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Accelerated HPSTM: An efficient semi-analytical technique for the solution of nonlinear PDE’s

  • Deepak Grover , Dinkar Sharma and Prince Singh EMAIL logo
Published/Copyright: August 13, 2020
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Abstract

In this paper a novel technique i.e. accelerated homotopy perturbation Sumudu transformation method (AHPSTM), which is a hybrid of accelerated homotopy perturbation method and Sumudu transformation to obtain an approximate analytic solution of nonlinear partial differential equation (PDE) with proportional delay, is used. This approach is based on the new form of calculating He’s polynomial, which accelerates the convergence of the series solution. The series solutions obtained from the proposed method are found to converge rapidly to exact solution. In order to affirm the effectiveness and legitimacy of proposed method, the proposed technique is implemented on nonlinear partial differential equation (PDE) with proportional delay. The condition of convergence of series solution is analyzed. Moreover, statistical analysis has been performed to analyze the outcome acquired by AHPSTM and other semi-analytic techniques.

1 Introduction

The model including delay differential equations may display physical frameworks for which the advancement rely upon the present and past circumstances. This type of model is found in the area of epidemiology and population dynamics, where the delay is due to the gesture or maturity period, or is in numerical control, where there is a delay in taking care of the controller input circle. The partial differential equation (PDE) with proportionate delay is a particular case of a delay differential equation which emerge uniquely in the field of medicine, population ecology, control frameworks, biology, and climate models [1]. Different authors have adopted different numerical techniques like Sarkar et.al [2] use homotopy perturbation method (HPM) to obtain the solution of time-fractional non-linear partial differential equation (PDE) with proportional delay. Chen and Wang [3] use variational iteration method (VIM) while Biazar and Ghanbari [4] apply HPM for solving neutral-functional differential equation with proportionate delay. Singh and Kumar [5] use fractional variational iteration method (VIM) for the solution of fractional PDE with proportional delay. Abazari and Ganji [6], Abazari and Kilicman [7] use differential transform method (DTM) to solve delay (PDE) partial differential equation. Many researchers use various techniques for the solution of such nonlinear PDE’s like HPM [8, 9, 10, 11], homotopy perturbation transformation method (HPTM) [12, 13, 14, 15, 16], homotopy analysis method (HAM) [17], homotopy perturbation Sumudu transformation method (HPSTM) [18, 19, 20], homotopy perturbation Elzaki transformation method HPETM [21, 22], Variational iteration method [23] etc. Khan [12] introduce HPTM which is blend of HPM and Laplace transformation for solving nonlinear equations using He’s polynomial. Here, we have used a new form of He’s polynomial called accelerated He’s polynomial [24] which accelerates the rate of convergence of the method. So, we propose a new form of semi-analytic technique named as AHPSTM (Accelerated homotopy perturbation Sumudu transformation method) to study the following type of PDE with proportional delay.

wtx,t=F(w(p1x,q1t),wx(p2x,q2t),wxx(p3x,q3t),),w(x,0)=g(x)(1)

pi, qj ∈ (0, 1), i, j ∈ ℕ, g(x) is the initial condition and F is the partial differential operator.

Definition 1.1

The Sumudu transformation over the set of functions

A=ftM,τ1,τ2>0,ft<Metτj,ift1j×[0,),j=1,2},

is defined as Sft=1u0ftetudt,t>0.

Properties of Sumudu Transform

  1. S {1} = 1

  2. Stmm!=um,

  3. S{fn(t)}=1unS{f(t)}k=0n11unkfk(0).(*)

2 Accelerated homotopy perturbation Sumudu transform method (AHPSTM)

To elucidate the proposed technique, consider the following nonlinear equations.

nϕtn+Lϕx,t+Nϕx,t=G(x,t)(2)

with condition ϕi(x, 0) = ki(x), i = 0, 1, 2, − 1.

