LDEofOrder1

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    Linear Differential Equationsof Order One

    Chapter 2

    Reference: DE by R. Marquez

    1

    First Order First Degree ODEs

    A special class of first-order ordinary Des which is

    generally a nonexact DE with special integrating

    factor is a linear differential equation.

    A linear DE of order one takes the form .

    )()( xQxyPdx

    dy dxxQdxxyPdy )()(

    Derivative form

    Differential form

    dxxpexv )()(Whose integrating factor, v(x)

    2

    The General Solution

    The general solution of

    Is found by multiplying the integrating factor,

    v(x) to each term and then solving for theexact DE formed.

    3

    )()( xQxyPdx

    dy

    dxxPdxxP edxxQdxxyPdye )()( )()(

    dxxQeyeddxxPdxxP

    )()()(

    dxxQedxxPyedyedxxPdxxPdxxP

    )()()()()(

    The General Solution

    Simplify the equation using

    Integrating both sides will result to

    Thus, the general solution is

    4

    dxxQxvxyvd )()()(

    dxxpexv )()(

    dxxQxvxyvd )()()(

    CdxxQxvxyv )()()(

    CdxxQxvxvy )()()( 1

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    The General Solution

    It is also possible that the given DE is not linear

    in ybut instead linear in other variable.

    Linear DE iny:

    Linear DE in x:

    . Linear in w:

    5

    CdxxQxvxvy )()()( 1

    CdyyQyvyvx )()()( 1

    CdttQtvtvw )()()( 1

    )()( xQxyPdx

    dy

    )()( yQyxPdy

    dx

    )()( tQtwPdt

    dw

    Example: Find the general solution

    6

    xxxydx

    dycossin4cos2)3 2

    xxyy cos2cot)1 0)tan(sec)2 3 dyyxydx

    2)1(1

    )4 xxy

    y

    0sectan)5 yywdy

    dw

    xyedy

    dx y sin)6

    Find the particular solution

    when x =1, y = 2

    ify(10) =0

    when x =1, y = 2

    7

    xyyx 212 dyyexdx y )sin4( 2

    xyx

    x

    dy

    dx

    463 3

    2

    The Bernoullis Equation

    8

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    Definition

    A differential equation that can be

    expressed in the form

    is called a Bernoullis equation (BE) in y.

    9

    )()( xQyxyPdxdy n

    Definition

    The BE

    may be made linear upon multiplication of

    and substitution of

    10

    )()( xQyxyPdx

    dy n

    nyn )1(

    dx

    dyyn

    dx

    dzyz nn )1(;1

    The General Solution of BE

    Thus, the BE becomes

    The general solution of this linear DE in

    z may be accomplished by the method

    of linear DE of order one.

    11

    )()1()()1()1( 1 xQnxPnydx

    dyyn nn

    )()1()()1( xQnxPnzdx

    dz

    Example: Solve the following DE

    12

    23)1 xexyxyy Solution

    dxdyy

    dxdzyz 32 2; Let

    Thus, the given DE becomes

    2)13()13( xxezx

    dx

    dz 2

    2)2( xxexzdx

    dz which is linear in z

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    Example: Solve the following DE

    13

    Continuation of Solution of Ex. 1

    So that the integrating factor is2)2( x

    xdxee

    Thus, Cdxexeze xxx ))(2(

    222

    )2(2 Cdxxze x

    Cxez x 22 2 yz22

    2Cxey x

    ,

    2)(1 22 xexCy

    Exercise: Solve the given DEs

    14

    xyxydx

    dy 33 sectan)1 xxyyyx ln)2 3/13/4

    )124(77)3 35 xxxyyyx)1()4 531 yxxy

    dy

    dx

    9

    )52

    2

    xx ee

    yy

    dx

    dy

    7.

    Exercise: Solve the given DEs

    15

    44534)6 yxxy

    dy

    dx 0)tancsc(2)7 2 dvvvwdww

    37)8 yxyyx 4cot)9 xyx

    dy

    dx

    7.

    Differential Equations

    Solvable by Simple

    Substitution

    16

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    Sometimes the DE

    may not be reducible at once to any of

    the forms discussed so far. This meansthat the previous methods even how

    effective they were would not work. But

    if a wise change of variable would be

    done, the equation could be

    transformed into an equation that could

    be well handled by one of the previous

    methods.

