Preface
This section studies some first order nonlinear ordinary differential equations describing the time evolution (or “motion”) of those hamiltonian systems provided with a first integral linking implicitly both variables to a motion constant. An application has been performed on the Lotka--Volterra predator-prey system, turning to a strongly nonlinear differential equation in the phase variables.
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Introduction to Linear Algebra with Mathematica
Glossary
Adomian Decomposition Method
We illustrate applications of the Adomian decomposition method (ADM for short) by considering nonlinear system of differential equations with two dependent variables:
\[
\begin{cases}
L_1 \left[ y_1 \right] &= N_1 \left[ y_1, y_2 \right] + g_1 (t) ,
\\
L_2 \left[ y_2 \right] &= N_2 \left[ y_1, y_2 \right] + g_2 (t) ,
\end{cases}
\]
subject to the initial conditions
\[
y_1 (0) = y_{10} , \qquad y_2 (0) = y_{20} .
\]
Here L1 and L2
are considered, without loss of generality, first order differential
operators, N1 and N2
are nonlinear operators that do not contain derivatives. In addition
g1(t) and g2(t)
are source terms. Operating with the inverse (integral) operators
L1-1 to the first equation and
L2-1 to the second equation, we reduce the
problem under consideration to a fixed point problem for bounded functions:
\[
\begin{cases}
y_1 (t) &= L_1^{-1}_1 N_1 \left[ y_1, y_2 \right] + L^{-1}_1 g_1 (t) ,
\\
y_2 (t) &= L^{-1}_2 N_2 \left[ y_1, y_2 \right] + L^{-1}_2 g_2 (t) .
\end{cases}
\]
The unknown functions y1(t) and
y2(t)
can be decomposed by infinite series of components
\[
\begin{split}
y_1 (t) &= \sum_{n\ge 0} u_n (t) ,
\\
y_2 (t) &= \sum_{n\ge 0} v_n (t) ,
\end{split}
\]
where the initial approximation is determined by solving the initial value
problems for the uncoupled differential equations:
\begin{align*}
L_1 \left[ u_0 (t) \right] &= g_1 (t) , \qquad u (0) = y_{10} ,
\\
L_2 \left[ v_0 (t) \right] &= g_2 (t) , \qquad v (0) = y_{20} .
\end{align*}
In turn, the nonlinear operators should be represented by using the
infinite series of the so-called Adomian polynomials
An and Bn
\[
\begin{split}
N_1 \left[ u,v \right] &= \sum_{n\ge 0} A_n ,
\\
N_2 \left[ u,v \right &= \sum_{n\ge 0} B_n ,
\end{split}
\]
To understand how the recurrence is derived, it is convenient to introduce
a grouping parameter (which we denote by λ) and represent the solutions
and nonlinear terms in the form of generating functions, where convergence
play no role:
\begin{align*}
y_1 (t) &= \sum_n\ge 0} u_n (t)\,\lambda^n ,
\\
y_2 (t) &= \sum_n\ge 0} v_n (t)\,\lambda^n ,
\\
N_1 \left[ u,v \right] &= \sum_{n\ge 0} A_n \lambda^n ,
\\
N_2 \left[ u,v \right &= \sum_{n\ge 0} B_n \lambda^n .
\end{align*}
Of course, we will set λ to 1 in the final answer, but for now we keep
the parameter λ alive. Substituting the generating functions into the
given system of nonlinear equations, we obtain
\begin{align*}
\sum_n\ge 0} u_n (t)\,\lambda^n &= \lambda\,\sum_{n\ge 0} A_n \lambda^n ,
\\
\sum_n\ge 0} v_n (t)\,\lambda^n &= \lambda\,\sum_{n\ge 0} B_n \lambda^n .
