Research Article

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

Table 4

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

๐‘˜ ๐‘ฃ ๐‘ = 0 . 1 ๐‘ฃ ๐‘ = 0 . 1 ๐‘ฃ ๐‘ = 0 . 2

0.1 1.36664 1.423 1.47494
0.2 1.31426 1.32782 1.33983
0.3 1.2968 1.30284 1.30814
0.4 1.28205 1.28547 1.28847
0.5 1.26666 1.26887 1.27081
0.6 1.25032 1.25188 1.25325
0.7 1.23339 1.23455 1.23556
0.8 1.21631 1.21722 1.218
0.9 1.19955 1.20027 1.20089
1 1.18344 1.18403 1.18454