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2.6 Existence and Uniqueness of Solutions, Wronskian
- Theorem 2 ; Existence and Uniqueness Theorem for IVP
If are continuous functions on some interval I andand is in I,
then IVP consisting of (1) and (2) has a unique solution
)(xp )(xq 0x
(1) 0)()( yxqyxpy
(2) ,)( 00 Kxy 10)( Kxy
- Theorem 3 ; Linear Dependence and Independence of Solutions
Let ODE (1) has continuous coefficients on an open interval I. )(xp )(xqand
Then two solutions of (1) on I are linearly dependent on I if and1y
only if their "Wronskian",
2yand
- Theorem 1 ; Existence of a General Solution
If )(xp )(xqand are continuous functions on an open interval I, then ODE (1)
has a general solution.
''),( 122121 yyyyyyW
is 0 at some in I. 0x
Ex. 1) wxy cos1 wxy sin2 and are solutions of .02 ywy
Wronskian is,
wwxwwxwwxwwxw
wxwxwxwxW
22 sincos
cossin
sincos)sin,(cos
→ linearly independent if and only if 0w
For.tan/ 12 wxyy 0,0 2 yw and 0/ 12 yy
→ linearly dependent
Ex. 2) General solution of 02 yyy is .)( 21
xexccy
andxe and xxe are linearly independent.
0)1()1(
),( 222
xxx
xx
xx
xx exeexexe
xeexeeW
Its Wronskian is not 0,
Namely,
where, ''''
),( 1221
21
21
21 yyyyyy
yyyyW
⇐ Wronski determinant or Wronskian
Hence, if there is an in I where, then,0W are linearly 1y 2yand1x
independent on I.
?)( 1 y
2.7 Nonhomogeneous ODEs
- (1)
(2)
- General solution of the nonhomogeneous ODE (1) on an open interval I is,
)()()( xyxyxy ph (3)
where, ; general solution of (2) on an open interval I 2211 ycycyh
py ; any solution of (1) containing no arbitrary constant
- Theorem 1 ; Relations of solutions of (1) to those of (2)
(a) The sum of solution of (1) on some open interval I and a solution
y~ of (2) on I is a solution of (1) on I.
In particular, (3) is a solution of (1) on I.
(b) The difference of two solutions of (1) on I is a solution of (2) on I.
0)(),()()( xrxryxqyxpy
0)()( yxqyxpy
y
- Method of Undetermined Coefficients ; method to find
This method is suitable for linear ODEs with constant coefficients a .b
(4)
is an exponential function, a power of)(xr ,x cosine or sine,
or sum or products of such functions.
itself.)(xr
Method to find py
Term in r(x) Choices for yp(x)
xkexCe
),1,0( nkxn01
1
1 KxKxKxK n
n
n
n
wxkwxk sin,cos wxMwxK sincos
,sin,cos wxkewxke axax )sincos( wxMwxKeax
py
These functions have derivatives similar to
)(xrbyyay
and
where
- Choice Rules for Method of Undetermined Coefficients
(a) Basic Rule ; py is determined using the above table and coefficients are
determined by substituting and its derivatives into (4).py
(b) Modification Rule ; If a term happens to be a solution of py
homogeneous ODE corresponding to (4), is multiplied topy (or byx 2x
if this solution corresponds to a double root of the characteristic
equation of the homogeneous ODE)
(c) Sum Rule ; If is a sum of functions in the first column of the above )(xr
table, is the sum of the functions in the corresponding lines of the py
second column.
