Maths II Formulas

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    Engineering Mathematic-II

    UNIT-I

    ORDINARY DIFFERENTIAL EQUATIONS:

    2 3 2

    ( ) ( )

    ( ) ; ( ) , , , , tan

    D y f x

    D is aD bD c or aD bD cD d where a b c d are cons ts

    =

    + + + + +

    1. ODE with constant coefficients: Solution C.F+P.Iy =

    Complementary functions: (C.F.)

    Sl.No. Nature of Roots C.F

    1.1 2m m= ( )

    mxAx B e+2.

    1 2 3m m m= = ( )2 mxAx Bx c e+ +3.

    1 2m m 1 2m x m xAe Be+

    4.1 2 3m m m 31 2

    m xm x m xAe Be Ce+ +

    5.1 2 3,m m m= 3( )

    m xmxAx B e Ce+ +

    6. m i = ( cos sin )xe A x B x +

    7. m i= cos sinA x B x +

    Particular Integral: (P.I.)

    Type-I

    If ( ) 0f x =

    then, P.I = 0.

    Type-II

    If ( )ax

    f x e=1

    .( )

    axP I ea

    =

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    Replace D by a. If ( ) 0a , then it is P.I. If ( ) 0a = , then diff. denominator

    w.r.t D and multiply x in numerator. Again replace D by a. If you get denominator again

    zero then do the same procedure.

    Type-III

    Case: (i) If ( ) sin ( ) cosf x ax or ax=

    1. sin (or) cos

    ( )P I ax ax

    D=

    Here you have to replace only 2D not D. 2D is replaced by2a . If the

    denominator is equal to zero, then apply same procedure as in Type-II.

    Case: ii If 2 2 3 3( ) (or) cos (or) sin (or) cosf x Sin x x x x=

    Use the following formulas2 1 cos 2

    2

    xSin x

    = ,

    2 1 cos 2cos2

    xx

    += ,

    ( )31

    sin 3sin sin 34

    x x x= , ( )31

    cos 3cos cos34

    x x x= + and separate 1 2. & .P I P I

    Case: iii If ( ) sin cos ( ) cos sin ( ) cos cos ( ) sin sinf x A B or A B or A B or A B=

    Use the following formulas:

    ( )

    ( )

    ( )

    ( )

    1( ) in cos ( ) sin( )2

    1(ii) cos sin ( ) sin( )

    2

    1( ) cos cos cos( ) cos( )

    2

    1( ) sin sin cos( ) cos( )

    2

    i s A B sin A B A B

    A B Sin A B A B

    iii A B A B A B

    iv A B A B A B

    = + +

    = +

    = + +

    = +

    Type-IV

    If ( ) mf x x=1

    .( )

    mP I xD

    =

    1

    1 ( )

    mxg D

    =+

    ( )1

    1 ( ) mg D x

    = +

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    Here we can use Binomial formula as follows:

    i) ( )1 2 31 1 ...x x x x

    + = + +

    ii) ( )

    1 2 3

    1 1 ...x x x x

    = + + + +

    iii) ( )2 2 31 1 2 3 4 ...x x x x

    + = + +

    iv) ( )2 2 31 1 2 3 4 ...x x x x

    = + + + +

    v)3 2 3(1 ) 1 3 6 10 ...x x x x+ = + +

    vi)3 2 3(1 ) 1 3 6 10 ...x x x x

    = + + + +

    Type-V

    If ( )axf x e V= where sin ,cos , mV ax ax x=

    1.

    ( )

    axP I e VD

    =

    Take out axe and replace D by D+a.

    1

    ( )

    axe VD a

    =+

    Type-VI

    If ( )nf x x V= where sin ,cosV ax ax=

    sin I.P of

    cos R.P of

    iax

    iax

    ax e

    ax e

    =

    =

    1. ODE with variable co-efficients : (Eulers Method)

    The equation is of the form2

    2

    2( )

    d y dyx x y f x

    dx dx+ + =

    Implies that2 2( 1) ( )x D xD y f x+ + =

    To convert the variable coefficients into the constant coefficients

    Put logz x= implies zx e=

    2 2

    3 3

    ( 1)

    ( 1)( 2)

    xD D

    x D D D

    x D D D D

    =

    =

    =

    whered

    Ddx

    = andd

    Ddz

    =

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    The above equation implies that ( )( 1) 1 ( )D D D y f x + + = which is O.D.E

    with constant coefficients.

