06 MSK Teori Lamina DH

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Mekanika Struktur Komposit 06. Teori Lamina Dwi Hartini, S.T., M.T.

description

Teori Lamina,,Komposit

Transcript of 06 MSK Teori Lamina DH

Page 1: 06 MSK Teori Lamina DH

Mekanika Struktur Komposit06. Teori Lamina

Dwi Hartini, S.T., M.T.

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PENDAHULUAN

Lamina diartikan sebagai lapisan komposit tunggal yang hanya mempunyai satu arah serat.

Lamina merupakan elemen pembangun struktur komposit, karena itu pengetahuan mengenai sifat-sifat mekanika lamina ini sangat penting untuk mengetahui lebih lanjut mengenai struktur komposit.

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PLATE UNDER MULTI-AXIAL LOADINGS

1 1

1

2

0

.

12

112

11

E

E

(Isotropic)

11

2

2

12

12

12

2

1

12

2

1

100

01

01

G

EE

EE

Constitutive Equations for Isotropic

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Or:

12

2

1

22

22

12

2

1

00

011

011

G

EE

EE

Stiffness Matrices for Isotropic Materials

Where:

12

EG

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PLATE UNDER MULTI-AXIAL LOADINGS

1 1

1

2

0

.

12

1

1121122

1

11

E

E

(Orthotropic)

11

2

2

12

12

12

2

1

12

22

21

1

12

1

12

2

1

100

01

01

G

EE

EE

Constitutive Equations for Orthotropic

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Or:

12

2

1

12

2112

2

2112

212

2112

121

2112

1

12

2

1

00

0.1.1

0.1.

.1

G

EE

EE

Stiffness Matrices for Orthotropic Materials

Where:

121

221 .

E

E

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COMPLIANCE MATRIX FOR ORTHOTROPIC

12

2

1

66

2212

1211

12

2

1

00

0

0

S

SS

SS

Where:

1266

222

2

21

1

1212

111

1 ;

1

; 1

GS

ES

EES

ES

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STIFFNESS MATRIX FOR ORTHOTROPIC

12

2

1

66

2212

1211

12

2

1

00

0

0

Q

QQ

QQ

Where:

12662112

222

2112

121

2112

21212

2112

111

; 1

11 ;

1

GQE

Q

EEQ

EQ

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EXAMPLE

Carbon-epoxy T300/5208 has properties as follows: E1 = 19.2 Msi ; E2 = 1.56 Msi ; v12 = 0.24 ; G12 = 0.82 Msi

Therefore, the compliance coefficients are (in 1/Msi):

0

2195.11

641.01

0125.0 05208.01

2616

1266

222

1

1212

111

SS

GS

ES

ES

ES

And the stiffness coefficients are (in Msi)

0

820.0 567.1

376.0 29.19

2616

6622

1211

QQ

QQ

QQ

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TRANSFORMED STIFFNESS MATRICES

x

y

12

Transformation of stress and strains in arbitrary direction:

xy

y

x

xy

y

x

TT

2

12

2

1

1

12

2

1

and

sin cos ;

22

2

2

22

22

22

222

22

22

1

nm

nmmnmn

mnmn

mnnm

T

nmmnmn

mnmn

mnnm

T

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From the stiffness matrix equation:

11 Q

Therefore, we find:

xx TQT 21

1

or

xy

y

x

xy

y

x

T

Q

QQ

QQ

T

2

66

2212

12111

1

00

0

0

Now we define:

xx Q

21

1 TQTQ

and

or

xy

y

x

xy

y

x

QQQ

QQQ

QQQ

662616

262212

161211

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The individual ijQ terms are given below:

)()22(

)2()2(

)2()2(

)()4(

)2(2

)2(2

4466

226612221166

3662212

366121126

3662212

366121116

4412

2266221112

422

226612

41122

422

226612

41111

mnQnmQQQQQ

nmQQQmnQQQQ

mnQQQnmQQQQ

mnQnmQQQQ

mQnmQQnQQ

nQnmQQmQQ

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DISPLACEMENT CHARACTERISTICS

Isotropic Orthotropic Off-axis Lamina

(Anisotropic)

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EXAMPLE (2)

Carbon-epoxy T300/5208 has properties as follows: E1 = 19.2 Msi ; E2 = 1.56 Msi ; v12 = 0.24 ; G12 = 0.82 Msi and fiber angle 30o to the global axis

Therefore, the compliance coefficients are (in 1/Msi):

465.1 ;3636.0

8434.0 5878.0

1065.0 2933.0

2616

6622

1211

SS

SS

SS

And the stiffness coefficients are (in Msi)

017.2 658.5

975.3 843.2

531.3 75.11

2616

6622

1211

QQ

QQ

QQ

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OFF-AXIS ENGINEERING CONSTANTS

Xx

y1

2

X

44

12

22

121

12

21

4

2

22

1

12

12

4

1

22

1221

44

1

12

4

2

22

1

12

12

4

1

114222

1

12111

111

12111

nmG

nmGEEEG

mE

mnEG

nEE

nmGEE

mnE

E

nE

mnEG

mEE

xy

y

xxy

x

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Pengaruh sudut orientasi serat terhadap

kekuatan bahan komposit.