unit 8 geotechnical engineering
TRANSCRIPT
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UNIT 8 SECOND-ORDER LINEAR ORDINARY
DIFFERENTIAL EQUATIONS
Unit Structure
8.0 Overview
8.1 Learning Objectives
8.2 Introduction
8.3 Homogeneous Equations with Constant Coefficients
8.4 Differential Operators
8.5 Solving the Inhomogeneous Equation
8.6 Summary
8.7 Answers to Activities
8.0 OVERVIEW
In this Unit, we shall study second-order ordinary differential equations. First we
consider the solution of homogeneous equations, and then show how to solve
inhomogeneous equations.
8.1 LEARNING OBJECTIVES
By the end of this unit, you should be able to do the following:
1.
Find the general solution of homogeneous equations.2. Use D-operators.3. Obtain the complementary function and particular integral of inhomogeneous
second-order linear differential equations.
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8.2 INTRODUCTION
We shall study 2nd
-order constant-coefficientordinary differential equations of the form
)(2
2
xfycdx
dyb
dx
yda =++ , (1)
where the coefficients a, b, care real constants and 0a . is called the free term
or the forcing function.
)(xf
If , then (1)is called a Homogeneousdifferential equation. If , then
(1)is called an Inhomogeneous differential equation.
0)( xf 0)( xf
8.3 HOMOGENEOUS EQUATIONS WITH CONSTANT
COEFFICIENTS
The simplest 2nd
-order differential equation is 02
2
=dx
yd. To find its general solution we
simply integrate twice w.r.t.x. Now,
002
2
=
=dx
dy
dx
d
dx
yd.
Integrating w.r.t.x, we have Adxdx
dy == 0 ;
Integrating again w.r.t. x gives +== BAxdxAy .
Hence the general solution of 02
2
=dx
yd is BAxy += , where A and B are arbitrary
constants, which can be fixed if we are given two conditions onxandy.
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Example 1
Solve 02
2
=dx
yd, given that 3)1(',2)1( == yy .
The general solution is BAxy += . The condition 2)1( =y (i.e., when2=y 1=x )
yields
BA += 12
The second condition (i.e.,3)1(' =y 3'=y when 1=x ) gives [since ]Axy =)('
A=3 .
Hence we have ; therefore theparticular solutionis1,3 == BA
13 = xy .
In general, to solve the equation )(xfdx
ydn
n
= , we just integrate ntimes w.r.t.x.
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Example 2
Solve xexxdx
yd 322
2
sin ++= .
Integrating once, we have
.3
cos3
)sin(
33
32
Ae
xx
dxexxdx
dy
x
x
++=
++=
Integrating once more now yields the general solution
BAxexxy x +++= 3
914
121 sin .
[N.B.Since we are not given any conditions onxandy, we cant determineAandB.]
Activity 1
Solve the following differential equations:
(i) 1)2(',3)2(,02
2
=== yydx
yd;
(ii) 2)0(',1)0(,02
2
=== yydx
yd;
(iii) 3)2(,2)1(,02
2
=== yydx
yd;
(iv) 2)1(,3)1(,02
2
=== yydx
yd;
(v) 252
2
= xdx
yd;
(vi) 4cosh3sinh22
2
++= xxdxyd
;
(vii) 3)0(',2)0(,1322
2
==+= yyxedx
yd x ;
(viii) 5)2(,3)1(,762
2
=== yyxdx
yd;
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We shall now learn how to solve the homogeneous equation
02
2
=++ ycdx
dyb
dx
yda . (2)
Let us assume that is a solution of (2). ThenmxAey=
mxmAe
dx
dy= ,
mxAemdx
yd 22
2
= .
On substituting into (2), we obtain
02 =++ mxmxmx cAebmAeAeam .
Since , this simplifies to0mxAe
02 =++ cbmam .
This quadratic equation is called the Auxiliary Equation (A.E.) of Eqn (2).
The auxiliary equation can easily be written down. We simply replaceyby 1,dx
dyby m,
and2
2
dx
ydby .2m
Now, the quadratic equation can have either 2 distinct roots, or 2 equal roots, or 2
complex roots. Each case gives a different type of solution to Eqn (2), which is given in
the table below.
