• Tidak ada hasil yang ditemukan

ʇ|ÀÆ» ®Ì¿Z°»

N/A
N/A
Protected

Academic year: 2024

Membagikan "ʇ|ÀÆ» ®Ì¿Z°»"

Copied!
8
0
0

Teks penuh

(1)

mme.modares.ac.ir

*1

2

- 1 - 2

* 43344

- 19991 [email protected]

: 13 1394

: 17 1395

: 27 1395

.

. .

.

. .

. .

Fracture analysis of a unidirectional composite double cantilever beam specimen with finite length

AmirReza Shahani

*

, Razieh Abolfathitabar

Department of Mechanical Engineering, K. N. Toosi University of Technology, Tehran, Iran.

*P.O.B. 19991-43344, Tehran, Iran, [email protected]

A RTICLE I NFORMATION A BSTRACT

Original Research Paper Received 03 January 2016 Accepted 05 April 2016 Available Online 16 May 2016

The unidirectional composite DCB specimen is considered as two finite length Timoshenko beams, attached together along a common edge except at the initial delamination length. Because of symmetry, only one half of the specimen is considered, which is partly free and partly resting on an elastic foundation. The problem is analytically solved by considering Timoshenko beam resting on Winkler and Pasternak elastic foundations and fracture toughness is generally derived. In the prior researches on this specimen using Timoshenko beam theory, the effect of the ligament length on the energy release rate was ignored. This research presents the solution for finite ligament length. Besides, the effect of ligament length on energy release rate and its minimum value that makes the energy release rate independent of the ligament length, is presented. For the special case when the ligament is large compared with the beam thickness, a closed form solution is derived for Timoshenko beam resting on Winkler elastic foundation. The analytical results are compared to prior researches on this subject and good agreement is observed. The fracture toughness and compliance obtained by Timoshenko beam resting on Winkler elastic foundation predicts more accurate results with respect to experimental results.

Keywords:

Delamination

Strain Energy Release Rate Double Cantilever Beam Specimen Timoshenko Beam Theory Elastic Foundation

- 1 .

.

1

.

1 Delamination

[ Downloaded from mme.modares.ac.ir on 2023-12-06 ]

(2)

.

.

1

] - 1 [ 3 )

.( 1

] [ 1 .

. .

) ( 1

= 8 ( )

.

] 2 [ 4 :

) ( 2

= 2 1 2

= 12 (3)

3

] 3

[ 5

) ( 4

= 2

+ 8

) ( 5

= 12 +

] [ 6

= /

6

) ( 6

= 8

4 + 4 +

) ( 7

= +

( )

] [ 7 .

1 DCB (Double Cantilever Beam)

] [ 8 .

2

] [ 9

3

.

] [ 7 . ] [ 10 ]

[ 9

. ] [ 11 .

] [ 5

- ]

[ 11

] [ 10 .

] [ 12

. ]

[ 13

. .

] [ 7

.

] [ 11 .

] [ 5 ] .

[ 14 -

.

4

.

. ]

[ 15

2 Winkler

3 Pasternak

4 Ligament

[ Downloaded from mme.modares.ac.ir on 2023-12-06 ]

(3)

.

1

. ]

[ 16

. .

] [ 17

] [ 8

> 2 )

.(

] [ 18 .

] [ 8

.

2

.

.

- 2

- 2 - 1 2

.

. )

.

1 Woven

2 Maple

] [ 10 . .

8

) ( 8

=

) ( /12

9 ) ( 9

=

] [ 19

) ( 10

= 10(1 + ) 12 + 11

.

) ( 11

=

:

) ( 12

=

) ( 12

=

8 11 12

) ( 13

+ =

) ( 13

=

= 0

) ( 14

= = 0

] [ 9 - 15

) ( 15

= ( /2)

) ( 15

= 2

Fig. 1 Double cantilever beam specimen

1

[ Downloaded from mme.modares.ac.ir on 2023-12-06 ]

(4)

Fig. 2 Model of the half of DCB specimen on elastic foundation 2

.

15 13

) ( 16

= 3 2

) ( 16

=

= =

.

) ( 16 -

17

) ( 17 + 1

2

1 + 3

2

1 = 0

- 2 - 2

) ( 18

(0) 0 (0)

M

V P

) ( 18

( ) 0

( ) 0

M a c V a c

=

) ( 19 ( ) = ( )

( ) = ( )

) ( 19 ( ) = ( )

( ) = ( )

) 1 .( 2

) 0 < <

) ( 20

=

) ( 20

=

) ) ( 8 ( 11 20

) ( 21

= 2 +

) ( 21

= 6 + +

< < +

=

=

= )

( 19

21

. .

= 0

) ( 22

= 4 + . 22

22

)

=

. ) . 17

21

= = 0 19

=

= 0

= 0 .(

17

) ( 23

2 + = 0

= +

. =

23 19

) ( 24

=

) ( 24

=

18

.

8 11 18

24

) ( 25

= + = 0

) ( 25

= + = 0

) ( 25

= =

) ( 25

= =

23

) ( 17

) ( 26 ( ) = exp( )( sin( ) + cos( )) +

exp( )( sin( ) + cos( )) )

( 23

,

=

. ±

<

= ± ±

.

