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Theory and Modern Applications

Table 1 The comparison of the \(l^{2}\)-norm and the \(l^{\infty}\)-norm when \(\tau^{2} = h_{x} =h_{y} \) for \(\mathcal{O}(h_{x}^{4} + h_{y}^{4})\) fourth-order compact finite difference schemes in Example 1, at different values of the step size (for \(N = 4, 8, 16,32,64,128\)) in the x and y directions

From: Fourth-order compact finite difference method for solving two-dimensional convection–diffusion equation

h

\(\mathrm{err}L^{2}\)

order

\(\mathrm{err}L^{\infty}\)

order

\(\frac{1}{4}\)

3.1833e–004

 

6.3680e–004

 

\(\frac{1}{8}\)

2.0323e–005

3.9158

4.0654e–005

3.9160

\(\frac{1}{16}\)

1.2761e–006

3.9815

1.6045e–007

3.9815

\(\frac{1}{32}\)

7.9847e–008

3.9955

1.6045e–007

3.9772

\(\frac{1}{64}\)

4.9917e–009

3.9989

1.0031e–008

3.9989

\(\frac{1}{128}\)

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