    2. Legendres Linear differential equation:

    The equation if of the form2

    2

    2( ) ( ) ( )

    d y dyax b ax b y f x

    dx dx+ + + + =

    Put Z = log( )ax b+ , then ( ) zax b e+ =

    2 2 2

    3 3 3

    ( )

    ( ) ( 1)

    ( ) ( 1)( 2)

    ax b D aD

    ax b D a D D

    ax b D a D D D

    + =

    + =

    + =

    whered

    Ddx

    = andd

    Ddz

    =

    UNIT-II

    VECTOR CALCULUS:

    1. Vector differential operator is / / /i x j y k z = + +

    2. Gradient of / / /i x j y k z = = + +

    3. Divergence ofF 31 2

    1 2 3,FF F

    F where F F i F j F kx y z

    = = + + = + +

    rr r r rg

    4. Curl of F

    1 2 3

    / / /

    i j k

    XF x y z

    F F F

    = = r

    5. If F is a Solenoidal vector then 0F =g

    6.

    7. If F is an Irrotational vector, then 0XF =

    8. Maximum Directional derivative =

    9. Directional derivative of in the direction of a aa

    = gr

    10. Angle between two normals to the surface1 2

    1 2

    cosn n

    n n =

    gr r

    Where ( )1 1 1

    1 1 ( , , )at x y z n = & ( )

    2 2 22 2 ( , , )at x y z

    n =

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    11. Unit Normal vector, n

    =

    12. Equation of the tangent plane 1 1 1( ) ( ) ( ) 0l x x m y y n z z + + = at 1 1 1( , , )x y z on

    the surface ( , , ) 0x y z = . Here l, m, n are coefficients of , ,i j k in .13. Equation of normal line

    1 1 1x x y y z z

    l m n

    = =

    14. Work Done =C

    F dr g , where dr dxi dyj dzk = + +r

    15. If .C

    F drr

    is independent of the path then curl 0F =

    16. In the surface integral,.

    dxdydSn k

    = r , .dydzdSn i

    = r , .dzdxdSn j

    = r & dS ndS =

    17. Greens Theorem:

    If , , ,u v

    u vy x

    are continuous and one-valued functions in the region R enclosed

    by the curve C, thenC R

    v uudx vdy dxdy

    x y

    + =

    .

    18. Stokes Theorem:

    Let F be the vector point function, defined over an open surface bounded by a

    closed curve C, then ( ) xC S

    F dr F nds= r

    g g

    19. Gauss Divergence Theorem:

    Let F be a vector point function in a region R bounded by a closed surface S,

    then S V

    F nds Fdv= g g

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    UNIT-III

    ANALYTIC FUNCTIONS:

    1. Necessary conditions for f(z) to be an analytic function are the

    Cauchy Riemann Equations; &u v u v

    x y y x

    = =

    (OR)

    X Y Y XU V and U V = = (C-R equations)

    2. The Polar form of Cauchy-Riemann Equations:1 1

    &u v v u

    r r r r

    = =

    3. The function u(x,y) is said to be harmonic if it satisfies the

    Laplace equation :

    2 2

    2 2 0u u

    x y

    + =

    4. If the function is harmonic then it should be either real or imaginary part of some

    analytic function.

    5. Milne Thomson method: for (finding the analytic function f(z) if the real or

    imaginary part is given

    i) If u is given ( ) ( ,0) ( ,0)x yf z u z dz i u z dz=

    ii) If v is given( ) ( ,0) ( , 0)

    y x

    f z v z dz i v z dz= +

    6. To find the analytic function

    i) ( ) ; ( )f z u iv if z iu v= + = adding these two

    We have ( ) ( ) (1 ) ( )u v i u v i f z + + = +

    then ( )F z U iV= + where , & ( ) (1 ) ( )U u v V u v F z i f z = = + = +

    Here we can apply Milne Thomson method for F(z).

