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Fig. 1 Applied sheath model.
We applied an analytical formula of the sheath capacitance with a step sheath model.
We applied a simple sheath model as illustrated in Fig. 1.
The electron temperature is therefore deduced from the observed sheath capacitance if the applied sheath model is valid.
We describe the potential profile corresponding to (1) in the matrix sheath model developed by Matsuoka et al. (2012).
To explain the phenomena observed in this study, pulsed plasma sheath model was used to simulate the ion sheath dynamics.
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All measurements were made using our previously developed and validated optic nerve sheath models [16, 18] with varying sheath diameters of known size (simulated from 3-D printediscscs), and conducted by expert point-of-care ultrasonographers (LG and GH).
These measurements can be used in support of RF sheath modeling that is an important part of the optimization of antenna design for next generation fusion energy devices, including ITER.
The CEA activity to this antenna design within the CYCLE consortium was focused on the Faraday screen design (Fig. 1) and associated radio frequency (RF) sheath modelling, the reflectometers design for edge density measurement in the antenna vicinity and a contribution to the remote handling/tooling of the antenna.
2, a plasma-sheath model is introduced using the fluid equations for positive ions and Boltzmann distribution for negative species and the initial boundary conditions are introduced.
With the sampling system at a negative potential with respect to the burner, the flame conforms to a sheath-convection model, so that convection to a sheath of positive ions covering the sampling nozzle dominates, while electrons are repelled.
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