Table 1 |
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The effect of the magnetic field parameter Hax on f"(0), θ' (0) and ϕ'(0) when Grx = 0.5, Gcx = 2, Df = 0.2, and Sr = 0.3 |
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ξ = 0.005 |
ξ = 0.01 |
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SLM results |
LNS Method |
SLM results |
LNS Method |
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Profile |
Hax |
M2 = 2 |
M2 = 3 |
M2 = 2 |
M2 = 3 |
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0.0 |
3.045324 |
3.045324 |
3.045324 |
3.045324 |
3.045324 |
3.045324 |
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|
0.5 |
2.299370 |
2.299370 |
2.299370 |
2.299370 |
2.299370 |
2.299370 |
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|
f"(0) |
1.0 |
1.940291 |
1.940291 |
1.940291 |
1.940291 |
1.940291 |
1.940291 |
|
2.0 |
1.532041 |
1.532041 |
1.532041 |
1.532041 |
1.532041 |
1.532041 |
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|
2.5 |
1.404033 |
1.404033 |
1.404033 |
1.404033 |
1.404033 |
1.404033 |
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0.0 |
0.513493 |
0.513493 |
0.513493 |
0.513493 |
0.513493 |
0.513493 |
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|
0.5 |
0.435640 |
0.435640 |
0.435640 |
0.435640 |
0.435640 |
0.435640 |
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-θ'(0) |
1.0 |
0.392869 |
0.392869 |
0.392869 |
0.392869 |
0.392869 |
0.392869 |
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2.0 |
0.335307 |
0.335307 |
0.335307 |
0.335307 |
0.335307 |
0.335307 |
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2.5 |
0.314405 |
0.314405 |
0.314405 |
0.314405 |
0.314405 |
0.314405 |
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0.0 |
0.289548 |
0.289548 |
0.289548 |
0.289548 |
0.289548 |
0.289548 |
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0.5 |
0.231673 |
0.231673 |
0.231673 |
0.231673 |
0.231673 |
0.231673 |
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-ϕ'(0) |
1.0 |
0.202778 |
0.202778 |
0.202778 |
0.202778 |
0.202778 |
0.202778 |
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2.0 |
0.169217 |
0.169217 |
0.169217 |
0.169217 |
0.169217 |
0.169217 |
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2.5 |
0.157771 |
0.157771 |
0.157771 |
0.157771 |
0.157771 |
0.157771 |
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Sibanda et al. Boundary Value Problems 2012 2012:25 doi:10.1186/1687-2770-2012-25 |
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