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Penetrative convection due to absorption of radiation in a magnetic nanofluid saturated porous layer


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Figure 1

Physical configuration.
Physical configuration.

Figure 2

Base flow profile of (1) Tb, (2) ϕb, (3) Hb, and (4) Mb for (a) J = +1, and (b) J = −1.
Base flow profile of (1) Tb, (2) ϕb, (3) Hb, and (4) Mb for (a) J = +1, and (b) J = −1.

Figure 3

Neutral stability curves for distinct values of Y for (a) J = +1 and (b) J = −1; for (1) I_C-I_C, (2) I_C-I_CHF, and (3) I_C-F_CHF boundaries.
Neutral stability curves for distinct values of Y for (a) J = +1 and (b) J = −1; for (1) I_C-I_C, (2) I_C-I_CHF, and (3) I_C-F_CHF boundaries.

Figure 4

Variation of Ra c as a function of E for distinct values of Le for (a) J = +1 and (b) J = −1; for (1) I_C-I_C, (2) I_C-I_CHF, and (3) I_C-F_CHF boundaries.
Variation of Ra c as a function of E for distinct values of Le for (a) J = +1 and (b) J = −1; for (1) I_C-I_C, (2) I_C-I_CHF, and (3) I_C-F_CHF boundaries.

Figure 5

Neutral stability curves for distinct values of Rn for (a) J = +1 and (b) J = −1; for (1) I_C-I_C, (2) I_C-I_CHF, and (3) I_C-F_CHF boundaries.
Neutral stability curves for distinct values of Rn for (a) J = +1 and (b) J = −1; for (1) I_C-I_C, (2) I_C-I_CHF, and (3) I_C-F_CHF boundaries.

Figure 6

Variation of Rac as a function of αL for distinct values of d for (a) J = +1 and (b) J = −1; for (1) I_C-I_C, (2) I_C-I_CHF, and (3) I_C-F_CHF boundaries.
Variation of Rac as a function of αL for distinct values of d for (a) J = +1 and (b) J = −1; for (1) I_C-I_C, (2) I_C-I_CHF, and (3) I_C-F_CHF boundaries.

Figure 7

Variation of Rac as a function of η for distinct values of N A for (a) J = +1 and (b) J = −1; for (1) I_C-I_C, (2) I_C-I_CHF, and (3) I_C-F_CHF boundaries.
Variation of Rac as a function of η for distinct values of N A for (a) J = +1 and (b) J = −1; for (1) I_C-I_C, (2) I_C-I_CHF, and (3) I_C-F_CHF boundaries.

The values of the kc and Rac for three different boundary conditions.

I_C-I_CI_C-I_CHFI_C-F_CHF
JYηkcRackcRackcRac
+110.0012.230.61441.760.36561.350.1476
0.0042.181.94341.741.23431.320.5100
0.0072.122.75611.721.84371.290.7712
0.0102.053.28831.702.28751.250.9622
50.0012.220.12981.760.07611.360.0304
0.0042.230.49571.760.29341.350.1176
0.0072.220.82361.760.49381.350.1980
0.0012.221.11511.760.67761.340.2717
100.0012.220.06531.760.03821.360.0153
0.0042.230.25491.760.14971.350.0597
0.0072.230.43371.760.25611.350.1019
0.0102.230.60131.760.35741.350.1418
–110.0012.180.66401.750.39201.350.1554
0.0042.012.41041.691.55001.30.6131
0.0071.823.55261.612.53001.241.0167
0.0101.634.23201.533.27181.171.3456
50.0012.220.13221.760.07731.360.0308
0.0042.200.53121.750.31171.350.1238
0.0072.170.92541.740.54771.350.2172
0.0102.151.30711.740.78311.350.3106
100.0012.220.06591.760.03851.360.0154
0.0042.210.26471.760.15471.360.0615
0.0072.210.46361.750.27121.360.1076
0.0102.200.66141.750.38791.360.1537

Comparison of Ra c and k2.

Hill [13]Present study
Jηk c2Ra ck c2Ra c
+10.0014.97200.6476676884.97200.647666602
0.0055.11743.0543211135.11753.054321508
0.015.29085.6997347545.29005.699684893
−10.0014.89900.6671257864.89910.667125722
0.0054.75253.5414428254.75243.541426234
0.014.56177.6667755444.56167.666778591
eISSN:
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Language:
English
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4 times per year
Journal Subjects:
Geosciences, other, Materials Sciences, Composites, Porous Materials, Physics, Mechanics and Fluid Dynamics