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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 +=