    7. Bilinear transformation is ; 0az b

    w ad bccz d

    +=

    +

    8. The cross-ration of 4 pts( ) ( )

    ( ) ( )1 2 3 4

    1 2 3 4 1 2 3 4

    2 3 4 1

    , , , ( , , , )z z z z

    z z z z is z z z zz z z z

    =

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    9. The cross-ratio is invariant under a bilinear transformation

    ( ) ( )

    ( ) ( )

    ( ) ( )

    ( ) ( )1 2 3 1 2 3

    1 2 3 1 2 3

    w w w w z z z z

    w w w w z z z z

    =

    UNIT-IV

    COMPLEX INTEGRATION:

    1. Cauchys Integral Theorem:

    If f(z) is analytic and ( )f z is continuous inside and on a simple closed curve C,

    then ( ) 0c

    f z dz= .

    2. Cauchys Integral Formula:

    If f(z) is analytic within and on a simple closed curve C and a is any point inside

    C, then( )

    2 ( )C

    f zdz if a

    z a=

    3. Cauchys Integral Formula for derivatives:

    If a function f(z) is analytic within and on a simple closed curve C and a is any

    point lying in it, then( )

    2

    1 ( )( )

    2C

    f zf a dz

    i z a =

    Similarly( )

    3

    2! ( )( )

    2C

    f zf a dz

    i z a =

    , In general

    ( )

    ( )

    1

    ! ( )( )

    2

    n

    n

    C

    n f zf a dz

    i z a+=

    4. Cauchys Residue theorem:

    If f(z) is analytic at all points inside and on a simple closed cuve c, except for a

    finite number of isolated singularities 1 2 3, , ,... nz z z z inside c, then

    { }1 1

    ( ) 2 (sum of the residues of ( )) 2 Re ( ) Re ( )z z z z

    C

    f z dz i f z i s f z s f z = =

    = = + +

    .

    5. Critical point:

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    The point, at which the mapping w = f(z) is not conformal, (i.e) ( ) 0f z = is called

    a critical point of the mapping.

    6. Fixed points (or) Invariant points:

    The fixed points of the transformationaz b

    w cz d

    +

    = + are obtained by putting w = z

    in the above transformation, the point z = a is called fixed point.

    7. Re { ( )} ( ) ( )z a z a

    s f z Lt z a f z=

    = (Simple pole)

    8. ( )( )1

    1

    1Re { ( )} ( )

    ( 1)!

    mm

    mz a z a

    ds f z Lt z a f z

    m dz

    = =

    (Multi Pole (or) Pole of order m)

    9. Taylor Series:

    A function ( )f z , analytic inside a circle C with centre at a, can be expanded in the

    series

    2 3( )( ) ( ) ( ) ( )( ) ( ) ( ) ( ) ( ) ... ( ) ...

    1! 2! 3! !

    nnz a z a z a z af z f a f a f a f a f a

    n

    = + + + + + +

    Maclaurins Series:

    Taking a = 0, Taylors series reduce to

    2 3

    ( ) (0) (0) (0) (0) ...

    1! 2! 3!

    z z zf z f f f f = + + + +

    10. Laurents Series:0 1

    ( ) ( )( )

    n nn n

    n n

    bf z a z a

    z a

    = =

    = +

    The part1 ( )

    n

    nn

    b

    z a

    = is called the Principal part

    where1

    1

    1 ( )

    2 ( )n n

    C

    f za dz

    i z a +=

    &2

    1

    1 ( )

    2 ( )n n

    C

    f zb dz

    i z a =

    , the integrals being

    taken anticlockwise around 1 2C and C .

    11. Isolated Singularity:

    A point 0z z= is said to be an isolated singularity of ( )f z if ( )f z is not analytic

    at 0z z= and there exists a neighborhood of 0z z= containing no other singularity

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    of f(z). Example:1

    ( )f zz

    = . This function is analytic everywhere except at

    0z= . 0z = is an isolated singularity of f(z).

    12. Removable Singularity:

    A singular point 0z z= is called a removable singularity of ( )f z if0

    lim ( )f z

    z z

    exists finitely.

    Example:

    sinlim ( ) lim 1

    0 0

    zf z

    z

    z z

    = =

    (finite) 0z = is a removable

    singularity.

    13. Essential Singularity:

    If the principal part contains an infinite number of non zero terms, then 0z z= is

    known as an essential singularity.

    Example:( )

    21 1/1/( ) 1 ...

    1! 2!z

    zzf z e= = + + + has 0z= as an essential

    singularity.

