Research Article

Dynamical System Analysis of Thermal Convection in a Horizontal Layer of Nanofluids Heated from Below

Table 4

Comparison between Vadasz case ( 𝜙 = 0 ) and the nanofluid case for 𝜙 = 0 . 0 5 with P r = 1 0 , 𝜆 = 8 / 3 for 𝑅 a solitary limit cycle signifying the loss of stability of the steady convection fixed points and the critical value of 𝑅 at which the chaotic behaviour solution occurs.

𝑅 𝑅
(limit cycle)(critical value, chaotic behaviour)

Vadasz 2 3 . 4 7 4 2 4 . 7 3 7
( 𝜙 = 0 )
Ag 3 6 . 9 1 8 3 7 . 5 0 3
Cu 3 5 . 7 6 9 3 6 . 3 0 5
A l 2 O 3 3 4 . 0 3 2 3 4 . 4 9 0
TiO2 3 3 . 3 5 2 3 3 . 8 0 0