General Solution of Eqn (2)
Distinct Roots21
, mm xmxm eBeAy 21 +=
Equal Roots00 ,mm
xmeBAxy 0)( +=
Complex Roots iqp )sincos( qxBqxAey px +=
Note that the arbitrary constants have been calledAandB here; other symbols could be
used.
We shall now consider a few examples to illustrate.
Example 3
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Consider the differential equation
d y
dxy
2
2 = , (3)
The A.E. is , which has distinct roots012 =m 1,1=m . Hence, from the table,
is the m
xample 4
xx BeAey += ost general solution of (3).
E
olve the differential equationS
0652
2
=+ ydxdy
dx
yd
.
Now the A.E. is , whose roots are0652 =+ mm 3,2=m . Therefore, the general
.
Example 5
solution is
xx BeAey32 +=
differential equationConsider the
0962
2
=+ ydxdy
dx
yd
.
The A.E. gives0962 =+ mm 3,3=m , two repeated roots.
general solution
.
Example 6
Hence the is
xeBxAy 3)( +=
uationSolve the eq
01342
2
=+ ydx
dy
dx
yd
.
The A.E. is given by , whose roots are01342 =+ mm im 32 = . The general solution
.
Obtaining Particular Solutions.
is
)3sin3cos(2 xBxAey x +=
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First we solve the A.E. and obtain the general solution. Using the 2 conditions given, we
then fix the 2 arbitrary constants.
Example 7
Solve the following differential equation
14'19''3 5)0(',1)0(,0 == yyy =yy .
The A.E. is , whose roots are014193 2 = mm 7,32=m . Hence the general solution
is xx
Aey 32
=
No
Be7+ .
w yields1)0( =y 1=+BA .
xxBexy 7)(' 3
2
+
at gives 5732 =+ BA .Ae 7
32= , so th 5)0(' =y
Solving simultaneously fo , we seerA andB that2317
236 , == B .A
Hence our particular solution is
xxeey
7
2317
236 3
2
+=
.
Example 8
ferential equationSolve the dif
6'' 5)0(',2)0(,025'+ yy = = =yyy .
The A.E. is , whose roots are02562 =+ mm im 43 = . The general solution is
by
.
We now determineAandB.
in == A .
, Bexy x ++= on using product rule.
0 ++=
therefore given
)4sin4cos(3
xBxAey x +=
s0cos(2)0(0 += BAey 22)0
So, )4sin4cos2(3 xBxey x +=
Now x ]4sin)83(4cos)64[()('3
xB
5' =]0sin)83(0cos)64[(5)0( BBe
i.e.
y
564 =+B
B41=
Hence, the particular solution is
)4sin4cos2(413 xxey= x .
Activity 2
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Solve the following differential equations:
i)
(i) 02'3'' =+ yyy ;
(i 1)0(',0)0(,04'4'' ===+ yyyyy ;
(,0'5''
(iii) 02'2'' =+ yyy ;
(iv) 06''' =+ yyy ;
(v) )0 1)0(',0 === yyy ;y
(vi) 0 ;'3''2 =+ yyy
(vii) 0'2''4 = yyy ;
(viii) 0'6''5 =+ yy ;
(ix) 1)0(',0)0(,05'4'' ===++ yyyyy ;
2++ kyk .(x) ' =yy 0'2'
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8.4 DIFFERENTIAL OPERATORS
The D-operator
LetDdenote the differentiation operatord
dx . Then
dy
dxDy= , ( ) yD
dx
ydyDDyD
dx
dy
dx
d
dx
yd nn
n
===
= ,,22
2
L .
We can now express our differential equations in terms of theDoperator. Thus Eqn (1)
can be written as
)()( 2 xfycbDaD =++ .
Similarly, the differential equation
xyyy 3sin2'3''5 =+
can be written as
. (*)xyDD 3sin)235(2 =+
Inverse of theD operator
SinceDdenotes differentiation w.r.t.x, its inverse will represent integration w.r.t.x.
