Table 1 Comparison between LRPSM with FTC-VIM and FTC-HPM for example 1.

From: Adapting Laplace residual power series approach to the Caudrey Dodd Gibbon equation

x

t

Numerical solution

LRPSM with 3 terms

LRPSM with 2 terms

FTC-VIM37

FTC-HPM37

α = 0.7

α = 0.9

α = 1

α = 1

α = 1

α = 1

-50

0

0

0

0

0

0

0

2

6.40972e−14

1.87107e−14

3.78100e−16

1.80551e−14

1.76778e−11

1.76778e−11

4

3.04059e−13

1.07794e−13

2.97855e−15

7.07545e−14

3.53211e−11

3.53211e−11

6

5.67030e−13

2.13785e−13

9.90035e−15

1.55999e−13

5.29318e−11

5.29318e−11

8

8.32476e−13

3.27108e−13

2.31153e−14

2.71817e−13

7.05119e−11

7.05119e−11

10

1.09255e−12

4.43976e−13

4.44757e−14

4.16356e−13

8.80633e−11

8.80633e−11

-40

0

0

0

0

0

0

0

2

9.51288e−12

2.77692e−12

5.61150e−14

2.67962e−12

2.62363e−09

2.62363e−09

4

4.51263e−11

1.59981e−11

4.42056e−13

1.05009e−11

5.24212e−09

5.24212e−09

6

8.41547e−11

3.17285e−11

1.469342e−12

2.31523e−11

7.85578e−09

7.85578e−09

8

1.23550e−10

4.85472e−11

3.43061e−12

4.03412e−11

1.04649e−08

1.04649e−08

10

1.62149e−10

6.58920e−11

6.60078e−12

6.17927e−11

1.30697e−08

1.30697e−08

0

0

0

0

0

0

0

0

2

1.50403e−04

4.18130e−05

1.26391e−06

1.85127e−05

6.54334e−02

6.54334e−02

4

7.46909e−04

2.52505e−04

1.01620e−05

7.91573e−05

1.30909e−01

1.30909e−01

6

1.41638e−03

4.96853e−04

3.44342e−05

1.89673e−04

1.96434e−01

1.96434e−01

8

2.09931e−03

7.42150e−04

8.18630e−05

3.57844e−04

2.62018e−01

2.62018e−01

10

2.76599e−03

9.68940e−04

1.60187e−04

5.91408e−04

3.27666e−01

3.27666e−01

40

0

0

0

0

0

0

0

2

1.24156e−12

3.47519e−13

7.83542e−15

3.78077e−13

4.02445e−10

4.02445e−10

4

6.99716e−12

2.45302e−12

6.36846e−14

1.54465e−12

8.04102e−10

8.04102e−10

6

1.44110e−11

5.42196e−12

2.18401e−13

3.55058e−12

1.20491e−09

1.20491e−09

8

2.3152e−11

9.15479e−12

5.26119e−13

6.44999e−12

1.60484e−09

1.60484e−09

10

3.31208e−11

1.36464e−11

1.04446e−12

1.03005e−11

2.00381e−09

2.00381e−09

50

0

0

0

0

0

0

0

2

8.36560e−15

2.34156e−15

5.27946e−17

2.54746e−15

2.71165e−12

2.71165e−12

4

4.71465e−14

1.65283e−14

4.29103e−16

1.04077e−14

5.41799e−12

5.41799e−12

6

9.71007e−14

3.65329e−14

1.47157e−15

2.39236e−14

8.11868e−12

8.11868e−12

8

1.55998e−13

6.16844e−14

3.54496e−15

4.34597e−14

1.08133e−11

1.08133e−11

10

2.23166e-13

9.19492e-14

7.03753e-15

6.94043e-14

1.35016e-11

1.35016e-11