On applying Sumudu transformation to Eq. (2), we have

Snϕtn+Lϕ(x,t)+Nϕ(x,t)=SG(x,t)(3)

Applying properties of Sumudu transformation (*) to Eq. (3), we get

S{ϕx,t}=unk=0n11unkϕk(x,0)+unSGx,tLϕx,t+Nϕx,t(4)

Further, operating inverse Sumudu transformation to Eq. (4) gives,

ϕx,t=k=0n1tkk!ϕkx,0+S1unSGx,tLϕx,t+Nϕx,t(5)

Now, appling homotpoy perturbation method to Eq. (5), we have

0=1pϕx,tϕx,0+pϕx,tk=0n1tkk!ϕkx,0pS1unSGx,tLϕx,t+Nϕx,t

where p ∈ [0, 1] is a parameter. Let

ϕx,t=n=0ϕnpn(6)

and

Nϕx,t=n=0H~npn(7)

where n represents accelerated He’s polynomial with

H~n(ϕ0,ϕ1,ϕ2,ϕn)=NSni=0n1H~i(8)

with 0 = N(ϕ(x0)), and Sk = (ϕ0 + ϕ1 + ϕ2 + … + ϕk). Using (6), (7) and (8) the Eq. (5) gives,

n=0ϕnpn=ϕx,0+pk=1n1tkk!ϕkx,0S1+unSGx,tLn=0ϕnpn+n=0H~npn(9)

Now, on comparing coefficients of the like power of p, we have

p0:ϕ0=ϕx,0p1:ϕ1==k=1n1tkk!ϕkx,0+S1{unS{Gx,t{Lϕ0+H~0}}}p2:ϕ2=S1{unS{Lϕ1+H~1}}

Hence, the solution of Eq.(1) is obtained by taking p → 1, i.e.

ϕx,t=n=0ϕn(10)

3 Condition of convergence of accelerated HPSTM

Here, we emphasize on condition of convergence of the above introduced method.

Theorem 3.1

Let ϕ and ϕn be elements of a Banach space, then the series

ϕx,t=n=0ϕnpn

converges to the solution of Eq. (1) if ∥ϕn+1∥ ≤ κϕn∥, where 0 < κ < 1.This conditions of convergence of the series is proved in [15, 20].

4 Application

Example 4.1

Solution of generalized Burgers’ equation with proportional delay.

Consider the following initial value problem [6]

ψx,tt=ψxxx,t+ψxx,t2ψx2,t2+12ψx,t,t>0,xR(11)

with ψ(x, 0) = x. By applying Sumudu transformation on Eq. (11), we have

S{ψx,tt12ψx,t}=Sψxxx,t+ψxx,t2ψx2,t2(12)

Or

Sψx,t=x22u+2u2uSψxxx,t+ψxx,t2ψx2,t2(13)

By applying inverse Sumudu transformation on Eq.(13), we have

ψx,t=xet2+S12u2uSψxxx,t+ψxx,t2ψx2,t2(14)

Now, apply AHPSTM on Eq. (14), we get

n=0ψn(x,t)pn=xet2+pS12u2uSn=0pnψnx,txx+n=0pnH~n(15)

and the initial couple of terms of n are given as

H~0=ψ0xx,t2ψ0x2,t2,H~1=ψ0xx,t2ψ1x2,t2+ψ1xx,t2ψ0x2,t2+ψ1xx,t2ψ1x2,t2,H~2=ψ0xx,t2ψ2x2,t2+ψ1xx,t2ψ2x2,t2+ψ2xx,t2ψ0x2,t2+ψ2xx,t2ψ2x2,t2+ψ2xx,t2ψ1x2,t2,H~3=ψ0xx,t2ψ3x2,t2+ψ1xx,t2ψ3x2,t2+ψ2xx,t2ψ3x2,t2+ψ3xx,t2ψ3x2,t2+ψ3xx,t2ψ2x2,t2+ψ3xx,t2ψ1x2,t2,

On looking at the like powers of p of Eq.(15), we get

p0:ψ0=xet2;p1:ψ1=t2xet2;p2:ψ2=xet2t2222!+12t3233!;p3:ψ3=xet212t3233!+78t4244!+58t5255!+516t6266!+564t7277!;p4:ψ4=xet218t4244!+2364t5255!+58t6266!+395512t7277!+24554096t8288!+(16)

As p → 1, we get the series solution of Eq. (11) as

ψx,t=n=0ψn(x,t)

Using Eq. (16), we get

ψx,t=xet21+t2+(t2222!)+(t3233!)+(t4244!)+6364(t5255!)+1516(t6266!)+435512(t7277!)+(17)

The exact solution of Eq. (11) in closed form is

ψx,t=xet(18)

On comparing (18) and (17), we find that the series solution rapidly converges to the actual solution. So, we discover that the accelerated homotopy perturbation Sumudu transformation method provides us the faster rate of convergence which can be seen in table 1 that the value of ψn (APSTM) decreases rapidly.