In general will mean integrate ntimes w.r.t.x. The symbol may also be written
as
1D
nD 1D
1
D. In general, it is customary to write asmD
1
Dmwhen mis a positive integer.
Thus,
DD D
=
=2
21 1
D
1, i.e., integrate twice.
So,
( )
.246
)(
;62
43213
32
2
===
===
xdx
xxDDxD
xdxxdxxxD
While evaluating , the arbitrary constant of integration may be omitted.)(1 xfD
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Some Properties of theDoperator
We shall denote by a function of theDoperator, e.g., in the above Eqn (*),)(DL
235)( 2 += DDDL .
Symbolically we can write a differential equation in the form)()( xfyDL = ,
or,
).()(
1xf
DLy=
Our task is to find ways of evaluating the RHS for different functions ).(xf
We first consider some properties of the D operator. You can easily verify all these
properties.
(i) ;)()( aLeeDL axax =
(ii) ;)()()]([)( xfaDLexfeDL axax +=
(iii) ;axaLaxDL cos)(cos)(22 =
(iv) ;axaLaxDL sin)(sin)(22 =
(v) ;axaLaxDL cosh)(cosh)(22 =
(vi) .axaLaxDL sinh)(sinh)(22 =
We note that there are no simple formulae for , and the
hyperbolics.
axDLaxDL cos)(,sin)(
Lets see how to use the above properties.
Example 9
(a) Suppose we wish to evaluate . Of course we could do it from
first principles; however, using Property (i), we find that here
xeDD 32 )725( +
725)( 2 += DDDL
and .3=a
447)3(2)3(5)3()( 2 =+== LaL .
Hence, .xx eeDD 332 44)725( =+
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(b) Prove that
( )( ) ( )1432122 233223 ++=+ xxeexDDD xx .
Here,
DDDDL += 23 2)( , . Then, Property (ii)gives2)(,3 xxfa ==
( )( ) ( ) ( ) ( ) 22333223 33232 xDDDeexDDD xx ++++=+
( )( ) ( )( )
( ).14321212216270
12167
23
23
2233
++=
+++=
+++=
xxe
xxe
xDDDe
x
x
x
(c) Evaluate .xDD 7cos)253(2 +
We use Property (iii). We have , and253)( 2 += DDDL 7=a .
We therefore replace by . [ Note: ]2D 27 4972 =
xx
xdx
dx
xDx
xD
xDxDD
7sin357cos145
7cos57cos145
)7(cos57cos145
7cos)5145(
7cos]25)49(3[7cos)253(2
+=
=
=
=
+=+
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8.5 SOLVING THE INHOMOGENEOUS EQUATION
The method of solution of the inhomogeneous equation
)(2
2
xfycdx
dyb
dx
yda =++
consists of 3 parts:
1.Find the Complementary Function Cy
2.Find the Particular Integral Py
3. The general solution is then given by
PC yyy += .
The complementary function (C.F.) is obtained by solving the corresponding
homogeneous differential equation, i.e.,
02
2
=++ ycdx
dyb
dx
yda , or 0)( 2 =++ ycbDaD
as we have done above.
The second step, finding the particular integral (P.I), is the hardest part. The P.I. is
obtained by the following result
)()(
1xf
DLyP = .
The following table summarizes the main results for different forcing functions .)(xf
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Table of Inverse Operator Techniques
1.ax
keDL )(
1, k :constant 0)(
)(aL
aL
ek ax
2. (i) )cos()(
12
baxkDL
+
(ii) )sin()(
12
baxkDL
+
)cos()( 2
baxaL
k+
0)(2 aL
)sin()( 2
baxaL
k+
3. )()(
1xP
DL, where is a)(xP
polynomial of degree m
Expand)(
1
DLin ascending powers ofDby
the Binomial Theorem as far as the term in
. Then operate on .m
D )(xP
4. )()(
1xe
DL
ax )()(
1x
aDLeax
+ [Shift Theorem]
5. )(1
xfmD
dxxfee mxmx )(
6. axre
aD )(
1
K,2,1,
!
