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The predictions closely mimic the observed evolution in charged particle size distributions and reproduce the experimentally observed Boltzmann charge distributions.
This means that such electric quantities as current, voltage, and charge distributions are not affected by the passage of time.
The charge distributions increased in water.
Inset shows surface charge distributions corresponding to each peak.
Insets shows surface charge distributions for ∆y = 14 nm.
For the organic molecules charge distributions were calculated using the Electronegativity Equalization Method (EEM[13]).
Table 2 shows the charge distributions and shielding parameters used for the mineral phases.
These categories and sub-categories are different for the three charge distributions.
In Fig. 8 the measured charge distributions for 510 nm and 990 nm particles are shown.
Conversely the two systems with different charge distributions behave differently at low temperature.
They enable us to visualize the charge distributions of molecules and charge-related properties of molecules.
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