Skip to main content

Theory and Modern Applications

Table 1 Numerical results with \(\varepsilon _{1}=2^{-9}\) for Example 1

From: An efficient adaptive grid method for a system of singularly perturbed convection-diffusion problems with Robin boundary conditions

\(\varepsilon _{2}\)

 

N = 32

N = 64

N = 128

N = 256

N = 512

N = 1024

20

\(E_{\varepsilon _{1},\varepsilon _{2}}^{N}\)

4.18e–02

2.31e–02

1.25e–02

6.40e–03

3.30e–03

1.70e–03

\(r_{\varepsilon _{1},\varepsilon _{2}}^{N}\)

0.86

0.89

0.97

0.96

0.96

 

K

5

4

4

3

3

3

2−2

\(E_{\varepsilon _{1},\varepsilon _{2}}^{N}\)

4.62e–02

2.65e–02

1.42e–02

7.40e–03

3.80e–03

2.00e–03

\(r_{\varepsilon _{1},\varepsilon _{2}}^{N}\)

0.80

0.90

0.94

0.96

0.93

 

K

5

4

4

3

3

3

2−4

\(E_{\varepsilon _{1},\varepsilon _{2}}^{N}\)

4.66e–02

2.68e–02

1.44e–02

7.30e–03

3.80e–03

1.90e–03

\(r_{\varepsilon _{1},\varepsilon _{2}}^{N}\)

0.80

0.90

0.98

0.94

1.00

 

K

5

4

4

3

3

3

2−6

\(E_{\varepsilon _{1},\varepsilon _{2}}^{N}\)

5.11e–02

2.73e–02

1.42e–02

7.30e–03

3.70e–03

1.90e–03

\(r_{\varepsilon _{1},\varepsilon _{2}}^{N}\)

0.90

0.94

0.96

0.98

0.96

 

K

5

4

4

3

3

3

2−8

\(E_{\varepsilon _{1},\varepsilon _{2}}^{N}\)

4.80e–02

2.59e–02

1.32e–02

6.90e–03

3.50e–03

1.80e–03

\(r_{\varepsilon _{1},\varepsilon _{2}}^{N}\)

0.89

0.97

0.94

0.98

0.96

 

K

4

5

3

3

3

3

2−10

\(E_{\varepsilon _{1},\varepsilon _{2}}^{N}\)

4.95e–02

2.62e–02

1.36e–02

6.80e–03

3.50e–03

1.80e–03

\(r_{\varepsilon _{1},\varepsilon _{2}}^{N}\)

0.92

0.95

1.00

0.96

0.96

 

K

8

4

4

3

3

3

2−12

\(E_{\varepsilon _{1},\varepsilon _{2}}^{N}\)

5.35e–02

2.93e–02

1.53e–02

7.90e–03

3.90e–03

2.00e–03

\(r_{\varepsilon _{1},\varepsilon _{2}}^{N}\)

0.87

0.94

0.95

1.02

0.96

 

K

5

5

5

4

3

3

2−14

\(E_{\varepsilon _{1},\varepsilon _{2}}^{N}\)

5.49e–02

3.06e–02

1.64e–02

8.40e–03

4.40e–03

2.10e–03

\(r_{\varepsilon _{1},\varepsilon _{2}}^{N}\)

0.84

0.90

0.97

0.93

1.07

 

K

7

6

5

4

4

3

2−16

\(E_{\varepsilon _{1},\varepsilon _{2}}^{N}\)

5.78e–02

3.06e–02

1.67e–02

8.70e–03

4.40e–03

2.30e–03

\(r_{\varepsilon _{1},\varepsilon _{2}}^{N}\)

0.92

0.87

0.94

0.98

0.94

 

K

6

5

6

5

4

4

2−18

\(E_{\varepsilon _{1},\varepsilon _{2}}^{N}\)

5.78e–02

3.25e–02

1.66e–02

8.40e–03

4.40e–03

2.30e–03

\(r_{\varepsilon _{1},\varepsilon _{2}}^{N}\)

0.83

0.97

0.98

0.93

0.94

 

K

7

8

5

4

4

4

2−20

\(E_{\varepsilon _{1},\varepsilon _{2}}^{N}\)

5.78e–02

3.09e–02

1.72e–02

8.70e–03

4.30e–03

2.30e–03

\(r_{\varepsilon _{1},\varepsilon _{2}}^{N}\)

0.90

0.85

0.98

1.02

0.90

 

K

7

6

9

5

4

4