=re
r
x axr
7. )cos(1
22 baxk
aD+
+
)sin(1
22 baxk
aD+
+
)sin(2
baxa
kx+
)cos(2
baxa
kx+
We shall now consider a few examples to illustrate.
Example 10
Solve the differential equation
912'5''2 = yyy .In terms of theDoperator, our equation is
9)1252(2 = yDD .
If we compare with the entries in the table, we find that here we need to use the first entry
where
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1252)( 2 = DDDL
9,0 == ka We now find the solution to our equation.
STEP 1. Obtain the Complementary Function .
.
Cy
Now, the A.E. is
01252 2 = mm
4,23= m .
Hence
STEP 2. Find the Particular Integral
rom the table,
xx
C eBeAy42/3 += .
Py
F
4
3
91200
1
91252
1=y2
=
=
DDP
[Putting 0==aD ]
TEP 3. Write down the General SolutionS PC yyy +=
4342/3 += xx eBeAy .
Example 11
Solve the differential equation
.x
eyyy 3410'3'' =+
Now we have
103)( 2 = DDDL
3,4 == ak
5,201032 == mmm A.E.
C.F. is
xxC eBeAy52 += .
P.I. is
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x
x
x
P
e
e
eDD
y
3
2
1
2
3
3
2
10)3(3)3(
4
4103
1
=
=
=
[Putting 3==aD ]
General solution is
xxxeeBeAy 3
2152 ++= .
Example 12
Solve the differential equation
xx eeydx
dy
dx
yd 22
2
5296 =++ .
7)0(',0)0( == yy .Here we note that the forcing function consists of 2 terms, and . To find the
P.I., we use entry 1 of the table twice, and add the results, i.e.,
xe xe 25 2
)5()(
12
)(
1 2xxP e
DLe
DLy += ,
where .
0962
==++ mmm
.F.
22 )3(96)( +=++= DDDDL
A.E. 3 3,
xC eBAxy3)(
+= C
P.I.
xx
xx
xx
P
ee
ee
eD
eD
y
2
81
2
2
2
2
22
5
)32(
5
)31(
2
)5()3(
12
)3(
1
=
+
+
+=
+
++
=
General solution is
xxxeeeBAxy
2
813 5)( ++= .
es ofAandB.We now fix the valu
839
81 050)0( ==+= BBy
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Also, we have on differentiating and simplifying
)]248(8024[)(' 381 eBexy
xx ++= 4 xAe x +
0]818024[0)0('81 =+++= ABy
29= A after putting
Hence, th lutionis
8/39=B .
e Particular So
xxxeeexy
2
813
839
29 5)( ++= .
Example 13
Solve the differential equation
.xyDD 2cos5)1( 2 =++
mm2 01 =++ imA.E.
2
3
21 =
+
=
xBxAey
x
C 2
3
sin2
3
cos
2/
C.F.
We now use entry 2(i)in the table with 0,2,5 === bak . Note we replace only
y . TheDstays as it is.
2D
2ab
xD
x
D
xDD
P
2cos53
1
2cos5
12
1
2cos51
1
2
2y
=
++
=
++
Since the result works only for , the trick is to obtain in the denominator. This is
achieved by multiplying top and bottom by
=
2D 2D 3+D . This then gives
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)2cos32sin2(13
5
2cos)3(13
5
2cos592
3
2cos59
3
2cos53
1
D
xD
yP
+
2
2
xx
xD
xD
xD
+=
+=
+
=
=
=
Hence the General solution is
.13
2cos152sin10
2
3
sin2
3
cos2
1x
xxxBxAey
+
+
=
Example 14
Solve the differential equation
xyDD 3sin4)65( 2 =++ ,
0)0(',0)0( == yy .
A.E.
C.F.
the Particular Integral. We use entry 2(ii) in the table with
.
3,20652 ==++ mmm
xx
C eBAey32 +=
Next, we find
k 0,3,4 === ba
P.I.
