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Bab 2 Transformasi Laplace mathematician and astronomer Pierre-Simon Laplace 1
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TRANSFORMASI LAPLACE

Sep 30, 2015

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TRANSFORMASI LAPLACE TABEL
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  • Bab 2 Transformasi Laplacemathematician and astronomer Pierre-Simon Laplace*

  • Transformasi Laplace,Definisi : Misalkan f(t) fungsi yang ditentukan untuk semua t yang positip, maka Transformasi Laplace dari f(t) adalah dan ditulis:

    L [f(t)]*

  • Transformasi LaplaceIVP = initial value problem (kondisi awal)*

  • Contoh*

  • L{A sin t}= A

    Contoh>fungsi sinusoidal*

  • Transformasi dari t n*

  • *Tabel Laplace (rekap)

    f(t)F(s)1(t)1Impulsa satuan21(t)tangga satuan3t4e-at5t. e-at6Sin t7Cos t

  • Tabel Laplace (lanj) *

    8tn (n=1, 2, 3, ..)9tn. e-at (n=1, 2, 3, ..)10e-at sin t

  • TurunanSifat2/Teorema TL*

  • Integral, S shifting, T shifting*Sifat2/Teorema TL

  • T Shiting, Convolution, Period*Sifat2/Teorema TL

  • Theorem.*The final value theorem is useful because it gives the long-term behaviour without having to perform partial fraction decompositions or other difficult algebra. If has poles in the right-hand plane or on the imaginary axis,on contrary if one pole is present on the imaginary axis atmost then Final Value theorem can be applied. (e.g., if or ) the behaviour of this formula is undefinedInitial value theorem:

    Final value theorem:

    if all poles of sF(s) are in the left half-plane

    First Shifting TheoremL{eatf(t)}=F(s+a)Second Shifting TheoremL{u(tc)g(tc)}=ecsG(s)

  • Sifat-sifat/Teorema Transformasi Laplace*

  • (ii)L{ a f1(t) + b f2(t) } = a L{ f1(t) } + b L{ (t) } Bila L{ f (t) } = F ( s ) maka :(iii) L{ e at f(t) } = F ( s a )

    (iv)L{ tn f(t) } = (-1)n

    (v)L{ f(t) } =

    *

  • Soal-soal12*

  • *

  • *

  • *

  • Unit Step FunctionEC&S CHAPTER 2L{u(t)}=sin(wt)01time u(t)0time sin(wt)u(t)Useful for representing sudden changese.g. application of sinusoid at t = 0*

  • Unit Impulse FunctionEC&S CHAPTER 2Mathematical representation of short burst of input (lightning, hammer blow, etc.)Exact shape unimportant if duration short relative to effectsL{d(t)} = = 1Impulse functions sometimes used to test system dynamics*

  • Transformasi LaplaceX(s) = L[x(t)]x(t) = L-1[X(s)]*

  • Inverse Transformasi LaplacePecahan Parsial X(s)dimana derajat P(s) < derajat Q(s)Jika X(s) berbentuk pecahan parsial yang pembilang dan penyebutnya berbentuk polinomial

    *

  • Akar-akar Q(s) berbeda, tidak ada yang samax(t) menjadi :Kasus-kasus yang sering dijumpai*

  • Q(s) mempunyai akar rangkap (berulang)*

  • Jika pi = pk*, maka penyelesaian dapat diselesaikan secara khusus yang menghasilkan x(t) merupakan fungsi Cosinus dan Sinusx(t) menjadi :*Q(s) difaktorkan menjadi

    Uraiannya

  • *A1 dan A2 diperoleh dari pers berikut,x(t) menjadi,

  • Contoh1*

  • 2*

  • 3*

  • *

  • *Soal soal Latihan

    *Transformasi Laplace* **