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    CHAP. 51

    FOURIER ANALYSIS OF TIME SIGNALS AND SYSTEMS

    Table

    5 2.

    Common Fourier Transforms airs

    sin t

    5 5

    THE FREQUENCY RESPONSE OF CONTINUOUS TIME LTI SYSTEMS

    A.

    Frequency Response:

    In Sec. 2.2 we showed tha t th e ou tput

    y t )

    of a continuous-time LTI system equals the

    convolution of the input

    x t )

    with the impulse response

    h t ;

    that is

    Applying th e convolution property

    5.58),

    we obtain

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    FOURIER ANALYSIS OF DISCRETE TIME SlGNALS

    AND

    SYSTEMS

    [CHAP.

    6

    Table

    6 2.

    Common Fourier Transform Pairs

    s n

    n

    o

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    CHAP.

    6

    FOUR IER ANALYSIS OF DISCRETE-TIME SIGNALS AND SYSTEMS

    Table

    6 1.

    Properties of the ourier Transform

    Property Sequence Fou rier transform

    Periodicity

    Linearity

    Tim e shifting

    Frequency shifting

    Conjugat ion

    Tim e reversal

    Tim e scaling

    Frequ ency differentiation

    First difference

    Accumulation

    Convolution

    Multiplication

    Real sequence

    Even component

    Odd component

    Parseval s r elations

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    CHAP. 3

    LAPLACE TRANSFORM AN D CONTINUOU S-TIME LTI SYSTEMS

    Table

    3 1

    Som e Laplace Transforms Pairs

    All s

    cos wotu t)

    sin wotu t

    s a

    e- '

    cos wotu t)

    Re s ) Re a )

    s + a 1 2 + w ;

    A.

    Linearity:

    I f

    The set notation

    A

    B

    means that set

    A

    contains set

    B,

    while A

    n

    B

    denotes the

    intersection of sets A and B, that is the set containing all elements in both A and B.

    Thus Eq

    3 . 15 )

    indicates that the

    ROC

    of the resultant Laplace transform is at least as

    large as the region in common between

    R ,

    and

    R 2 .

    Usually we have simply

    R R ,

    n

    R , .

    This is illustrated in Fig. 3-4.

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    CHAP. 31

    LAPLACE TRANSFORM AND CONTINUOUS-TIME LTI SYSTEMS

    Table 3 2 Properties of the Laplace Transform

    Property Signal Transform ROC

    x ( t ) X ( s ) R

    x , ( t ) x , w R

    x 2 W x , w R2

    Linearity

    a , x , ( t )

    +

    a 2 x 2 ( l )

    a ,X , ( s )

    +

    a , X 2 ( s) R ' I R , n R 2

    Time shifting

    x ( t o ) e - X ( s )

    R' R

    Shifting in

    s

    es 'x( X ( s o) R' R Re (s , )

    Time scaling x( a t - X ( s ) R' aR

    la

    Time reversal R ' =

    - R

    Differentia tion in

    Differentia tion in s x ( t )

    d X( s )

    R f = R

    ds

    Integration

    Convolution

    then

    % ( t )

    ~ 2 0 ) X I ~ ) X ~ ~ ) R ' I R , n R 2 ( 3 . 2 3 )

    Th is convolution p roperty plays a central role in th e analysis and design of continuous-time

    LTI systems.

    Table 3 2 summarizes the properties of the Laplace transform presented in this

    section.

    3 5 THE INVERSE LAPLACE TRANSFORM

    Inversion of the Laplace transform to find the signal

    x ( t )

    from its Laplace transform

    X s) is called the inverse Laplace transform, symbolically denoted as

    A Inversion Formula:

    There

    is

    a procedure that is applicable to all classes of transform functions that

    involves the evaluation of a line integral in complex s-plane; that is,

    In this integral, th e real c is to be selected such that if th e ROC of X s) is

    a

    Re s )

    < a 2

    then a < c

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    TH E Z-TRANSFORM AND DISCRETE-TIME LTI SYSTEMS

    [CHAP.

    4

    Thus,

    [n] all

    B.

    Unit Step Sequence

    d n l :

    Setting a in Eqs. ( 4 . 8 ) to (4.101, we obtain

    C.

    z Transform Pairs:

    Th e z-transforms of some common sequences are tabulated in Table 4-1.

    Table 4 1. Some Common z Transform Pairs

    All z

    lzl

    >

    1

    Iz l< 1

    Z- '

    All z except 0 if

    m

    >

    0) r m if

    m

    0)

    Z

    1 - a z - ' ' 2 - a

    Izl

    >

    lal

    z 2 COS o ) z

    (COS on)u[n l

    z 2 2 co s R o )t

    1

    l z l >

    (sin n o )

    (sin R,n)u[ n]

    z 2 ( 2cos R , ) z 1

    Iz l>

    z 2 r c o s R 0 ) z

    ( r n cos R,n)u[n]

    z 2 2 r cos R o ) z r 2

    Izl> r

    ( r sin R , )z

    r n

    in R,n)u[nI

    z 2 2 r co s R , ) z r 2

    Iz l>

    r

    O < n s N - 1 1 ~ ' z - ~

    otherwise az- '

    lz l> 0

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    CHAP. 41 T H E Z-TRANSFORM AND DISCRETE-TIME LTI SYSTEMS 173

    Table

    4 2.

    Some Properties of the z Transform

    Property Sequence Transform RO C

    Linearity

    Tim e shifting

    Multiplication by

    z,

    Multiplication by

    einon

    Tim e reversal

    Multiplication

    by n

    Accumulation

    Convolution

    ( z )

    2

    d ?

    H. Summary of Some z transform Properties

    For convenient reference, the properties of the z-transform presented above are

    summarized in Table

    4-2.

    4 5

    THE

    INVERSE Z TRANSFORM

    Inversion of the z-transform to find the sequence x n ] from its z-transform X ( z ) is

    called th e inverse z-transform , symbolically den oted as

    ~ [ n ]s - ' { X ( z > } ( 4 . 2 7 )

    A.

    Inversion Formula:

    As in the case of the Laplace transform, there is a formal expression for the inverse

    z-transform in terms of an integration in the z-plane; that is,

    where C is a counterclockwise contour of integration enclosing the origin. Formal

    evaluation of

    Eq

    (4.28 ) requires a n un derstanding of com plex variable theory.

    B.

    Use of Tables of z Transform Pairs:

    In th e second method for the inversion of X (z ), we attem pt to express X (z ) as a sum

    X ( z ) = X , ( z )

    .

    +X,(z) (4 .29)