ASSOCIATED TRANSFORMS FOR SOLUTION OF NONLINEAR
EQUATIONSJOYATIDEBNATHandNARAYANC.DEBNATH
Department
of Mathematics and ComputerScienceUniversity ofWisconsin River
Falls, WI
54022U.S.A.
Abstract. Nonlinearmultivariable differentialorintegrodifferential equations with terms of mixed dimensionalitycanbe solvedusingmultidimensional Laplace transform. Thespecial technique usedtofindthe inverseofthe multidimensional Laplace transform is knownas
theassociationof variables.Inthis paper,somebasictheoremsaredevelopedforthetheory oFassociation. Examples arepresented foreach theorem. Once the basic theorems are established,itispossible to derive manyusefulssociatedpairs.
KEY WORDS AND PHRASES.
MultidimensionalLaplace
transform and Nonlinearequations.1980
AMS SUBJECT CLASSIFICATION
CODE. 44A10, 44A30.1. INTRODUCTION.
In
systems engineering,nonlinear differentialorintegrodifferential equationsare solved usingmultiple dimensional Laplace transform.A
commonly used method forobtaining theinverseof the multidimensionalLaplacetransformiscalledtheassociationofvariables.Suppose F(sl,
s2,...,sn)
beaLaplace transform.Its
n-dimensionalinversecanbefound bytheintegralf(tl,t2,...,t,)
=_L’ [F(s,s2,...,sn);tl,t2,... ,t,]
1
(2ri)"
at --ioo
.
--ioo j=lF(s,s2,...,s,) I dsj (1.1)
In
certain nonlinearsystems analysis, particularlyinVolterraseries applications[1-2]
onNonlinear systems
[3-5],
it becomes necessary to take the inverse of the n-dimensional Laplacetransform andspecifythis inverseimagein the specialcase:t
t2tn
t.We
denotethisimage function ofonevariablebyg(t),
org(t) f(t,tz,...,tn)],,=,,
,.=,(1.2) An
alternative approach to obtain the time function,g(t),
is to associate with givenF(s,s,...,sn)
afunctionG(s)
from whicha directapplication of theone- dimensional inversetransform yieldsg(t).
Thisspecial method of computing theinverse transformis saidtobethe association of variables. ThefunctionG(s)
iscalledthe associated transform ofF(sl
s2,DEBNATH
Recently,Chert and Chiu
[6]
and Koh[7]
have presented several theorems forevaluating the associated transformG(s)
using certain types ofF(sl,s2,...,s,). In
this paper, a set ofnew and important theoremsare developed Several illustrative examples are in- cluded.However,
once the fundamental theorems areestablished, we can derivemany usefulassociatedpairs anduse themconveniently.2. THEOREMS ON ASSOCIATED
TRANSFORMS.
Suppose G(s)
be the associated transform ofF(I,2,...,,)
andG(s)
be that ofF(,...
,s,,_,,,+,...,s,),
m<
n. Letk be any constant andwerestrictthe vaxiables1,
,..., ,
totherighthalf of thecomplex plane.Theorem 2.1. /.fagivenfunction
F(sl,sz,...,sn)
can bewritten in theformF(sl,sz,... ,s,)
An-I
and if
F(s,... ,Sm-,sm+,...,sn) G(s).
Then theassoc/ated transformwhere
Ai
means the association process for finding associated transform ofa function consisting of variables.PROOF:
By
equations(1.1)
and(1.2),
wehave?(t) f(t, t,..., t,)l,t=,
,.=t1
(2ri)"
c,t-iooc,--ioo .--ioo j=l
ox+ioo o.+ioo
k
exp
Fl(..ql,...
,,.qm_l,8re+l,,,5,)
1
/
kexp(s,t)dam
2ri 8
(,S2m +
ot(27ri) "-
--iO0f...II...l
Ore-- --ioOre+ On--io0
F(s,...,Sm_t,sm+t,...,s,)exp
k 1-cost
g(t)
kTingLaplaceTrsform of bothsidesof the equation
(2.1)
yieldsG’(8)--,
- G’I(, GI(,S- is)-
Hence
thetheoremisproved. |Example 2.1.
(2.1)
Consider
and let
F(s,,s2,s3)
s3(s, + a)(s2 + b)(s +
c) F,(,,,,=)
Using the table givenin
[6],
wefindFl(l,82)---.i, GI(,..q)"
A2s+a+b"
By
Theorem2.1A3 k 1
f(sl,S2, S3) G(s)’-
- - ( k[ + +
sjrajrb,+a+
1)[(
k-(, +
2+ 4,;@ s+a+b-ic s+a+b] ) + 1 +c -’
s+a+b+ic180 J. DEBNATH AND
Example 2.2.
