Table 3 Computations for \(f({\eta })\) ,\(g({\eta })\), \(h({\eta })\), \(k({\eta })\), \(\theta ({\eta })\), \(\Psi ({\eta })\) with \(\xi _{rad} = 0.1\), \(\xi _{sq} = 0.1\), \(\xi _{z} = 0.2\), \(\xi _{\theta } = 0.5\), \(\xi _{mag} = 0.3\), \(\xi _{pr} = 0.2\), \(\xi _{hm} = 1\), \(\xi _{pm} = 0.2\), \(\xi _{sm} = 1\), \(\xi _{ec} = 0.1\), \(\xi _{vis} = 0.3\), \(S = 0.5\) and various values of \(\eta\).

From: Hydrodynamic analysis of the magnetic field dependent viscous fluid flow and thermosolutal convection between rotating channels

\(\eta\)

HAM result

BVP4c result

 

\(f({\eta} )\)

\(g({\eta} )\)

\(h({\eta} )\)

\(\theta ({\eta} )\)

\(\Psi ({\eta} )\)

\(f({\eta} )\)

\(g({\eta} )\)

\(h({\eta} )\)

\(\theta ({\eta} )\)

\(\Psi ({\eta} )\)

0

0

1

0

1

1

0

1

0

1

1

0.1001

0.0261

0.9267

0.0899

0.8987

0.8974

0.0261

0.9264

0.0899

0.8989

0.8977

0.2002

0.0668

0.8497

0.1911

0.7987

0.7978

0.0669

0.8499

0.1912

0.7989

0.7978

0.3003

0.1258

0.7703

0.2716

0.6989

0.6954

0.1259

0.7704

0.2717

0.6989

0.6955

0.4004

0.1839

0.7100

0.3654

0.5986

0.5944

0.1839

0.7101

0.3655

0.5987

0.5945

0.5005

0.2582

0.6579

0.4619

0.4983

0.4938

0.2582

0.6579

0.4619

0.4983

0.4938

0.6006

0.3324

0.6245

0.5723

0.3994

0.3946

0.3325

0.6246

0.5724

0.3995

0.3947

0.7007

0.3985

0.5875

0.6765

0.2993

0.2951

0.3986

0.5876

0.6766

0.2994

0.2952

0.8008

0.4622

0.5568

0.7845

0.1994

0.1959

0.4623

0.5569

0.7846

0.1995

0.1959

0.9009

0.4981

0.5315

0.8965

0.0997

0.0976

0.4982

0.5316

0.8966

0.0998

0.0977

1

0.5

0.5

1

0

0

0.5

0.5

1

0

0