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For more detailed training evaluation, a quantitative risk assessment based on the calculated gas amounts from the model or additional calculations for fire and explosion effects is now in progress.
Calculated and experimental (by PIV-measurements) obtained velocity vector maps, as well as measured and calculated gas phase pressure fluctuations over the entire bed are compared.
Shown are calculated gas temperatures and velocities at 190 km for equinox solar cycle minimum conditions.
If calculated gas volume is different from assumed volume in Step 5, repeat Steps 5 through 8 until a converged volume is obtained.
Theoretically calculated gas compositions-are given in figures 2.4 to 2.6.
The calculated gas core positions match the ECVT images well.
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A nanometer-thick film of TiO2 is formed on the PEDOT PSS surface and forms an adhesion layer to bond phosphonic acids to the polymer; the work function of the PEDOT PSS (ΦPEDOT PSS) is adjusted by choice of phosphonic acid over a range of approximately 0.8 eV, and ΔΦPEDOT PSS correlates strongly with the calculated gas-phase dipole moments of the phosphonates.
The calculated gas-phase relative basicity of the six dianions follows the order SQ2− > 4-CDCB2− > 2,4-CDCB2− > 3,4-CDCB2− > 2,3,4-CDCB2− 2,3,4-CDCB2−CB2− which support the experimental results that the dianions SQ2− and 4-CDCB2− can be protonated, in strongly acidic medium, to the corresponding monoanions, whereas no protonation occurs in the case of di-, tri- and tetra-substituted compounds.
In Table 4 we present calculated gas-phase energetics for the Cu+ family and Zn2+ family complexes of SbS SH)(OH)-.
To establish the protonation state expected for the polysulfides and As and Sb sulfides in the solutions of interest, we employ the procedure of ref. 9, in which we calculated gas-phase deprotonation energies at the polarized SBK MP2 level, and hydration energies at the 6-31G* HF level using COSMO.
Since the 1ATC9 molecules within the tilt domains are identical, and since their calculated gas-phase polarizabilities change very little when normal to the surface or tilted, we posit that the difference in the polarizabilities between the tilt domains is due to differences in the bonding at the molecule−surface interface.
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