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Theory and Modern Applications

Table 1 Error estimates and convergence rates

From: An expanded mixed covolume element method for integro-differential equation of Sobolev type on triangular grids

h , Δ t

\(\boldsymbol{\|u-u_{h}\|_{L^{\infty}(L^{2}(\Omega))}}\)

Rate

\(\boldsymbol{\| \boldsymbol{\sigma}-\boldsymbol{\sigma}_{h}\|_{L^{\infty}((L^{2}(\Omega ))^{2})}}\)

Rate

\((\frac{\sqrt{2}}{8},\frac{1}{8})\)

3.8464e − 003

 

1.6043e − 002

 

\((\frac{\sqrt{2}}{16},\frac{1}{16})\)

2.0591e − 003

0.90

8.6877e − 003

0.88

\((\frac{\sqrt{2}}{32},\frac{1}{32})\)

1.0637e − 003

0.95

4.5181e − 003

0.94

\((\frac{\sqrt{2}}{64},\frac{1}{64})\)

5.4043e − 004

0.98

2.3037e − 003

0.97

h , Δ t

\(\boldsymbol{\|\lambda-\lambda_{h}\| _{L^{\infty}((L^{2}(\Omega))^{2})}}\)

Rate

\(\boldsymbol{\|\lambda -\lambda\|_{L^{\infty}(H(\operatorname{div},\Omega))}}\)

Rate

\((\frac{\sqrt{2}}{8},\frac{1}{8})\)

1.5432e − 002

 

5.1929e − 002

 

\((\frac{\sqrt{2}}{16},\frac{1}{16})\)

8.3902e − 003

0.88

2.7873e − 002

0.90

\((\frac{\sqrt{2}}{32},\frac{1}{32})\)

4.3491e − 003

0.95

1.4411e − 002

0.95

\((\frac{\sqrt{2}}{64},\frac{1}{64})\)

2.2108e − 003

0.98

7.3231e − 003

0.98