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Table 4 \(C_{2}\)-order of convergence for Test problem 3

From: High-order compact scheme for the two-dimensional fractional Rayleigh–Stokes problem for a heated generalized second-grade fluid

γ = 0.1

h/τ

Max error

\(C_{2}\)-order

\(h =\tau =\frac{1}{2}\)

9.293 × 10−2

\(h =\frac{1}{4} \), \(\tau =\frac{1}{32}\)

6.869 × 10−3

3.76

\(h = \tau =\frac{1}{4}\)

4.962 × 10−2

\(h =\frac{1}{8} \), \(\tau =\frac{1}{64}\)

3.558 × 10−3

3.80

γ = 0.2

h/τ

Max error

\(C_{2}\)-order

\(h =\tau =\frac{1}{2}\)

8.200 × 10−2

\(h =\frac{1}{4} \), \(\tau =\frac{1}{32}\)

5.916 × 10−3

3.78

\(h = \tau =\frac{1}{4}\)

4.298 × 10−2

\(h =\frac{1}{8} \), \(\tau =\frac{1}{64}\)

3.058 × 10−3

3.81

γ = 0.3

h/τ

Max error

\(C_{2}\)-order

\(h =\tau =\frac{1}{2}\)

7.092 × 10−2

\(h =\frac{1}{4} \), \(\tau =\frac{1}{32}\)

5.068 × 10−3

3.81

\(h = \tau =\frac{1}{4}\)

3.643 × 10−2

\(h =\frac{1}{8} \), \(\tau =\frac{1}{64}\)

2.616 × 10−3

3.80

γ = 0.4

h/τ

Max error

\(C_{2}\)-order

\(h =\tau =\frac{1}{2}\)

5.966 × 10−2

\(h =\frac{1}{4} \), \(\tau =\frac{1}{32}\)

4.206 × 10−3

3.83

\(h = \tau =\frac{1}{4}\)

2.996 × 10−2

\(h =\frac{1}{8} \), \(\tau =\frac{1}{64}\)

2.171 × 10−4

3.80

γ = 0.5

h/τ

Max error

\(C_{2}\)-order

\(h =\tau =\frac{1}{2}\)

4.824 × 10−2

\(h =\frac{1}{4} \), \(\tau =\frac{1}{32}\)

3.402 × 10−3

3.82

\(h = \tau =\frac{1}{4}\)

2.359 × 10−2

\(h =\frac{1}{8} \), \(\tau =\frac{1}{64}\)

1.669 × 10−3

3.82

γ = 0.6

h/τ

Max error

\(C_{2}\)-order

\(h =\tau =\frac{1}{2}\)

3.668 × 10−2

\(h =\frac{1}{4} \), \(\tau =\frac{1}{32}\)

2.652 × 10−3

3.79

\(h = \tau =\frac{1}{4}\)

1.735 × 10−2

\(h =\frac{1}{8} \), \(\tau =\frac{1}{64}\)

1.201 × 10−3

3.85