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)3sin3cos5(39
2
3sin)35(117
2
3sin49)3(25
35
3sin4925
35
3sin435
1
3sin4653
1
3sin465
1
2
2
2
2
xx
xD
xD
xD
D
xD
xD
xDD
yP
+=
+=
+
=
+
=
=
++=
++=
Hence, the General Solution is
)3sin3cos5(39232 xxeBAey
xx ++= .
We now determine the arbitrary constants.
00)0(3910 =+= BAy ----- (i)
Also,
)3cos3sin5()32()('13
232 xxeBeAxy xx ++=
0320)0('132 =++= BAy -----(ii)
Solving (i)and (ii)simultaneously, we obtain32
1312 , == BA .
Hence, the Particular Solution is given by
)3sin3cos5(3923
3
22
13
12
xxeey xx
+=
.
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Evaluating )()(
1xP
DLwhen is a polynomial of degreem.)(xP
In this case we expand the operator)(
1
DLby the binomial theorem in ascending powers
ofD as far as the term in .mD
If is factorisable, use partial fractions and then expand.)(DL
For this purpose, the following binomial expansions are useful:
( )
( ) L
L
+++++=
++=+
4321
4321
11
11
DDDDD
DDDDD
( )( ) L
L
+++++=++=+
4322
4322
543211
543211
DDDDD
DDDDD
Note that we need to have our expression in the right form before carrying out the
expansion. Thus to expand we must first express it as1)53( +D 1531 )1(5 + D .
Likewise, must first be written as1)72( D 1721 )1(7 D . Also, we must express
as2
)45(
D2
542
)1(5
D and then expand.
Example 15
Evaluate 4
1
1x
D.
Here the degree of the polynomial is 4; we therefore expand1
1
Dup to .4D
).2424124(
)1(
)1(
)1(
1
1
1
234
4432
41
44
++++=
+++++=
=
=
xxxx
xDDDD
xD
xD
xD
L
Note:We just differentiate the previous term as we go along.
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Example 16
Solve the differential equation
323672'3'' xxxyyy +=+ .
A.E. 2,10232 ==+ mmm
C.F. xxC eBeAy2+=
P.I.
]367[23
1 322
xxxDD
yP ++
=
Here the degree of the polynomial is 3, therefore expand up to . Also, the operator is
factorisable and so we split it into partial fractions before expanding. Thus
3D
1
1
2
1
)2)(1(
1
23
12
=
=+ DDDDDD
.
On using the binomial theorem we obtain
)1()( 3216842
132
LL DDDDDD
which simplifies to
)1514128( 32161 DDD +++
Hence, is given byPy
]51864[
)]6(15)66(14
)366(12)367(8[
]367)[1514128(]367[23
1
23
81
232
161
3232
16132
2
+=
+++
+++=
++++=++
xxx
x
xxxxx
xxxDDDxxxDD
Note again, we just differentiate previous brackets, while paying attention to the coefficients of the in
the first brackets.
iD
General Solution: )51864( 23812 +++= xxxeBeAy xx .
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Example 17
Solve the differential equation
9725'3'' 3 +=+ xxyyy .
A.E. immm2
11
232 053 ==+
C.F. ]sincos[2
11
2
112/3 xBxAey x
C +=
P.I.
)972(53
1 32
++
= xxDD
yP .
In this case, the degree of the polynomial is 3, so that we need to expand up to . But
now the operator does not factorize, so that we cant use partial fractions. We therefore
proceed as follows:
3D
L
L
+++=
+
+
=
+=+=
+
32
32
222
12
12
2
625
3
125
4
25
3
5
1
5
3
5
3
5
31
5
1
5
31
5
1)53(
53
1
DDD
DDDDDD
DDDD
DD
Hence, the P.I. is
].6361115450250[
)12()12()76()972(
)972(625
3
125
4
25
3
5
1)972(
53
1
23
625
1
6253
12542
2533
51
3323
2
++=
++++=
+
++=++
xxx
xxxx
xxDDDxxDD
Then, the general solution is given by
]6361115450250[]sincos[ 236251
2
11
2
112/3 ++++= xxxxBxAey x .