Table 1

Approximate solution of Eq. (11) using AHPSTM

xtψ2ψ3ψ4
0.250.0022592890.0000486750.000000387068
0.250.50.0104494260.000465360.00000754081
0.750.0271745220.001875250.0000464816
10.0558160850.005302690.000178857
0.250.0045185770.00009734990.000000774136
0.50.50.0208988510.0009307210.0000150816
0.750.0543490450.0037504990.0000929631
10.1116321690.010605380.000357713
0.250.0067778660.0001460250.0000011612
0.750.50.0313482770.0013960810.0000226224
0.750.0815235670.0056257490.000139445
10.1674482540.0159080690.00053657

Table 2

Approximate solution of Eq. (11) up to 4th order approximation

xtExact solutionAHPSTMDTM [6]HPM [2]Abs. error (AHPSTM)Abs. error (DTM)Abs. error (HPM)
0.250.250.3210063.21E-013.21E-010.3210041.22E-092.12E-062.12E-06
0.50.4121800.4121804.12E-010.4121094.83E-087.09E-057.09E-05
0.750.5292500.5292495.29E-010.5286874.52E-075.63E-045.63E-04
10.6795700.6795680.6770830.6770832.35E-062.49E-032.49E-03
0.50.250.6420126.42E-016.42E-010.6420082.40E-094.24E-064.24E-06
0.50.8243600.8243608.24E-010.8242199.66E-081.42E-041.42E-04
0.751.0585001.0584991.06E+001.0573739.03E-071.13E-031.13E-03
11.3591401.3591361.3541671.3541674.70E-064.97E-034.97E-03
0.750.250.9630190.9630199.63E-010.9630133.70E-096.36E-066.36E-06
0.51.2365411.2365411.24E+001.2363281.45E-072.13E-042.13E-04
0.751.5877501.5877491.586061.586061.36E-061.69E-031.69E-03
12.0387112.0387042.031252.031257.05E-067.46E-037.46E-03

Example 4.2

Solution of non-linear PDE with proportional delay,

Consider the following initial value problem [6]

ψx,tt=ψxxx,t2ψxx,t2ψx,t,t>0,xR(19)

with ψ(x, 0) = x2. By applying Sumudu transformation on Eq. (19), we have

Sψx,tt+ψx,t=Sψxxx,t2ψxx,t2(20)

Or

Sψx,t=x211+u+u1+uSψxxx,t2ψxx,t2(21)

By applying inverse Sumudu transformation on Eq. (21), we have

ψx,t=x2et+S1u1+uSψxxx,t2ψxx,t2(22)

Now, apply AHPSTM on Eq.(22), we get

n=0ψn(x,t)pn=x2et+pS1u1+uSn=0pnH~n(23)

and the initial couple of terms of n are given as

H~0=ψ0xxx,t2ψ0x,t2,H~1=ψ0xxx,t2ψ1x,t2+ψ1xxx,t2ψ0x,t2+ψ1xxx,t2ψ1x,t2,H~2=ψ0xxx,t2ψ2x,t2+ψ1xxx,t2ψ2x,t2+ψ2xxx,t2ψ2x,t2+ψ2xxx,t2ψ0x,t2+ψ2xxx,t2ψ1x,t2,H~3=ψ0xxx,t2ψ3x,t2+ψ1xxx,t2ψ3x,t2+ψ2xxx,t2ψ3x,t2+ψ3xxx,t2ψ3x,t2+ψ3xxx,t2ψ2x,t2+ψ3xxx,t2ψ1x,t2,

On looking at the like powers of p of Eq. (23), we get

p0:ψ0=x2et;p1:ψ1=x2et(2t);p2:ψ2=x2et(22t22!)+1223t33!;p3:ψ3=x2et12(23t33!)+78(24t44!)+5825t55!+51626t66!+564(27t77!)p4:ψ4=x2et18(24t44!)+2364(25t55!)+58(26t66!)+395512(27t77!)+2455409628t88!+(24)

As p → 1, we get the series solution of Eq. (19) as

ψx,t=n=0ψn(x,t)

Using Eq. (16), we get

ψx,t=x2et1+(2t)+(22t22!)+23t33!+(24t44!)+6364(25t55!)+1516(26t66!)+435512(27t77!)+(25)

The exact solution of Eq. (11) in closed form is

ψx,t=x2et(26)

On comparing (26) and (25), it is clear that the series approaches to the exact solution. Also from the table 3, we find that ∥ψ4∥ < ∥ψ3∥ < ∥ψ2∥, i.e. the series solution satisfy the condition of convergence.