Let
and take
k
[(, + ) +b(,, + ) + ] ( +d)
F(,, )
a(, + ) + b(, + ) + "
Use
of the tablein[6]
givesA2 1
F1 (, s2) ----+G(s)=
as2
+
bs+
cThusTheorem2.1yields
A3 k 2
F(s,,s2,s3) a(s)
as2
+
bs+
ca(s id) + b(s id) +
c1
a(s + id)
:z+ b(s + id) +
cTheorem 2.2. Ifagivenftmction
F(sl,s2,...,s,,)
can be factoredinthe form ks,,,(Sm + a)(s,,, + b) F(s’’’’’s"-l’s’’+l’’’’’s’)
and if
then theassociatedtransform
C(,) -C,(,) + ab(a
kb) [bC, (s + a) aC, (s + b)].
PROOF"
By
equations(1.1)
and(1.2),
weget9(t) f(t,t=,...,t,)l,,=,2
,.=,LX’ [F(,,=,...,,);t,,t=,...,t,]l,,=,,
1
t -ioo on-io
exp
Fl(..ql,...
sin_l,am+l,...,Sn)
exp m
+
iooexp(smt)dm
(2ri)"-
t+ioo om-t+ioo m+t +ioo =n+ie
/...//.../
Ott --io0 Ore- --iO0m+t-ioo on-ioo
Fl(,Sl,... ,Sm-l,Sm+l,...,n)exp
j=l
dsx dsm-1 dSm+l ds.
L? ",(’m + )(.. +
1);
i’ll [Fl(81,..
=k 1
+ ,t,(,- t,)
1(be_at ae_b,)] gl(t)
a,(t) + (_ )
On
taking Laplacetransform of bothsidesgf
equation(2.2),
weobtain(,) (,) + ab(
ak,
o)[bGl(s + a) aG(s,)]
This establishes the theorem. |
(2.2)
Example 2.3.
Suppose
F(s,,
s2,sa)
(s + s + a)sa(sa + b)(sa + c)
182 J.
and let
Fromthe table shmvnin
[5]
F,(, )
sl
+
s2+
a(,,)----,v,()=
A2 1Thenbyusing Theorem2.2,weget
A3 k
F(s,,s2,s3) G(s)
bc(s + a)
k
bc( + )
k
be(
s+ A)
Example 2.4.
k c b
bc(b-c)
s+a+bs+a+c (c )( + + + c) bc(c b) (s +
a+ b)(s
4-a4-c)
k s4-a4- b 4-
c) ( + + )( + + )
Consider
and take
k
F,(,,,)
(s + a)(s: + b)"
Fromthe table shownin
[6]
r,(,)--a()=
A2s+a+b"
Thenbyusing Theorem2.2,weget
As k
l
k d cF(sl,.S2,83)
G(.s)
-
dk 8++
4-a14- b4-cd(c (+++)(+a++d) d) s+a+b+c+d
.s4-a4-b 4-c .s4-a4-b4- dTheorem2.3. /f afunction
F(sl,s2,... ,sn)
isof the formF(Sl,S2,... ,Sn) k(s2m
4-aSm4-b)
( _,,) F,(,,..., -,,
a+,,..)
with
rl(8l,...,.Sm-l,.m+l,...,sn) a(s).
ThenF(,,,... ,s,)
.-__,a(,)
PROOF: By
definitions(1.1)
and(1.2), g(t) f(tl,
t2,...,tn)ltt=,,
exp
/...//.../
Fl(sl,...,sm-l,Sm+l,...,s,)exp
ds
...dOm-ldSm+l ...ds.
2+b b]
=k
a_sinhat+
2 coshat-- gl(t)
_
91(t)
sinh t+ g,(t)eoshat k(a a2 + b)
kb(2.3)
Taking Laplace transformonbothsidesof(2.3)
a(s)
ka[a,(s a) a,(s + a)] + k(a
2+ b)
= [a,(, =) + a,( + =)1-
[(* +
a,+ )C,(, ) + (* + )a,( + ) 2a,(,)]
2a2
Example
2.5.Suppose
andsay
l(s] + as + b) F(,,,)
(, + ,)( +,)( + + )(, _.)
1
(81 + )(82 " )(81 ""
82+ )"
184 J. DEBNATH AND N.C.
Use
of the table givenin[6]
A2 1
V,(sl,s2) al(s)
(s + 2c)(s +/3)"
Applicationof Theorem 2.3 gives k [ 72
+aT+
b() [( + 2)(
72-aT
+b (, +. + 2)(, +. + Z)
Example 2.6.
