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Table 2 The numerical errors

From: Application of C-Bézier and H-Bézier basis functions to numerical solution of convection-diffusion equations

Basis

h

α

\(\|u-u_{h}\|_{\infty}\)

\(\|u-u_{h}\|_{0}\)

\(|u-u_{h}|_{1}\)

Lagrange

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

3.4000e − 03

1.9000e − 03

5.0900e − 02

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

4.1488e − 04

2.4555e − 04

1.2800e − 02

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

4.9912e − 05

3.0760e − 05

3.2000e − 03

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

6.0911e − 06

3.8470e − 06

7.9789e − 04

[3pt] C-Bézier

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

\(\frac{\pi}{4}\)

1.3192e − 08

7.4480e − 09

2.0785e − 07

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

\(\frac{\pi}{8}\)

4.9641e − 11

2.6246e − 11

1.5837e − 09

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

\(\frac{\pi}{16}\)

7.5162e − 14

4.0419e − 14

4.9740e − 12

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

\(\frac{\pi}{32}\)

6.8501e − 14

3.1989e − 14

3.6248e − 12