Modeling of CollisionsEditions Scientifiques et Medicales Elsevier, 1998 - 222 من الصفحات |
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الصفحة 88
... 1.283 1.312 1.334 1.377 1.414 1.455 Yo 9.067 9.673 10.13 10.50 11.23 11.90 12.67 Table I. Transport coefficients as functions of Z. Note that we recover , in the case useful for 888 8 Numerical computations Numerical results.
... 1.283 1.312 1.334 1.377 1.414 1.455 Yo 9.067 9.673 10.13 10.50 11.23 11.90 12.67 Table I. Transport coefficients as functions of Z. Note that we recover , in the case useful for 888 8 Numerical computations Numerical results.
الصفحة 96
... Note that the magnetic field source term ( essentially VT - Vne ) does not exist in one - dimensional geometries . Orders of magnitude and limitations Orders of magnitude ( in a loose meaning ) of sections 2.3 and 3.3 are well verified ...
... Note that the magnetic field source term ( essentially VT - Vne ) does not exist in one - dimensional geometries . Orders of magnitude and limitations Orders of magnitude ( in a loose meaning ) of sections 2.3 and 3.3 are well verified ...
الصفحة 131
... , kz Te T Once again , the number of electrons in a Debye sphere must be large in a classical plasma : ND 4π ne 3 1 ( note that this condition is more restrictive than the B Plasma frequency is the largest 131 Wp » B 2 B 3.
... , kz Te T Once again , the number of electrons in a Debye sphere must be large in a classical plasma : ND 4π ne 3 1 ( note that this condition is more restrictive than the B Plasma frequency is the largest 131 Wp » B 2 B 3.
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