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MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE 1

MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

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Page 1: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

MATERI 3

MATEMATIKA TEKNIK 1

PEMETAAN LAPLACE

1

Page 2: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

Kawasan Waktu Vs Kawasan Frekuensi

2

Page 3: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

Kawasan Waktu Vs Kawasan Frekuensi

3

Page 4: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

Kawasan Kompleks4

Page 5: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

Pemetaan Laplace

Introduction

The solution of most electrical circuit problems can be

reduced ultimately to the solution of differential equations.

The use of Laplace transforms provides an alternative

method to those discussed in first and second order

differential equations for solving linear differential

equations.

5

Page 6: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

Laplace Notation

6

Page 7: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

Pendahuluan

7

Pemetaan Laplace didefinisikan sebagai berikut :

dengan fungsi f(t) terdefinisi untuk seluruh t≥0

Contoh 1.

Tentukanlah pemetaan Laplace dari f(t) = 1

Jawab.

Page 8: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

Tujuan8

Setelah mempelajari Pemetaan Laplace maka diharapkan :

1. Dapat memetakan suatu fungsi dalam kawasan waktu (t)

kekawasan kompleks (s).

2. Dapat memetakan balik (Invers) dari kawasan kompleks (s)

kekawasan waktu (t).

3. Dapat membuat model matematis suatu rangkaian Listrik R, L

dan C.

4. Dapat menyelesaikan suatu Linear Time Invariant System

dengan menggunakan metode Laplace.

Page 9: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

Fungsi dalam kawasan waktu (t) ke

kawasan kompleks (s).9

f(s)f(t)

Page 10: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

Penyelesaian Persamaan Laplace

10

Menggunakan Persamaan Laplace(1), Teorema(2) dan Melihat table Laplace(3) dari beberapa fungsi f(t) yang telah ada pada tabel Laplace

Page 11: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

1. Persamaan Laplace11

Page 12: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

Persamaan Laplace12

Contoh 1.

1. Tentukanlah pemetaan Laplace dari f(t) = 1

Jawab.

Gunakan persamaan Laplace

Page 13: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

Contoh13

1.

2.

3.

4.

2t£

2te£

t2sin£

Page 14: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

2. Teorema14

Page 15: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

Teorema 115

Page 16: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

Teorema 216

Page 17: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

Teorema 317

Page 18: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

Teorema 418

Page 19: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

3. Tabel19

Page 20: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

20

Page 21: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

21

Page 22: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

Tugas 3A22

1.

2.

3.

4.

5.

6.

7.

8.

t2£

4t£

5t2£

6t3£

32t£

3

3

2£ tt

-t2 4e3£ te

t2cos3t4sin2£

Page 23: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

Fungsi dalam kawasan kompleks (s) ke

kawasan waktu (t). (INVERS)23

f(s) f(t)

Page 24: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

Inverse Laplace Transforms24

Definition of the inverse Laplace transform

Page 25: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

Contoh25

1.

2.

3.

4.

Page 26: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

Inverse Laplace transforms using partial

fractions26

Page 27: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

Tugas 5B27

1.

2.

3.

4.

3s

1£ 1-

2

1-

s

3s

2

1-

4s

2

1-

5.

6.

7.

8.

25s

2

1-

13

4£ 1-

s

4

1-

s

4s

7s£

2

1-

Page 28: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

Penerapan Pemetaan Laplace pada

Persamaan Diferensial28

Page 29: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

Penerapan Pemetaan Laplace pada

Persamaan Diferensial29

Pemetaan Laplace adalah tool yang sangat berguna dalam menyelesaikan persamaan diferensial. Dipakainya Pemetaan Laplace dalam menyelesaikan persamaan diferensial dikarenakan pemetaan Laplace mengubah persamaan dalam kawasan waktu menjadikawasan s (kompleks).

Pemetaan Laplace mengubah persamaan diferensial menjadi bentuk aljabar biasa.

Penyelesaian persamaan diferensial adalah dengan mengubah balik pemetaan Laplace sehingga diperoleh suatu penyelesaian dalam kawasan waktu t (waktu)

Page 30: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

30

Page 31: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

The Laplace transforms of derivatives31

The Laplace transforms of derivatives

Page 32: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

Contoh32

Page 33: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

Latihan

33

Selesaikanlah persamaan diferensial berikut.

1. y’’−y = 0 dengan y(0) = 1 dan y’(0)=0.

Solusi

Page 34: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

Tugas 5C

34

Selesaikanlah persamaan diferensial berikut.

1. y’’−3y’+2y = 0 dengan y(0) = 1 dan y’(0)=0.

2. y’+3y=0. dengan y(3) = 1;

3. y’’−4y’+4y = 0 dengan y(0) = 1 dan y’(0)=1.

4. y’’-4y’-3y=0. dengan y(0) = 0 dan y’(0)=1.

5. y’’−4y’+13y = 0 dengan y(0) = 1 dan y’(0)=0.

6. y’’+2y’+2y=0. dengan y(0) = 1 dan y’(0)=0.

Page 35: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

Tugas 5C

35

Soal Tambahan

Page 36: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

Penerapan Pemetaan Laplace pada Filter

36

RF Filter Sebuah rangkaian filter merupakan rangkaian yang

dapat melewatkan sinyal dari satu range frekuensitertentu tetapi menghadang sinyal frekuensi yang lainnya.

Rangkaian filter ini merupakan gabungan darirangkaian reaktansi yang terdiri dari induktor dankapasitor.

Page 37: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

37

RF Filter Design – Basic Filter Types

Page 38: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

38

Filter Attenuation Profiles

Page 39: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

39

RF Filter Parameters

Insertion Loss:

Ripple

Bandwidth: BW 3dB = fu3dB – fL

3dB

Shape Factor:

Rejection

210 10 1in

in

L

PIL log log

P

min

max

A

A

BWSF

BW

Page 40: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

Contoh40

Page 41: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

Contoh41

Page 42: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

Low pass filter (LPF)

42

Low pass (3 elemen)

Page 43: MATERI 3 MATEMATIKA TEKNIK 1 PEMETAAN LAPLACE · Pemetaan Laplace Introduction The solution of most electrical circuit problems can be reduced ultimately to the solution of differential

Contoh43

Low pass (7 elemen)

L3L2L1

C1C2 C3

C4