Table 3

Approximate solution of Eq.(19) using AHPSTM

xtψ2ψ3ψ4
0.250.0065914130.0006262030.0000211215
0.250.50.0221130970.0047555620.000350289
0.750.0415165920.0150738010.001831803
10.061313240.0332569580.005952034
0.250.0263656520.0025048130.0000844858
0.50.50.0884523880.0190222460.001401156
0.750.1660663660.0602952040.007327211
10.2452529610.1330278340.023808135
0.250.0593227160.005635830.000190093
0.750.50.1990178730.0428000540.003152601
0.750.3736493240.1356642090.016486225
10.5518191620.2993126260.053568305

Example 4.3

Consider the following initial value problem [6]

ψx,tt=ψxxx2,t2ψxx2,t2ψxx,tψx,t,t>0,xR(27)

with ψ(x, 0) = x2.

On operating Sumudu transformation on Eq. (27), we have

Sψx,tt+ψx,t=Sψxxx2,t2ψxx2,t2ψxx,t(28)

Or

Sψx,t=x211+u+u1+uSψxxx2,t2ψxx2,t2ψxx,t(29)

By applying inverse Sumudu transformation on Eq. (29), we have

ψx,t=x2et+S1u1+uSψxxx2,t2ψxx2,t2ψxx,t(30)

Now, apply AHPSTM on Eq. (30), we get

n=0ψn(x,t)pn=x2et+pS1u1+uSn=0pnH~nψxx,t(31)

and the initial couple of terms of n are given as

H~0=ψ0xx2,t2ψ0xxx2,t2,H~1=ψ0xx2,t2ψ1xxx2,t2+ψ1xx2,t2ψ0xxx2,t2+ψ1xx2,t2ψ1xxx2,t2,H~2=ψ0xx2,t2ψ2xxx2,t2+ψ1xx2,t2ψ2xxx2,t2+ψ2xx2,t2ψ2xxx2,t2+ψ2xx2,t2ψ0xxx2,t2+ψ2xx2,t2ψ1xxx2,t2,H~3=ψ0xx2,t2ψ3xxx2,t2+ψ1xx2,t2ψ3xxx2,t2+ψ2xx2,t2ψ3xxx2,t2+ψ3xx2,t2ψ3xxx2,t2+ψ3xx2,t2ψ2xxx2,t2+ψ3xx2,t2ψ1xxx2,t2,

On looking at the like powers of p of Eq. (31), we get

p0:ψ0=x2et;p1:ψ1=0,p2:ψ2=0,p3:ψ3=0,

Hence, the solution of Eq. (27) is given by

ψx,t=n=0ψn(x,t)

i.e.

ψx,t=x2et(32)

Also, the exact solution of Eq. (27) is in the closed form is

ψx,t=x2et(33)

So from Eq.(32) and Eq.(33), we have found this exact solution in only one iteration.

Figure 1 Approximate solution of Eq. (11) using AHPSTM
Figure 1

Approximate solution of Eq. (11) using AHPSTM

Figure 2 Exact solution
Figure 2

Exact solution

Figure 3 Approximate solution of Eq. (11) using AHPSTM
Figure 3

Approximate solution of Eq. (11) using AHPSTM

Figure 4 Exact solution
Figure 4

Exact solution

Figure 5 Approximate solution of Eq. (27) using AHPSTM
Figure 5

Approximate solution of Eq. (27) using AHPSTM

Figure 6 Exact solution
Figure 6

Exact solution

5 Statistical analysis

In order to validate the solution obtained from the semi-analytic technique AHPSTM, and to investigate the techniques (AHPSTM, HPM and DTM) for their outcome in regard of solution of non-linear problem considered in Eq. (11), (19) and (28) we employe a statistical technique i.e. paired student’s t-test at 5% level of significance to the data of Tables 2, 4 and 6. The null hypothesis is

Table 4

Approximate solution of Eq.(19) up to 4th order approximation

xtExact solutionAHPSTMDTM[6]HPM [2]Abs. Error (AHPSTM)Abs. Error (DTM)Abs. Error (HPM)
0.250.250.0802518.03E-028.03E-020.0802512.77E-075.30E-075.30E-07
0.50.1030450.1030351.03E-010.1030279.80E-061.77E-051.77E-05
0.750.1323120.1322291.32E-010.1321728.30E-051.41E-041.41E-04
10.1698930.1694990.1692700.1692713.93E-046.22E-046.22E-04
0.50.250.3210063.21E-013.21E-010.3210041.11E-062.12E-062.12E-06
0.50.4121800.4121414.12E-010.4121093.92E-057.09E-057.09E-05
0.750.5292500.5289175.29E-010.5286873.32E-045.63E-045.63E-04
10.6795700.6779980.6770830.6770831.57E-032.49E-032.49E-03
0.750.250.7222640.7222617.22E-010.722262.50E-064.78E-064.78E-06
0.50.9274050.9273179.27E-010.9272468.82E-051.60E-041.60E-04
0.751.1908121.1900651.1895451.1895457.47E-041.27E-031.27E-03
11.5290331.5254971.5234371.5234383.54E-035.60E-035.60E-03

