Research Article

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

Figure 5

Variation of ๐‘Š , given by (14), with the wavenumber for different values of magnetic field in ๐‘ง direction ๐ป ๐‘ง when ๐œ‡ ๎…ž = 0 . 1 โ€‰gmโ€‰cmโˆ’1โ€‰secโˆ’2, ๐œ‚ = 1 โ€‰mHโ€‰cmโˆ’1, ๐‘ฃ ๐‘ = 0 . 1 โ€‰secโˆ’1, ฮฉ = 0 . 0 5 โ€‰radโ€‰secโˆ’1, ๐œ‡ = 0 . 1 โ€‰gmโ€‰cmโˆ’1โ€‰secโˆ’1, ๐œŒ ๐‘‘ = 0 . 0 0 1 โ€‰gmโ€‰cmโˆ’3, ๐ฟ = 0 . 1 โ€‰cm2โ€‰secโˆ’1 and ๐œƒ = 0 โˆ˜ .
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