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The former would optimize the inactive part (charge time) of a cycle for a given charging condition, while the latter would optimize the active part (draw time) for a given hardware configuration (i.e., capacitor size).
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Tumour destruction for a given charge was significantly greater following anodic than cathodic treatment.
The solution to the Poisson equation for a given charge density reads (6) Φ (r → ) = 1 4 π ∈ 0 ∈ ∫ ρ (r → ) | r → | d V (r → ).
The lowest energy 2D structures identified for B12H6 and B12F6 were used as initial structures for the structural optimization at a given charge state.
Each cycle consisted of three phases: (I) a linear increasing ramp from 20 to 50 V, at a rate of 0.5 V/s, (II) an interval at 50 V for certain time duration to flow a given charge Q0 through the system, and (III) a subsequent linear decreasing ramp from 50 to 20 V at 0.1 V/s.
The presence of salt during complex formation induces a smaller complexation efficiency for each given charge ratio.
Knowing that the presence of salt induces a smaller complexation efficiency for each given charge ratio, as quantified in our work, we can justify that apparent "distance increase" (inferred by a decrease on energy transfer efficiency) with the presence of free DNA, containing isolated donors.
PPy/p20 surfaces consistently demonstrate the lowest impedance and largest charge capacity for a given deposition charge.
The tensile strength of CFRP after anodic polarization decreases with increasing circulated charge, and, for a given circulated charge, it increases with increasing [Cl−].
Metastable defects occur when at least two different atomic arrangements are possible for a given defect charge state.
This work elucidates the key parameters that are needed for emittance preservation, such as the required field and aspect ratio for a given bunch charge.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com