Exact(11)
Again, all experiments at 850 900 °C are clustered at Mg/(Mg + Fe) 0.8 0.9 in the variety of experimental charge setup.
The simple avalanche multiplication model can reproduce the experimental charge spectra reasonably well at the beginning of the high-voltage plateau region.
There were several attempts to obtain molecular (hyper polarizabilities from electric moments using experimental charge density studies of materials with potential non-linear optical properties and therefore to predict the size of the NLO effect.
Current trends in crystal engineering are critically discussed based on experimental charge density analysis for quantifying various interatomic interactions, from weak van der Waals to coordinate bonds, as applied to the design of crystalline materials.
Nevertheless, for cubic NaCl particles in the same charging conditions (i.e. ion density and transit time), the experimental charge level appears to be greater than predicted by classical field charging law.
Despite the differences in the bulk composition of the experimental charge, due to the different proportions in carbonates, silicates, and volatile sources, we obtained identical Mg/(Mg + Fe) ratio in clinopyroxenes of the three experimental setups at 4.2 GPa, 900 °C, in "forward" and sandwich experiments.
Similar(49)
The results of the semi-analytical model are verified against those of full model and validated with experimental charge-discharge curves.
Experimental charging data of numerous weak polyelectrolytes are discussed in terms of these models in detail.
The experimental charging discharging voltage signal (ECDVS) is applied as source data for the WMULDEN based analysis.
After each run and quenching of the products, experimental charges were weighed to measure volatile loss and were punctured to verify the presence of liquid H2O.
Moreover, most, although not all, characterizations of experimental charges were carried out on fluids after returning the sample to ambient temperature and pressure.
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