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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