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Theory and Modern Applications

Table 4 Numerical results with \(\varepsilon _{1}=10^{-4}\) for Example 2

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

10−2

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

1.99e–02

1.13e–02

6.12e–03

3.10e–03

1.48e–03

6.48e–04

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

0.82

0.88

0.98

1.06

1.19

 

10−4

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

2.07e–02

1.16e–02

6.05e–03

2.96e–03

1.43e–03

6.09e–04

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

0.84

0.93

1.03

1.05

1.23

 

10−6

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

2.22e–02

1.21e–02

6.29e–03

3.17e–03

1.49e–03

6.29e–04

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

0.88

0.94

0.99

1.09

1.24

 

10−8

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

2.19e–02

1.21e–02

6.32e–03

3.16e–03

1.49e–03

6.29e–04

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

0.86

0.94

1.00

1.08

1.24

 

10−10

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

2.17e–02

1.21e–02

6.45e–03

3.17e–03

1.49e–03

6.31e–04

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

0.84

0.91

1.02

1.09

1.24

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