( + 2)( + Z)
Consider
F(sl,s:,sa) k(s +
as3+ b)
813233{(,Sl
-t-32) -I" (81 -- 82) -- d}(8
O2)
and let
FI(s, se)
1{( + ) + ( + ) + d}"
Thenbyusing the result shownin
[6],
s(s +
cs+ d)"
Theorem 2.3 gives
k a
+aa+b
() ( ){( ) + ( ) + d}
aZ-aa+b
( + ){( + .) + ( + a) + d}
2b s(s
+
cs+ d)
Theorem2.4. If
F(s,s2,... ,s,,)
can beexpressed
inthefollowingform(s., +a)
F(sl,s2,...,s,,)=
2F(s ...,s,,_,s,,,+,,...,s,,) s,.(,. + ,)
where
Then the associatedtransform
G(s)
kV,(s)-
- sV,(d)-
1+ -a G,(s-
1
(I-a)Gl(S+itr)]
2c2
PROOF:
By
definitions(1.1)
and(1.2),
By
the results ofinverseLaplacetransform shownin[8],
weobtainOn
taking Laplace transform of both sidesof(2.4)
L[9(t);s] L 91(t) + -dg(t) 9(t)cosat
ka t
1
-igl (t)
sinWeestablish the theorem. Thatis,
Simplifying,
ka d k
[al(
3ion) + Gl(3 + io)l
ka
2ic---
S[G(s ia) Gx(s + it,)].
[1
aff__Gl(s)_
1( a)
a(s)
k-TG(s)-
22- a(s + i)
|1+al(s ict)
Example
(2.4)
Consider
Thenwefind
/( + -)
F(sl,S2,S3)-
22
b)"
s(s+ )(s+s2+
1 A2 1
FI(Sl, 32)
Sl 4"324" b
G(s)
34"b"
Use
of Theorem 2.4 gives1 a
( + ) ( + ) ( l+.--a o) 2a2(s_ia+b)
1( l-i-- o) 2a2(s+ia+b)
1k 2 2a a-ai a+ai
2a
"-F +
----7(s + b) tr(s
ia+ b) a(s +
ia+ b)
k
[2(s+a+b)_ 2ct(s+a+b)
2
( + b) c,(s +
b+ ia)(s +
b-ia)
k(s
4"a4"b)
1 Io2
(3
4"b)
2(3
4"b)
24"2 Example 2.8.Suppose
k(s + a)
F(31,32,33) 3132332(31
4"324"5)(31
4"2)"
186 J. DEBNATH Thenwe canfind
1 A2 1
( + + ) ,()
( + )
UsingTheorem2.4, weget
2a(2s + b)
a-ais2(s + b)
2a(s ia)(s
ia+ b)
a+ai
a(s + ia)(s +
ia+ b)
Theorem2.5. /fa function
F(Sl,S2,...,s,,)
canbeexpressedinthe form(3 4-a32m 4-b8 4-)k F(3I,...,3m_l,m+l,...,,Sn), F(sl,S2,...,s,,)
(Sm + a)(Sm + fl)(Sm +7)(Sm + 6)
thenitsassociated transform
() - ( -,)(Z- ,)( -,)
a73 a7aa22+
4- bab7 cc( + ) + ( 3 )( a/2
4-)( b
c) ( + )
63--a624- b6 c
a,( + "r) +
(, 1( )(-r 1 G,( + )
where
G (s)
is the associatedtransformof PROOF:By
definitions(1.1)
and(1.2)
9(t) L [F(Sl,S2,...,sn);t,t,...
.qm 4-
-I-
kL[1 (sin + a)(Sm + )(Sm + 7)(Sin + 6)
;tLZ_ [Fl(s,...,Sm-a,Sm+l,...,s,,);t,t,...,t].
Referringtothe results givenin
[8],
a
3-aa 24-ba-c
(t) - + ( (, 7:1 1( -)(
a724-)( -)( b7
c-r) 1
e-Tt+ (- )(- Z)(6- Z) /3 a/2
4-b
c( )( )(7 )
Taking Laplace transformonbothsidesof equation
(2.5),
a
3-aa 24-ba-c
L [g(t); s]
-kL(-_ -)-"-a- = ) e-atgl(t)
4-(- 3 )(- Z)(- Z) a2
4-bfl
c(2.5)
7 a72
+
b7 c+ (, "r)( ")( ") -’,(t) +
63 a624- b6 c
(- )(- )(- ) e-St
ga(t); s]
We
finallyobtaina
3-aa 2+ba-c a() -,
( ,1(, )( ) G(s+a)+ 3 a2
4-b
cGl(S 4-/)
7 a72
+ b7
c( )(- )(- ) a(s+7)+
63 a624- b c
( )(- )(- ) al(3
4-6)] I
Example 2.9.
