GTA SA NFS Carbon Mod 2010 V 2.00.epub
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c1 and c2 are both almost independent of c content in 20 at.% c-alloyed -tial. this hints towards a constancy of the cohesive energy of the single phases. in this context, it is interesting to compare our results with the work of matarand and co-workers [ 22 ], who also found c1 constancy. however, they also report large fluctuations of c2 (a positive c2 at 0 k, then a negative c2 at 500 k). in contrast, our results suggest a trend of increasing c1 and constancy of c2 with c content (figure 6). within the pure single phase the variation of c1 and c2 is hardly detectable.
the elastic anisotropy describes a material's ability to withstand load in a specific direction and has therefore profound impact on the material's mechanical behaviour. this is of particular interest for alloys, which at certain concentrations have a very distinct alignment of the principal stresses resulting in failure via uniaxial tension along these directions [ 54, 55, 56 ]. the conventional definition of the anisotropy coefficient is the ratio of the change of the elastic constants c11, c12, c33, c44, and c66 compared to their maximum value (table 2 ). since the c11 and c12 remain approximately the same, it is, in principle, possible to define a new anisotropy coefficient k, which describes a material's ability to withstand load in its diagonal direction parallel to the cubic axes. in other words, the obtained values of c44 and c66 are still considerably smaller than the c11, c33, and c12. as the main reason for the discrepancy between the c11 - c66 values, the presence of carbon atoms disturbs the layers and favors the formation of the cubic tial phase. the most evident effect is the shift and rotation of one (or more) ti layer(s) along the cubic axes to create space for carbon atoms. at around 3 at.% c, c44 is reduced by 2.8%, while c11, c66, c11, and c33 change by a factor of 1.3, 1.8, 3.5, and 2.3 respectively. d8a7b2ff72
Numeric modeling was used to assess the translocation of carbon black particles from the initial instillation site (main bronchus) to the lung periphery. Once inhaled, CBNPs translocate to the lung periphery on the basis of size and physiochemical properties of the particles [ 32, 34 ]. The model identified a rapid transition of the particle size distribution, with smaller particles within the first hour of the instillation. The smallest particles were predicted to remain at the initial instillation site for the duration of the 6-month exposure. The average particle diameter in the alveoli/bronchial region decreased over time, most rapidly by the first week after the dose (Figure S1), indicating clearance of the particles from the lung.
This R package can also be used to model the carbon flow to other regions of fisheries important in international context and to the problem areas mentioned above. Any issues that arise during data extraction and preparation, for example the linearisation of data using the pointInRegion command from the spatialEco package, can be reported to the user and fixed.
These datasets are distributed as a binary in CRAN (using the file RData/NFS.carbon.flow.data.rdata. RData/NFS.carbon.flow.data.rdata.csv) and also as a PDF as supplementary data (NFS.carbon.flow.data.pdf).
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