Skip to main content

Theory and Modern Applications

Table 3 Comparative study between ADM [28], VIM [29], LADM [30], CRFDTM [26] and q-HATM for the approximate solution \(u(x,t)\) at \(\omega =0.005\), \(\ell= 0.1\), \(c=10\), \(\alpha =1 \) and \(\hslash =-1\) for Example 6.2

From: A reliable technique for fractional modified Boussinesq and approximate long wave equations

(x,t)

\(\vert {u}_{\mathrm{Exact}} - {u}_{\mathrm{ADM}} \vert \)

\(\vert {u}_{\mathrm{Exact}} - {u}_{\mathrm{VIM}} \vert \)

\(\vert {u}_{\mathrm{Exact}} - {u}_{\mathrm{LADM}} \vert \)

\(\vert {u}_{\mathrm{Exact}} - {u}_{\mathrm{CRFDTM}} \vert \)

\(\vert {u}_{\mathrm{Exact}} - {u}_{{q}\text{-}\mathrm{HATM}}^{ ( {3} )} \vert \)

(0.1,0.1)

8.02989 × 10−6

1.23033 × 10−4

7.10000 × 10−9

2.77556 × 10−17

2.77556 × 10−17

(0.1,0.3)

7.38281 × 10−6

3.69597 × 10−4

6.50000 × 10−9

2.77556 × 10−17

2.77556 × 10−17

(0.1,0.5)

6.79923 × 10−6

4.92780 × 10−4

5.90000 × 10−9

3.33067 × 10−16

3.33067 × 10−16

(0.2,0.1)

3.23228 × 10−5

1.69274 × 10−5

2.82000 × 10−8

2.77556 × 10−17

2.77556 × 10−17

(0.2,0.3)

297172 × 10−5

1.89210 × 10−4

2.59000 × 10−8

4.16334 × 10−17

4.16334 × 10−17

(0.2,0.5)

2.73673 × 10−5

1.55176 × 10−4

2.41000 × 10−8

3.60822 × 10−17

3.60822 × 10−17

(0.3,0.1)

7.32051 × 10−5

1.12345 × 10−5

6.33670 × 10−8

1.38778 × 10−17

1.38778 × 10−17

(0.3,0.3)

6.73006 × 10−5

6.55176 × 10−5

5.85000 × 10−8

2.77556 × 10−17

2.77556 × 10−17

(0.3,0.5)

6.19760 × 10−5

2.12346 × 10−5

5.40000 × 10−8

3.19189 × 10−16

3.19189 × 10−16

(0.4,0.1)

1.31032 × 10−4

7.36513 × 10−5

1.12400 × 10−7

1.38778 × 10−17

1.38778 × 10−17

(0.4,0.3)

1.20455 × 10−4

9.5016 × 10−5

1.03900 × 10−7

2.77556 × 10−17

2.77556 × 10−17

(0.4,0.5)

1.10919 × 10−4

8.23160 × 10−4

9.61000 × 10−8

3.19189 × 10−16

3.19189 × 10−16

(0.5,0.1)

2.06186 × 10−4

5.55176 × 10−5

1.75500 × 10−7

0

0

(0.5,0.3)

1.89528 × 10−4

3.21715 × 10−6

1.62200 × 10−7

5.55112 × 10−17

5.55112 × 10−17

(0.5,0.5)

1.74510 × 10−4

2.00176 × 10−5

1.5010 × 10−7

3.19189 × 10−16

3.19189 × 10−16