Consider
F(sl,s2,s3) (d + + + )
(, + d)(, + )(,, + )(,, + Z)(, + 7)( + )"
Directuseof the table givenin
[7],
wefind1 A2 1
(’ =)
( + )(2 + ) -- ’() + +
Thus, by Theorem2.5
F(sl,s2,s3)- G(s)
-k a3 aa
+
ba c( ,)( )( ,)( + , +
d+ )
3 a + b
c( Z)(V Z)( Z)(, + Z +
d+ )
7 a7
+ b7-
c( )( )( )(, +
7+
d+ )
$3
a62 +
bd c( )(Z )( )(, + +
d+ )
Example 2.10.Suppose
Thenwefind
1 A 1
F,(,)
+ +
dG,() + d"
Use
ofTheorem2.5givesA,
r
a3 aa2+
b cF(, , ) G()
-k[( )(7 )( )( + + d)
Theorem2.6. /fafunction
then
k
($m
q")2($m "l-) F(al’’’’’Sm-a’’m+l’’’’’$n)’
k
,
G(,) ( )2 C,(, + ) (Z )G,(, + ,) C,(, + )
PROOF:
By
definitions(1.1)
and(1.2)
g(t) L=’ [F(sl,S2,...,Sn);t,t,...,t]
188 J. DEBNATH
( + )=( +
;_ [,(,,...,_,,
+,...,,); ,,...,t]
[-, + (- )-, -,] ().
(_ )
On
ting Laplace trsformonboth sides,oneobtns,
d(s+a) G(s +a)] ,
,( + ) (# )
() (Z )
Example 2.11.
Let
F(sl,s2,ss)
(sl
4-a)(2
4-b)(s3
4-)(s3
4-d)
2"Then
F(,)
1( + )( +
Thus, the application ofTheorem2.6shows
A2 1
--- () s4-a+b"
(c-d) s+a+b+c
(c d)
1(s+a+b+d) s+a+b+d F(s,s2,s3)---,G(s)=
Examvle 2.12.
Suppose
F(81, s2,.3)
{a(, + ) + b(, + ) + }( + )2( + )-
Thus
1 A2 1
F,(,,)
{( + ,), + ( + ,) + } --- () = +
and usingTheorem 2.6,weget
A3 k 1
F(,, , ) -- V() ( ) [( + ) + b( + ) +
( a)(2as + 2a + b)
1+ {( + ) + b( +/) + } ( + ) + b(
Following
analogous
arguments,it iseasytoprove thefollowingresults.Theorem2.7.
F(sl,s2,... ,s,,)
thenitsassociatedtransformk
[G(s 2a) + 2a(s) + G(s + 2a)l.
G()
Example 2.13.
Consider
Then
Example 2.14.
(.91
4-a)(.92 + b).93(.93 4a2)"
G()
ks+a+b-2a ++ s+a+b s+a+b+2a
{( += + b)’- = ’ }
{( +
a+ b)=
-4}( +
a+ b)"
Considering
We
obtainF(.91,
.92,.93) (s
22c,)/
{( + ) + b(, + ) + }( 4)"
k[
1 4- 9.G() ( 2) + b( 2) + +
b+
or,
( + 2.) + b( + 2) +
k
[ (a
4-b)s
4-4a24-ca() ,{( 21 + b( 21 + c}{.( + 21 + b( + 21 + } +
a.9 2 i4- bs 4-c Theorem2.8.
F(.sl,
.92,,sn)
k(.gin4-
[)(.92m 92) F(.9’"
Sm-1, .gm+l,thenitsassociatedtransform
G() 2( )
Example 2.15.
Let
F(sl,s2,sa)
k(.91
4-a)(.92
4-b)(s3
4-a)(.9 -/2)"
Then,
directapplicationofTheorem2.8 gives,G(s)
12(f
2-or2) -(.9 4-a4-b4-
k s+a+b-ct
/2
a(s +
a+ b)2 -1
2k
(/- )
+ (++b-)
.9+a+b+
{(.9
4-a4-b) --/2 }(.9
4-a4- b 4-)"
(+)
Z( +
a+
b+ Z)
190
Example 2.16.
Suppose
{( + ,), + b( + ,) + }(, + )( 3)"
Then,weobtain
G() 2( ) -( + ) + b( + ) + {a( )’- + b( ) + } + {( + )2 + b( + ) + }
3.
CONCLUSIONS.
Theoremsonassociated transforms
developed
in this paperarerigorous andshouldbe veryusefulincalculatingtheinverse Laplacetransform forcertainfunctions. Theseresults should be applicable forobtainingsolutions ofawide classofnonlinear equations, which may be encounteredfrequently
in systems engineering.Moreover,
these theorems can directlybe applied to derive manynew associated pairs, and thusone can easily extend thetablesgivenin[5-7]
many fold. Theresultsof thispaperwillhelpdevelop
morebasic theoremsin thisdirectionand willapear insubsequentpapers.ACKNOWLEDGEMENT.
Authorsexpress theirgrateful thanksto theUniversity ofWisconsin at River Falls for providingfinancial supportinpublishingthis paper.
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