\end{align*}
Equating coefficient of like powers of λ, we derive the recurrence:
\begin{align*}
u_{n+1} &= A_n \left( u_0 , u_1 , \ldots , u_n ; v_0 , v_1 , \ldots , v_n
\right) , \qquad n=0,1,2,\ldots ;
\\
v_{n+1} &= B_n \left( u_0 , u_1 , \ldots , u_n ; v_0 , v_1 , \ldots , v_n
\right) , \qquad n=0,1,2,\ldots .
\end{align*}
We present some codes prepared by
J.-S. Duan. The subroutine PSSOL helps to determine multivariable Adomian polynomials. It has six inputs: Init is 2-D table of the initial values Ck,j, Alpha denotes the 3-D table of the coefficients αk,s,j, Be denotes the 1-D table of the coefficients βk of nonlinearities, F denotesthe 1-D table of the nonlinearities fk, G denotesthe 1-D table of the system input gk, and M is a nonnegative integer that determines the degrees of the output Taylor polynomial solutions to be pk + M for the solutions uk(x), 1 &le k ≤ q.
PSSOL[Init_,Alpha_,Be_,F_,G_,M_]:=Module[{p,q,s,j,ps,g,be,n,i,j1,m,r,k,k1,nu,U,CC,tr,alpha,A,T,se,c},p=Table[Length[Init[[k]]],{k,1,Length[Init]}];q=Length[p];ps=Sum[p[[k]],{k,1,q}];For[k=1,k<=q,k++,For[n=0,n<=M,n++,g[k,n]=1/n!*(D[G[[k]],{x,n}])/.x->0;be[k,n]=1/n!*(D[Be[[k]],{x,n}])/.x->0 ] ];Module[{},For[k=1,k<=q,k++,For[s=1,s<=q,s++,For[j=0,j<=p[[s]]-1,j++,For[n=0,n<=M,n++, alpha[k,s,j,n]=1/n!*(D[Alpha[[k]][[s]][[j+1]],{x,n}])/.x->0]]]]];U=Flatten[Table[Table[Subscript[v, i,j],{j,0,M}],{i,1,Sum[p[[r]],{r,1,q}]}]];CC=Flatten[Table[Table[Table[Product[r+j,{j,1,h}]*c[i,r+h],{r,0,M}], {h,0,p[[i]]-1}],{i,1,q}]];tr=Table[U[[j1]]->CC[[j1]],{j1,1,(M+1)*Sum[p[[r]],{r,1,q}]}];Module[{},For[k=1,k<=q,k++,A[k,0]=F[[k]]/.Subscript[v, j_]->Subscript[v, j,0];Table[T[i,j],{i,1,M},{j,1,i}];se=Table[_,{ps}]/.List->Sequence;For[r=1,r<=M,r++, T[r,1]=Table[Subscript[v, i,r]*D[A[k,0],Subscript[v, i,0]],{i,1,ps}];For[k1=2,k1<=r,k1++,T[r,k1]=Union[Flatten[Table[D[Map[#*Subscript[v, i,1]/(Exponent[#,Subscript[v, i,1]]+1)&,T[r-1,k1-1]], Subscript[v, i,0]], {i,1,ps}]]]];For[k1=2,k1<=Floor[r/2],k1++,T[r,k1]=T[r,k1]\[Union]
(T[r-k1,k1]/.Flatten[Table[Subscript[v, i,j]->Subscript[v, i,j+1],{i,1,ps},{j,1,r-2*k1+1}]])];A[k,r]=(Sum[Total[T[r,k1] ],{k1,1,r}]);
If[EvenQ[r], Do[T[r/2,k1]=., {k1,1,r/2}]]; ];Table[A[k,r],{r,0,M}]]];For[k=1,k<=q,k++, For[r=0,r<=M,r++,A[k,r]= A[k,r]/.tr]];For[k=1,k<=q,k++,For[j=0,j<=p[[k]]-1, j++, c[k,j]=Init[[k]][[j+1]]/j!]];For[n=0,n<=M,n++, For[k=1,k<=q,k++,c[k,p[[k]]+n]=(g[k,n]-Sum[Sum[Sum[Product[m+j,{j,1,p[[s]]-1-nu}]*alpha[k,s,p[[s]]-1-nu,n-m]*c[s,m+p[[s]]-1-nu],{nu,0,p[[s]]-1}],{s,1,q}]+be[k,n-m]*A[k,m],{m,0,n}]) / Product[n+i,{i,1,p[[k]]}]]];For[k=1,k<=q,k++,v[k]=Sum[c[k,j]*x^j,{j,0,p[[k]]+M}]]; j=.;Table[v[k],{k,1,q}] ];
The subroutine NSOL is to find the numerical solution for a nonlnear system of differential equations. It has eight inputs. The first six of them are the same as in the previous routine PSSOL. The last two are the end point X and the step-size h.
