Research Article

Gravitational Instability of Rotating Viscoelastic Partially Ionized Plasma in the Presence of an Oblique Magnetic Field and Hall Current

Figure 2

Variation of ๐‘Š , given by (14), with the wavenumber for different values of viscoelasticity ๐œ‡ ๎…ž when ๐œ‚ = 1 mHโ€‰cmโˆ’1, ๐œ‡ = 0 . 1 โ€‰gmโ€‰cmโˆ’1โ€‰secโˆ’1, ๐‘ฃ ๐‘ = 0 . 1 โ€‰secโˆ’1, ฮฉ = 0 . 0 5 โ€‰radโ€‰secโˆ’1, ๐ป ๐‘ง = 0 . 1 โ€‰Ampโ€‰cmโˆ’1, ๐œŒ ๐‘‘ = 0 . 0 0 1 โ€‰gmโ€‰cmโˆ’3, ๐ฟ = 0 . 1 cm2โ€‰secโˆ’1, and ๐œƒ = 0 โˆ˜ .
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