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The Shift Theorem
Evaluating )()(
1xe
DL
ax . [Here, ])()( xexf ax=
We use the formula
)()(
1)(
)(
1x
aDLexe
DL
axax +
=
TheDis shiftedto .aD +
Example 18
Evaluate ).(
12
1 32
xe
DD
x
+
Here, ( ) .)(,1,12 32 xxaDDDL ==+=
1
2 1
1
123
2
3
D De x
De x
x x
+ =
( ) 3
2]1)1[(
1x
Dex
+=
3
2
1x
Dex= .
20
5x
ex= (Integrating twice).
Example 19
Solve the differential equation .xexxyy 32 )976(4'5'' +=+
A.E. .0452 =+ mm 4,1= m
C.F. .xxC BeAey4+=
We now need to find the particular integral.
P.I. xP exxDD
y 322
)976(45
1+
+=
Here .976)(,3,45)( 22 +==+= xxxaDDDL
The Shift Theoremgives
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)976(12
)976()1)(2(
1
)976(
2
1
)976(4)3(5)3(
1)976(
45
1
231
31
3
23
2
2
3
2
2
332
2
+
++
=
++
=
+
+
=
++++
=++
xxDD
e
xxDD
e
xx
DD
e
xxDD
eexxDD
x
x
x
xx
We now proceed as for Case 3; we expand the operators by the binomial theorem up to
the term in since we have a 2nd
degree polynomial. Thus2D
[ ]
.8
3
42
1
)1()2/1(3
1
122
11
213
131
+++=
++=
++
L
DD
DDDD
Now,429
2122
2
3)976(8
3
42
1+=+
++ xxxx
DD.
)3(429
2123 += xxey xP .
The general solution is hence given by
)3(4
2921234 +++= xxeBeAey xxx .
Example 20
Solve the equation .0)0(',1)0(,sin2'3'' 2 ===++ yyxeyyy x
A.E. , so that0232 =++ mm 2,1 =m .
xx
C BeAey2 += .
Next we find theP.I. We have here
Then, by the Shift Theorem( ) .sin)(,2,232 xxaDDDL ==++=
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xDD
exeDD
y xx
P sin2)2(3)2(
1sin
23
12
22
2 ++++=
++=
=+ +
eD D
xx22
1
7 12sin
= + +
eD
xx2 1
1 7 12sin (replacing by2D 21 )
( )
=+
=
eD
x
e DD
x
x
x
2
2
2
1
11 7
11 71
121 49
sin
sin
( )= +
e Dx2 11 71
121 49sinx (replacing by )2D 21
( )
( ).cos7sin11170
1
sin711170
1
2
2
xxe
xDe
x
x
=
=
Therefore, the general solution is
170/)cos7sin11(22 xxeBeAey xxx ++= .
We now fix the arbitrary constantsAandBby using the given data .0)0(',1)0( == yy
1170/71)0( =+= BAy . ----(i)
Now, , so that170/)cos3sin29(2)(' 22 xxeeBAexy xxx +=
0170/320)0(' == BAy . -----(ii)
Solving (i) and (ii) simultaneously forAandB, we obtain 17/18,170/357 == BA .
Hence, the particular solution is
( )}cos7sin11{180357170
1 22 xxeeey xxx += .
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Forcing Function Consisting of Several Functions
When the forcing function consists of several terms, the P.I. is given by the sum of
the P.I.s of each term. Thus,
)(xf
)]([)(
1)]([
)(
1)]([
)(
1)]()()([
)(
1xr
DLxq
DLxp
DLxrxqxp
DL++=++ .
Example 21
Evaluate ]2sin[23
1 3322
xexeDD
xx +++
.
Letting ]2sin[23
1 3322
xexeDD
y xxP +++= , we have 321 yyyyP ++= , where
)cos7sin11(170
1]sin[
23
1 2221
xxexeDD
y xx =++
= ,
xxee
DDy 33
22 2
1][
23
1 =++
= ,
445
2212
2933
23]2[
231 +=
++= xxxx
DDy .
Hence,
4
45
2
21
2
9
2
1)cos7sin11(
170
1 2332 ++= xxxexxey xxP .