    17

    0),(),( dyyxNdxyxMDEs Solvable by Simple Substitution

    Solve the following

    18

    DEs Solvable by Simple Substitution

    021 yxxedx

    dy

    w = x ydx

    dw

    dx

    dy

    dx

    dy

    dx

    dw 11Substituting these to the given DE, we get

    0211 wxedx

    dw

    0202 ww xedx

    dwxe

    dx

    dw

    Continuation of solution

    19

    DEs Solvable by Simple Substitution

    But w = x y

    Variable Separable DE

    02 wxedx

    dw

    02 xdxdwe w02

    xdxdwe w

    Cxe w 2xyyx eCxCxe 22)(

    Solve the following

    20

    7.

    0)733()4( dyyxdxyx0)74( 2 yx

    dx

    dy

    0)tan3(sec)3(tan 222 dyyxxdxyx 0tan25cos3 2 dyyxdxxyx

    021 yxxedx

    dy

    xxyxdy

    dxy ln)1(ln

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    Solve the following

    21

    7.

    021 1

    xdx

    dyey

    0tan])(tan1)[(tan 222 ydydxeyyyyx x

    DES WITH COEFFICIENTS

    LINEAR IN TWO VARIABLES

    22

    DE w/ Coefficient Linear in Two Variables Consider the DE whose form is

    (1)

    It is noted that the coefficients ofdxand dyare both linear in the variables xandy. If

    these coefficients are each equated to zero,

    we obtain two equations of the lines of the

    forms

    and

    23

    0)()( 222111 dycybxadxcybxa

    0111 cybxa0222 cybxa

    DE w/ Coefficient Linear in Two Variables For these associated equations of the lines,

    we consider the following three cases:

    Case 1: If

    then the graph of the associated equations

    of the lines are coincident and the DE is

    reducible to

    kdx + dy = 0 , k is a constant (2)

    24

    0111 cybxa 0222 cybxa

    2

    1

    2

    1

    2

    1

    c

    c

    b

    b

    a

    a

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    DE w/ Coefficient Linear in Two Variables Case 2: If

    then the graph of the associated equationsof the lines are parallel and the DE is

    reducible to

    which can be handled by simple substitution.

    25

    2

    1

    2

    1

    2

    1

    c

    c

    b

    b

    a

    a

    0)()( 222122 dycybxadxcybxak

    DE w/ Coefficient Linear in Two Variables Case 3: If

    then the associated lines are intersecting

    and the DE is reducible to homogeneous

    DE using the substitution

    x = u + h ; dx = du

    y = w + k ; dy = dw

    where (h, k) is the point of intersection of

    the linear system

    26

    2

    1

    2

    1

    b

    b

    a

    a

    0

    0

    222

    111

    ckbha

    ckbha

    DE w/ Coefficient Linear in Two Variables In case the DE falls under case 3, try also to

    check if it is an exact DE. If so, it is

    suggested to use the method for exact DE

    since it is much easier to perform.

    27

    Example1) Find the general solution of(x+ 2y + 6)dx

    (2x+y )dy = 0

    Solution

    For the associated system of linear equations, wehave

    The solution point of this is (h, k) = (2, 4)

    If we let x= u + 2 ; dx = du and

    y = w 4 ; dy = dw

    then, upon substitution we obtain

    (u +2w)du (2u +w)dy =0.28

    02

    062

    kh

    kh

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    ExampleContinuation:

    This is a homogeneous DE with

    u = zw ; du = zdw + wdz

    Then, by substitution, we get

    (zw +2w) (zdw + wdz) (2zw + w)dw =0

    (z +2) (zdw + wdz) (2z +1)dw =0

    (z2 +2z 2z 1)dw + w(z +2)dz =0

    (z2 1)dw + w(z +2)dz =0

    29

    01

    22

    dz

    z

    z

    w

    dw

    Example

    30

    11

    23

    1

    21 Cdz

    zzw

    dw

    12321 |1|ln|1|ln||ln Czzw 1

    32

    21

    )1(ln C

    z

    zw

    1232

    1

    )1( Cez

    zw

    C

    y

    yx

    yx

    1

    1)4(

    42

    3

    422

    )2()6( 3 yxCyx

    Exercise

    Solve the following differential equations.

    1. (3x + y 8)dx + (x2y +2)dy =0

    2. (16x +5y 6)dx + (3x + y 1)dy =0

    3. (xy

    2)dx + (3x + y

    10)dy =0

    4. (2x +3y +3)dx + (3x4y +13)dy =0

    5. (3x + y 9)dx + (x4)dy =0

    6. (x + y +1)dx + (xy 5)dy =0

    7. (6x + y 9)dx + (x2y +5)dy =0

    8. (y 1)dx2(x + y +1)dy =0

    9. (3x + y 10)dx + (x +3y +2)dy =0

    10.(7x + y 8)dx + (x2y +5)dy =031