Table 5

Approximate solution of Eq. (19) up to 4th order approximation

xtExact solutionAHPSTMDTM [6]HPM [2]Abs. Error (AHPSTM)Abs. Error (DTM)Abs. Error (HPM)
0.250.250.048684.87E-024.87E-020.048675504.88E-074.88E-07
0.50.037910.03790813.79E-020.037923101.50E-051.50E-05
0.750.029520.02952292.96E-020.029632501.10E-041.10E-04
10.022990.02299240.0234370.023437504.45E-044.45E-04
0.50.250.194701.95E-011.95E-010.194702101.95E-061.95E-06
0.50.151630.15163261.52E-010.151692706.00E-056.00E-05
0.750.118090.11809161.19E-010.118530204.39E-044.39E-04
10.091960.09196980.093750.0937501.78E-031.78E-03
0.750.250.438070.43807544.38E-010.438079804.39E-064.39E-06
0.50.341170.34117343.41E-010.341308501.35E-041.35E-04
0.750.265700.26570610.2666930.266693109.87E-049.87E-04
10.206930.20693210.2109370.210937504.01E-034.01E-03

Null hypothesis: H0A:μ1A=μ2jA,H0B:μ1B=μ2jB,H0C:μ1C=μ2jC,

where μ1k,;k = A; B; Cdenotes the exact solution of (11), (19) and (28) respectively, while μ2jk;k=A;B;C;j = 1; 2; 3 denote the approximate solution of Eq. (11), (19) and (27) via AHPSTM, DTM and HPM, respectively. The considered degree of freedom is nk − 1 = 12 − 1 = 11 and the tabulated value of tat α = 5% is ∣ttab.∣ = 2.201. The calculated values of test statistic of Eq. (11), (19) and (27) for pair AHPSTM with exact solution Ai; DTM with exact solution Bi; and HPM with exact solution Ci, i = 1, 2, 3 are given below:

tcal.A1=2.192,tcal.B1=2.282,tcal.C1=2.282,tcal.A2=1.884,tcal.B2=1.914,tcal.C2=1.914,tcal.B3=1.954,tcal.C3=1.954.

From the above analysis, it is clear that null hypothesis H0 is accepted for Eq. (11) only for pair of AHPSTM solution and exact solution, and is rejected for DTM with pair of exact solution and HPM with exact solution. For Eq. (19) and (27), null Hypothesis is accepted in all the three cases (Note: For Eq. (27), as we get exact solution with AHPSTM, so we do not test statistically). Hence, with this statistical analysis we conclude that AHPSTM gives better solution than other semi analytical technique like DTM and HPM.

6 Conclusion

A new semi analytic technique of accelerated AHPSTM is implemented for the approximate analytical solution of non-linear partial differential equations with proportional delay. It provides the power series solution in the form of a rapidly convergent series. The proposed technique converges faster than other semi- analytic techniques like HPM, VIM and DTM. To validate the efficiency and reliability of the proposed technique, the condition of convergence is verified and statistical analysis is performed. Tables 1 and 3 show that the series solution obtained from the proposed method satisfied condition of convergence, while Tables 2, 4, 5 and Figures 1, 2, and 3 show that the approximate results are close to the exact solution of the considered models with given initial conditions. Also, the approximate solution obtained from AHPTM gives better result with just four iterations than other methods like HPM, VIM and DTM. The proposed method gives a better result for the solution of non-linear PDEs as no discritizing algorithm and no linearization is required for non-linear problems. Further, it is concluded that with the proposed techniques only few iterations will lead to the solution and hence it reduces the computational cost. Thus, this technique is equally competent for linear and non-linear partial differential equation.

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Received: 2020-03-23
Accepted: 2020-06-09
Published Online: 2020-08-13

© 2020 Deepak Grover et al., published by De Gruyter

This work is licensed under the Creative Commons Attribution 4.0 International License.

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