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Theory and Modern Applications

Table 8 The \(L_{\infty }\), \(L_{2}\) errors and spatial convergence orders with \(\tau = 1/1000\) for Example 4

From: A high-order numerical scheme using orthogonal spline collocation for solving the two-dimensional fractional reaction–subdiffusion equation

α

h

\(L_{\infty }\) error

Rate

\(L_{2}\) error

Rate

0.2

\(\frac{1}{10}\)

1.5852e−006

 

1.2379e−006

 

\(\frac{1}{20}\)

9.9075e−008

4

7.5769e−008

4.0301

\(\frac{1}{40}\)

6.1922e−009

4

4.6847e−009

4.0156

\(\frac{1}{80}\)

3.8703e−010

3.9999

2.9120e−010

4.0079

0.4

\(\frac{1}{10}\)

1.6877e−006

 

1.3212e−006

 

\(\frac{1}{20}\)

1.0548e−007

4

8.0871e−008

4.0301

\(\frac{1}{40}\)

6.5926e−009

4

5.0005e−009

4.0155

\(\frac{1}{80}\)

4.1219e−010

3.9995

3.1094e−010

3.9995

0.6

\(\frac{1}{10}\)

1.8132e−006

 

1.4238e−006

 

\(\frac{1}{20}\)

1.1333e−007

3.9999

8.7164e−008

4.0299

\(\frac{1}{40}\)

7.0834e−009

3.9999

5.3902e−009

4.0153

\(\frac{1}{80}\)

4.4314e−010

3.9986

3.3537e−010

4.0065

0.8

\(\frac{1}{10}\)

1.9644e−006

 

1.5484e−006

 

\(\frac{1}{20}\)

1.2278e−007

3.9999

9.4810e−008

4.0296

\(\frac{1}{40}\)

7.6745e−009

3.9999

5.8639e−009

4.0151

\(\frac{1}{80}\)

4.8065e−010

3.9970

3.6525e−010

4.0049

0.98

\(\frac{1}{10}\)

2.1217e−006

 

1.6799e−006

 

\(\frac{1}{20}\)

1.3261e−007

4

1.0288e−007

4.0293

\(\frac{1}{40}\)

8.2897e−009

3.9997

6.3642e−009

4.0148

\(\frac{1}{80}\)

5.1997e−010

3.9948

3.9697e−010

4.0029