SPECIAL CASES
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ofax
keDL )(
11. Evaluation when 0)( =aL
In this case we can proceed in two ways. One is to use the Shift theorem, the other is to
use Case 6 in the table.
Example 22
Lets find the P.I. for the equationx
eyyy252'3'' =++ .
x
x
P
eDD
eDD
y
2
2
2
5)1)(2(
1
523
1
++=
++=
Clearly, the denominator is zero when we replace D by 2 . We therefore proceed as
by in the factor
follows.
ReplaceD only. We then have2 )1( +D
x
P eD
y25
)1)(2(
1=
+ ------ (#)
Now we use the Shift Theorem with . So theDis shifted to . Thus)2( D5)( =x
.5
)5(
)5(1
5
)1](2)2[(
1
2
2
2
2x
x
x
x
P
xe
xe
De
D
=
=
=+
[Recall means Integrate]
Hence the P.I. is .
lternatively, we can use Result 6 in the table to Eqn. (#) above, where
ey =
D/1
xxe 25
A 1=r . This
yields againx
P xey25 = .
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2. Evaluation of )cos()(
12
baxkDL
+ and )sin()(
12
baxkDL
+ when 0)( 2 =aL
We use Result 7 in the table.
Example 23
To find the P.I of the equation xyy 2cos34'' =+ , we proceed as follows:
xx
xx
xD
yP
2sin
2sin)2(2
3
2cos34
1
4
3
2
=
=
+=
[Using Result 7 with 0,2,3 === bak ]
Activity 3
Solve the following differential equations:
(i) ;725'6'' 3 =++ xeyyy
(ii) ;18)0(',1)0(,549'' 3 === yyeyy x
(iii) ;xyy cosh2''' =
(iv) ;xeyy 28'4'' =
(v) ;xyy 2sin'' =+
(vi) ;xyyy 4sin1006'5'' =+
(vii) xxyyy sin16cos4825'8'' =++ ;
(viii) ;xxyyy 20cos4020sin401'2'' +=++
(ix) ;0)0(',0)0(,''
3
===+ yyxyy(x) ;xeyy x 2sin'2'' =+
(xi) ;24876442''' xxyyy =
(xii) ;18549'6'' +=+ xyyy
(xiii) 1)0(',2)0(,cos4'' ===+ yyxyy .
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8.6 SUMMARY
In this unit, you have studied how to solve homogeneous linear second-order ordinary
differential equations and inhomogeneous equations by finding the complementary
functions and particular integrals usingD-operators.
8.7 ANSWERS TO ACTIVITIES
Activity 1
(i) ;xy = 5
(ii) ;12 += xy
(iii) ;1+=xy
(iv) ;2/)5( xy =
(v) BAxxxy ++= 2365 ;
(vi) BAxxxxy ++++= 22sinh2cosh3 ;
(vii) 3212
212 xxxey x += ;
(viii) ;2/)711(3 xxxy +=
Activity 2
(i) ;xx
BeAey2+=
(ii) ;xxey 2=
(iii) ;)sincos( xBxAey x +=
(iv) ;xx BeAey 32 +=
(v) )4( 551 xey += ; (vi) ;2/xx BeAey +=
(vii) )4/5sin4/5cos(4/ xBxAey x += ;
(viii) ;5/6x
BeAy +=
(ix) ;xey x sin2=
(x)kx
eBxAy += )( .
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Activity 3
(i)573
1615 ++= xxx eBeAey ;
(ii) ;
xx
eexy
33
2)91(
+=(iii) xx exCexBAy ++++= )()(
21
21 ;
(iv) xx eBAey 2324 ++= ;
(v) xxBxAy 2sinsincos31+= ;
(vi) ;xxBeAey xx 4sin24cos432 ++=
(vii) ;xxBxAey x cos2)3sin3cos(4 ++=
(viii) ;xxBxAey x 20sin)20sin20cos( ++=
(ix) ;xxxy sin663 +=
(x) xeBeAy xx 2sin512 += ;
(xi) ;51424 22 +++= xxBeAey xx
(xii) ;66)( 3 +++= xeBxAy x
(xiii) .xxxy sin)12(cos2 +=