NSOL[Init_,Alpha_,Be_,F_,G_,M_,X_,h_]:=Module[{p,q,ps,xn,N1,k,in,al,be,f,g,j1,sol,new},p=Table[Length[Init[[k]]],{k,1,Length[Init]}];q=Length[p]; ps=Sum[p[[k]],{k,1,q}];N1=Floor[X/h]; xn[0]=0;sol={Table[Init[[k]][[1]],{k,1,Length[Init]}]};in=Init;al=Alpha; be=Be;f=F; g=G;For[k=1,k<=N1, k++, xn[k]=N[xn[k-1]+h];new=Table[Table[D[PSSOL[in,al,be,f,g,M][[k]],{x,j1}],{j1,0,p[[k]]-1}], {k,1,q}]/.{x->(xn[k]-xn[k-1])};sol=Append[sol,Table[new[[k]][[1]],{k,1,q}]];in=new; al=al/.{x->h+x}; be=be/.{x->h+x};g=g/.{x->h+x};];Prepend[Transpose[sol],Table[xn[k],{k,0,N1}]]];
Example: Consider the following initial value problem for the linear system of equations:
\begin{align*}
\dot{y}_1 &= -0.1\,y_1 - 49.9\,y_2 ,
\\
\dot{y}_2 &= -50\,y_2 ,
\\
\dot{y}_3 &= 70\,y_2 -120\, y_3 ,
\end{align*}
subject to the initial conditions
\[
y_1 (0) =2 , \quad y_2 (0) =1, \quad y_3 (0) =2.
\]
The exact solution of the above system is
\[
\begin{split}
y_1 (t) &= e^{-50\,t} + e^{-0.1\,t} ,
\\
y_2 (t) &= e^{-50\,t} ,
\\
y_3 (t) &= e^{-50\,t} + e^{120\,t} .
\end{split}
\]
■
Example: Consider the initial value problem:
\begin{align*}
\dot{y}_1 &= -12\, y_1 + 10\, y_2^2 ,
\\
\dot{y}_2 &= y_1 - y_2 - y_1 y_2 ,
\end{align*}
subject to the initial conditions
\[
y_1 (0) =0 , \quad y_2 (0) =0.
\]
The exact solutions of the system is given by
\[
y_1 (t) = e^{-2t} , \quad y_2 (t) = e^{-t} .
\]
■
Example: ■
Example: ■
- Chowdhury, M.S.H., Hashim, I., Hosen, M.A., Solving Linear and Non-Linear Stiff System of Ordinary Differential Equations by Multistage Adomian Decomposition Method, Proc. of TheThirdIntl. Conf. On Advances in Applied Science and Environmental Technology,/E,> -ASET 2015
- Ganji, D.D., Nourollahi, M., Rostamian, M., A comparison of variational iteration method with Adomian’s Decomposition Method in some highly nonlinear equations. International Journal of Science and Technology, 2007, 2(2):179–188
- Rabie, M.E.A. and Elzaki, T.M., A study of some systems of nonlinear partial differential equations by using Adomian and modified decomposition methods, African Journal of Mathematics and Computer Science Research, Vol. 7(6), pp. 61-67, October, 2014; doi: 10.5897/AJMCSR2014.0541 Article Number: 98918D947930
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