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Global Stability For Double-Diffusive Convection In A Couple-Stress Fluid Saturating A Porous Medium

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Apr 08, 2019

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Figure 1

Geometrical configuration of the problem.
Geometrical configuration of the problem.

Figure 2

The variation in the critical thermal Rayleigh number Rcef with the couple-stress parameter F1.
The variation in the critical thermal Rayleigh number Rcef with the couple-stress parameter F1.

Figure 3

The variation in the critical thermal Rayleigh number Rcef with the couple -stress parameter Da
The variation in the critical thermal Rayleigh number Rcef with the couple -stress parameter Da

Figure 4

The variation in the critical thermal Rayleigh number Rcef with the solute gradient Sf
The variation in the critical thermal Rayleigh number Rcef with the solute gradient Sf

The variation in the fluid-based critical thermal Rayleigh number R cef with the couple-stress parameter (Da ) for F1=2, Vr=1 and Sf = 100_

DaxceRcef
0.010.56841897.1
0.020.56821001.9
0.030.56797017
0.040.56765532
0.050.56734636
0.060.5671405.2
0.070.5668365.0
0.080.5665330.6
0.090.5663305.7
0.100.5660285.8
0.110.5667269.5

The variation in the fluid-based critical thermal Rayleigh number Rcef with the couple-stress parameter F1 for Da=0_02, Vr =1 and Sf = 100_

F1xceR cef
010.9636307.90
20.6154661.40
30.56821001.9
40.54831340.8
50.53741679.0
60.53052017.0
70.525823537
80.52232696.0
90.51973030.3
100.51763367.9
0.51593705.6

The variation in the fluid-based critical thermal Rayleigh number R cef with the solute gradient (Sf) for Da, Vr =1_

SRcef(F1=1xce=0.6164)${{R}_{cef}}\left( \begin{align}& {{F}_{1}}=1 \\ & {{x}_{ce}}=0.6164 \\ \end{align} \right)$Rcef(F1=2xce=0.5682)${{R}_{cef}}\left( \begin{align}& {{F}_{1}}=2 \\ & {{x}_{ce}}=0.5682 \\ \end{align} \right)$Rcef(F1=3xce=0.5483)${{R}_{cef}}\left( \begin{align}& {{F}_{1}}=3 \\ & {{x}_{ce}}=0.5483 \\ \end{align} \right)$
100661.41001.91340.8
200761.41101.91440.8
300861.41201.91540.8
400961.41301.91640.8
5001061.41401.91740.8
6001161.41501.91840.8
700271.41601.91940.8
8001361.41701.92040.8
9001461.41801.92140.8
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