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Theory and Modern Applications

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

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

\(\varepsilon _{1}\)

 

N = 32

N = 64

N = 128

N = 256

N = 512

N = 1024

20

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

5.02e–02

2.74e–02

1.37e–02

7.30e–03

3.80e–03

1.90e–03

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

0.87

1.00

0.91

0.94

1.00

 

K

4

4

3

3

3

3

2−2

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

5.26e–02

2.90e–02

1.45e–02

7.80e–03

4.10e–03

2.10e–03

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

0.86

1.00

0.89

0.93

0.97

 

K

4

4

3

3

3

3

2−4

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

5.33e–02

2.94e–02

1.48e–02

8.00e–03

4.10e–03

2.10e–03

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

0.86

0.99

0.89

0.96

0.97

 

K

4

4

3

3

3

3

2−6

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

5.11e–02

2.85e–02

1.44e–02

7.70e–03

3.90e–03

2.00e–03

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

0.84

0.98

0.90

0.98

0.96

 

K

4

4

3

3

3

3

2−8

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

4.76e–02

2.62e–02

1.31e–02

6.80e–03

3.50e–03

1.80e–03

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

0.86

1.00

0.95

0.96

0.96

 

K

4

4

3

3

3

3

2−10

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

4.70e–02

2.59e–02

1.29e–02

6.90e–03

3.60e–03

1.80e–03

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

0.86

1.01

0.90

0.94

1.00

 

K

4

4

3

3

3

3

2−12

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

5.10e–02

2.83e–02

1.50e–02

7.80e–03

3.90e–03

2.00e–03

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

0.85

0.92

0.94

1.00

0.96

 

K

5

5

6

4

3

3

2−14

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

5.54e–02

3.03e–02

1.62e–02

8.40e–03

4.30e–03

2.20e–03

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

0.87

0.90

0.95

0.97

0.97

 

K

6

5

4

4

4

3

2−16

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

5.98e–02

3.14e–02

1.66e–02

8.60e–03

4.40e–03

2.30e–03

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

0.93

0.92

0.95

0.97

0.94

 

K

8

7

6

4

4

4

2−18

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

5.89e–02

3.14e–02

1.68e–02

8.70e–03

4.50e–03

2.30e–03

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

0.91

0.90

0.95

0.95

0.97

 

K

8

6

5

5

4

4

2−20

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

5.86e–02

3.14e–02

1.69e–02

8.70e–03

4.50e–03

2.30e–03

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

0.90

0.89

0.96

0.95

0.97

 

K

9

8

6

5

6

4