Some Examples
22 xyyy xx
h ececyyyy 2
21
2 ,02,02
,01
2
2 KxKxKyp ,2 12 KxKyp 22Kyp
2
01
2
2122 )(2)2(22 xKxKxKKxKKyyy ppp
4/3,022,2/1,2/1 0012122 KKKKKKK
75.05.05.0 2 xxyp
1)
75.05.05.0 22
21 xxececyyy xx
ph
xeyy 34 2)
,04 yy ,042 xBxAyh 2sin2cos
xeyy 34 13/1,149 CCCx
p ey 3
13
1
x
ph exBxAyyy 3
13
12sin2cos
,3x
p Cey ,3 3x
p Cey x
p Cey 39
Some Examples
xyyy sin2 xx
h ececyyyy 2
21
2 ,02,02
,sincos xMxKyp ,cossin xMxKyp xMxKyp sincos
xxMxKxMxKxMxKyyy ppp sinsin2cos2cossinsincos2
13,03 KMKM
xxyp sin1.0cos1.0
3)
xxececyyy xx
ph sin1.0cos1.02
21
xeyyy x 3cos134 24)
,0134 yyy ,01342 )3sin3cos(2 xBxAey x
h
),3sin3cos(2 xMxKxey x
p
1.0,1.0 KM
,32 i
ph yyy
Ex. 5) Solve IVP, 5.1)0(,0)0(,001.0 2 yyxyy
xBxAyyy h sincos,0
,01
2
2 KxKxKyp ,2 12 KxKyp 22Kyp
,001.02 2
01
2
22 xKxKxKKyy pp
002.02,02,0,001.0 200212 KKKKKK
002.0001.0 2 xyp002.0001.0sincos 2 xxBxAyyy ph
002.0,0002.0)0( AAy
5.1)0(,002.0cossin ByxxBxAy
002.0001.0sin5.1cos002.0 2 xxxy
Ex. 6) Solve IVP, ,1025.23 5.1 xeyyy 0)0(,1)0( yy
,025.23 yy ,0)5.1(25.23 22 x
h exccy 5.1
21 )(
,5.12 x
p eCxy ,)5.12( 5.12 x
p exxCy x
p exxxCy 5.12)25.2332(
xeyyy 5.11025.23
,1025.2)5.12(3)25.262( 222 CxxxCxxC 5C
,5 5.12 x
p exy xx
ph exexccyyy 5.125.1
21 5)(
,1)0( 1 cy xxx exxeexcccy 5.125.15.1
212 5.710)5.15.1(
,05.1)0( 12 ccy 5.15.1 12 cc
xxx exxexexy 5.125.125.1 )55.11(5)5.11(
Ex. 7) Solve IVP,
,09.0sin25.0cos275.02 xxxyyy ,78.2)0( y 43.0)0( y
,075.02 yyy ,075.022 2/3,2/1 2/3
2
2/
1
xx
h ececy
,21 ppp yyy ,cossin,sincos 11 xMxKyxMxKy pp
xMxKyp sincos1
1,0 MK
32.012.02 xyp
32.012.0sin2/3
2
2/
121 xxececyyyy xx
pph
78.232.0)0( 21 ccy
12.0cos5.15.0 2/3
2
2/
1 xececy xx
0,1.3,43.012.015.15.0)0( 2121 ccccy
32.012.0sin1.3 2/ xxey x
xyp sin1
,275.02 KMK 25.075.02 MKM
0,, 212012 ppp yKyKxKy
0275.0,09.075.0 101 KKK 32.0,12.0 01 KK
2.10 Solutions by Variation of Parameters
- Method of undetermined coefficients is efficient for obtaining in (1), if py
)(xr is not complicated.
(1)
This method is restricted to functions )(xr whose derivatives are similar
form to )(xr itself.
- The method of variation of parameters is generally used for obtaining py
where are assumed to be continuous on open interval I.
(2) dxW
ryydx
W
ryyxyp
12
21)( ; variation of parameters
where form a basis of solutions of the corresponding homogeneous 21, yy
ODE
)()()( xryxqyxpy
(3)
and is the Wronskian of 21, yyW
(4) 1221 yyyyW
0)()( yxqyxpy
rqp ,,
- Formula (2) is possible only if formula (1) is a standard form. And it may
often cause difficulties when the integration in (2) is not simple or (1) has
variable coefficients.
Ex. 1) Solve, xyy sec
,sin,cos 21 xyxy 1)sin(sincoscos),( 21 xxxxyyW
xxcxxcyyy ph sin)(cos)cosln( 21
xdxxxxdxxxxyp seccossinsecsincos)( xxxx sincoslncos
Ex. 2) Solve, xyy tan
,sin,cos 21 xyxy 1)sin(sincoscos),( 21 xxxxyyW
xxxxcxcyyy ph tanseclncossincos 21
xdxxxxdxxxxyp tancossintansincos)(
xdxxdxx
xx sinsin
cos
sincos
2
xxdxx
xx cossin
cos
1coscos
2
xxdxxxx cossin)sec(coscos
xxxxxx cossin)tansecln(sincos xxx tanseclncos