitting, as described by (4.48) and shown before in Fig. 4.9. In this example, the field B = (0,0,B), which defines the quantization axis, is chosen as the z-direction. The additional quadrupole interaction, as shown on the right side of Fig. 4.10, leads to a pair-wise shift of the Zeeman states with mj = 3/2 and mi = 1/2 up- and down-wards in opposite sense. In first order, all lines are shifted by the same energy as expected from the m/-dependence of the electric...
For this purpose, the starting situation in this section is reflected by Equation9.1 and, depending on the results obtained, will show whether this equation is still valid and, if so, under which conditions. Possible differences in results between those described in this section and those in section9.2 need to be explained by the fact that a textile structure is used as electrode material, since this is the only modification of the electrochemical cell characterised in section9.2 and used for the studies described here in section... [Pg.255]

We assume that the time resolution of the STM-measurements is sufficient to discriminate the effect of the entire random walk of one individual vacancy from that of the next, which was already shown to be the case in Section 2.2. The starting situation is shown in Fig. 13. A tracer atom is embedded in the origin of a square lattice with a vacancy sitting next to it at (1, 0). We assume that the only diffusion barrier that is modified by the tracer atom is that for vacancy-tracer exchange. [Pg.365]

Figure 13 The random walk starting situation, with the vacancy directly next to the tracer atom. The probabilities x, y and pKC are introduced in the text. Figure 13 The random walk starting situation, with the vacancy directly next to the tracer atom. The probabilities x, y and pKC are introduced in the text.
Therefore, another idea is the synthesis of amphiphilic systems via radical polymerization using a two-phase or heterophase starting situation. In principle, these techniques allow the kinetic control of the copolymer structures or monomer sequence of the polymer chain. The final polymer chain is not only defined by the... [Pg.47]

The solid-phase method allows application of the samples, which are soluble in a nonvolatile solvent only. In this case, the sample must be dissolved in a suitable solvent and mixed with 5-10 times its weight of a deactivated adsorbent. The mixture will be carefully dried by rotary evaporation and will then be introduced into the layer that must be specifically prepared to accept it. For this reason, Botz et al. created a device that enables regular sample application in the entire cross section of the preparative layer with the advantage of in situ sample concentration and cleanup. With this device, the sample can be applied to improve the starting situation for a preparative chromatographic separation, independent of the migration of whether the mobile phase is achieved by capillary action or by forced flow. [Pg.1390]

After completion of the exchange procedures, the two phases, which now exhibit different concentrations to the starting situation, are separated. Combined with the phase separation is a partial separation of the homogeneous mixture. [Pg.9]

Figure 3.8 The two worksheets in the spreadsheet, fig3-8.xls, for the calculation of the orthonormal double-zeta Slater radial function of the lithium 2s orbital. The comparison graphs in this figure show the possible starting situation, with both C coefficients equal 1 and the C2 equal 0. In both cases, changing the value of cj in cell SCSI 1 leads to the best fit results shown in the next diagram. Figure 3.8 The two worksheets in the spreadsheet, fig3-8.xls, for the calculation of the orthonormal double-zeta Slater radial function of the lithium 2s orbital. The comparison graphs in this figure show the possible starting situation, with both C coefficients equal 1 and the C2 equal 0. In both cases, changing the value of cj in cell SCSI 1 leads to the best fit results shown in the next diagram.
This sub-section develops a simple graphical method for quickly estimating volt-drops for direct-on-line starting situations. The following data forms the basis of the graphical results ... [Pg.580]

The AE measurement began with only eight AE sensors (Numbers SE20 to SE27 of Fig. 11.10) located in the southern part of the test site. At this time no mining activity was going on at the test site. Thus the starting situation could be monitored in a time period of approximately 4 months. [Pg.258]

The starting situation (reaction out of equilibrium) is given for a chanical potential p corresponding to initial qnantities of A and B. The final situation corresponds to a null chemical potential (equality of chemical potentials of the poles) that is, it corresponds to the eqnilibrium of the dipole (i.e., energy extremum). [Pg.161]

Current production situation should always be considered—every optimization builds on top of a starting situation. [Pg.12]


See other pages where Starting Situation is mentioned: [Pg.359]    [Pg.392]    [Pg.394]    [Pg.210]    [Pg.202]    [Pg.47]    [Pg.53]    [Pg.22]    [Pg.57]    [Pg.201]    [Pg.88]    [Pg.262]    [Pg.366]    [Pg.192]    [Pg.431]    [Pg.213]    [Pg.206]    [Pg.396]    [Pg.409]    [Pg.413]    [Pg.277]    [Pg.122]    [Pg.298]    [Pg.302]    [Pg.22]    [Pg.360]    [Pg.61]    [Pg.479]    [Pg.190]    [Pg.272]    [Pg.276]    [Pg.313]    [Pg.190]    [Pg.783]   


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Situation

Situational

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