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Table 4 Effects of different parameters on the development of thermal runaway

From: The analysis of a reactive hydromagnetic internal heat generating poiseuille fluid flow through a channel

Pade

H

\(\gamma\)

\(\delta\)

G

\(\beta\)

\(\lambda _c(m=-2)\)

\(\lambda _c(m=0)\)

\(\lambda _c(m=0.5)\)

2/2

1

1

1

1

0.5

−1.7811263742438508

1.0523144807452944

1.2366868184966630

2/2

1

2

1

1

0.5

−1.6241610492525835

0.9575639392658895

1.2326845092486176

2/2

1

3

1

1

0.5

−1.4923147215659487

0.8785368728933426

1.2284706885201377

2/2

1

1

1

1

0.5

−1.7811263742438508

1.0523144807452944

1.2366868184966630

2/2

2

1

1

1

0.5

−1.8283359751229398

1.0788970932308604

1.2370083898323496

2/2

3

1

1

1

0.5

−1.8785238395429784

1.1097801101901550

1.2381827113700314