    CONTOUR INTEGRATION:

    14. Type: I

    To evaluate the integrals of the form2

    0(cos ,sin )f d

    Here we shall choose

    the contour (closed curve) as the unit circle : 1, ,0 2iC z Put z e = = .

    Then2 1

    cos2

    z

    z

    += ,

    2 1sin

    2

    z

    iz

    = and

    1d dz

    iz = .

    15. Type: II

    To evaluate integrals of the form

    ( )

    ( )

    P x

    dxQ x

    , Here P(x) and Q(x) are polynomials

    in x such that the degree of Q exceeds that of P at least by two and Q(x) does not

    vanish for any x. Choose the closed curve C consisting of the following parts.

    (i) the semi circle : Z R = in the upper half plane.

    (ii) The line segment [-R, R] on the real axis.

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    Here ( ) ( ) ( )R

    C R

    f z dz f x dx f z dz

    = + as ( ) 0R f z dz

    = .

    Where,( )

    ( )( )

    P zf z

    Q z=

    16. Type: III

    The integrals of the form ( )cos (or) ( )sinf x mxdx f x mxdx

    where

    ( )( )

    ( )

    P xf x

    Q x= as in Type II.

    Use cos . . , sin . .imx imxmx R P of e mx I P of e= = Proceed as in Type II.

    UNIT-V

    LAPLACE TRANSFORM:

    1. Definition:

    [ ] 0( ) ( )stL f t e f t dt

    =

    2.

    Sl.No Nature of Roots C.F

    1. [ ]1L1

    s

    2.nL t 1 1

    ! ( 1)n n

    n n

    s s+ +

    +=

    3.at

    L e 1

    s a

    4. atL e 1s a+

    5. [ ]sinL at 2 2a

    s a+

    6. [ ]cosL at 2 2s

    s a+

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    7. [ ]sinhL at 2 2a

    s a

    8. [ ]coshL at2 2

    s

    s a

    3. Linear Property: [ ] [ ] [ ]( ) ( ) ( ) ( )L af t bg t aL f t bL g t =

    4. First Shifting property:

    If [ ]( ) ( )L f t F s= , then

    i) [ ]( ) ( )at

    s s aL e f t F s = = F(s-a)

    ii) [ ]( ) ( )ats s a

    L e f t F s +

    = = F(s+a)

    5. Second Shifting property:

    If [ ]( ) ( )L f t F s= ,( ),

    ( )0,

    f t a t ag t

    t a

    >=

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    10. Final value Theorem:

    If [ ]( ) ( )L f t F s= , then( ) ( )

    s 0

    Lt f t Lt sF s

    t

    =

    11.

    Sl.No

    1.1 1L

    s

    1

    2.1 1

    Ls a

    ate

    3.1 1L

    s a

    +

    ate

    4.1

    2 2

    sL

    s a

    +

    cos at

    5.1

    2 2

    1L

    s a

    +

    1sin at

    a

    6.1

    2 2

    sL s a

    cosh at

    7.1

    2 2

    1L

    s a

    1sinh at

    a

    8.1 1

    nL

    s

    1

    ( 1)!

    nt

    n

    12. Deriative of inverse Laplace Transform:

    [ ] [ ]1 11

    ( ) ( )L F s L F s

    t

    =

    13. Colvolution of two functions:0

    ( ) ( ) ( ) ( )t

    f t g t f u g t u du = 14. Covolution theorem:

    If f(t) & g(t) are functions defined for 0t then [ ] [ ] [ ]( ) ( ) ( ) ( )L f t g t L f t L g t =

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    15. Convolution theorem of inverse Laplace Transform:

    [ ]1

    0

    ( ) ( ) ( ) ( )

    t

    L F s G s f u g t u du =

    16. Solving ODE for second order differential equations using L.T

    i) [ ] [ ]( ) ( ) (0)L y t sL y t y =

    ii) [ ] [ ]2( ) ( ) (0) (0)L y t s L y t sy y =

    iii) [ ] [ ]3 2( ) ( ) (0) (0) (0)L y t s L y t s y sy y =

    17. Laplace Transform:

    If f(x+T) = f(x), then f(x) is said to be a of Periodic function with period T.

    For such a periodic function, the Laplace Transformation is given by

    [ ]0

    1( ) ( )

    1

    Tst

    sTL f t e f t dt

    e

    =