27

]

[: 10

) ( 27

2 = +

) ( 27 2 =

26 25

26

= 22 =

h c

a x

,

[ Downloaded from mme.modares.ac.ir on 2023-12-06 ]

(5)

) ( 28

= 2

= 2 2

. + = 29

) ( 29

= 2

.

- 3

12

( )

. 17

30

) ( 30

+ = 0

30

) ( 31

+ = 0

31

30 26

) ( 32 ( ) = exp( )( sin( ) + cos( )) +

exp( )( sin( ) + cos( )) ( ) 32

25

- 4 >

> 2 .

( ) .

26 ) ( 33 ( ) = exp( )( sin( ) + cos( ))

25 25 33

) (

= . 22

28 2

.

.

32 34

) ( 34 ( ) = exp( )( sin( ) + cos( ))

25 25 34

) ( 35

= +

/

+

/

] [ 7

- 5

- 5 - 1

. )

( ] [ 18 )

= /2(1 + )

= =

4

.(

] [ 18 3

. .

1 ] 1

[ 10

C

. 1

= 1/

=

1/

= 1/

/

[ Downloaded from mme.modares.ac.ir on 2023-12-06 ]

(6)

Fig. 3 Verifying present study (Timoshenko beam on Winkler foundation) by comparing with [

18

]

]

3

[ 18 )

1

) .(

1

.

- 5 - 2

. 4

> 2

-

] [ 14 . 5

.

Fig. 4 Normalized energy release rate variation as a function of / (Timoshenko beam on Winkler foundation)

4

) / .

6

.

) 2 .( 3

.

) (

] [ 14 ) -

.

= 5

] [ 7

4 5

< 2 6

> 2

] 1 [ 10

Table 1 Compliance indicator comparison of present study and ref

] [ 10

1 2

3 4 5 6

1000 × (a

11 (GPa)-1

6.8

)

6.8 6.8

6.8 13.6 3.4

1000 × (a

22 (GPa)-1

128

)

128

128 128 128 128

1000 × (a

66 (GPa)-1

)

362

362 362

362 362 362

h/a

0.025

0.033 0.05

0.1 0.05 0.05

C/C

0

-1

)

0.169 0.228

0.363 0.83 0.256 0.525

C/C

0

-1 ( [ 10 )]

0.169 0.228

0.363 0.83 0.256 0.525

Fig. 5 Comparing present solution (Timoshenko beam on Winkler elastic foundation) and [

14

]

( )

5

] [ 14

[ Downloaded from mme.modares.ac.ir on 2023-12-06 ]

(7)

Fig. 6 Comparing normalized energy release rate of the present study (Timoshenko beam on Winkler foundation) with [

7

] and [

14

]

)

6

( ] [ 7 ] [ 14

- 5 - 3 -

. 7

] [ 14

.

.

8 ]

[ 14

. .

Fig. 7 Comparing energy release rate of different analytical models with ref [

14

]

7

]

[ 14

Fig. 8 Comparing compliance of different analytical models with

experimental results [

14

]

8 ] [ 14

- 6

] [ 14 .

.

-

- ]

[ 14

[ Downloaded from mme.modares.ac.ir on 2023-12-06 ]

(8)

- 7

) ( m ) ( m ) (

) (

) (

) ( m

) ( m ( (

) ( J/m

) ( J/m

( ) ( m

) ( m

) (

) ( N. m

) ( N

) ( N ) ( N/m

) ( m

(

) ( - 8

[1] A. Standard, D5528, Standard test method for mode I interlaminar fracture toughness of unidirectional fiber-reinforced polymer matrix composites, ASTM (American society of testing and materials), Philadelphia PA, 2002.

[2] B. ISO, 15024, Fiber-reinforced plastic composites–determination of mode I interlaminar fracture toughness, HIC for unidirectionally reinforced materials, British Standards International, 2001.

[3] K. JIS, 7086: Testing methods for interlaminar fracture toughness of carbon fiber reinforced plastics, Japanese Standards Association, 1993.

[4] G. R. I. a. J. A. Kies, Critical energy rate analysis of fracture strength, Welding Journal Research Supplement, Vol. 33, pp. 193-198, 1954.

[5] R. Olsson, A simplified improved beam analysis of the DCB specimen, Composites Science and Technology, Vol. 43, No. 4, pp. 329-338, 1992.

[6] J. Weatherby, Evaluation of energy release rates in unidirectional double cantilevered beam fracture specimens, in: Mechanics and Materials Report Number MM4665-82-9, Master's thesis Texas A&M University, 1982.

[7] K. Kondo, Analysis of double cantilever beam specimen, Advanced Composite Materials, Vol. 4, No. 4, pp. 355-366, 1995.

[8] M. Kanninen, An augmented double cantilever beam model for studying crack propagation and arrest, International Journal of fracture, Vol. 9, No. 1, pp. 83-92, 1973.

[9] M. Kanninen, A dynamic analysis of unstable crack propagation and arrest in the DCB test specimen, International Journal of Fracture, Vol. 10, No. 3, pp. 415-430, 1974.

[10] J. Williams, End corrections for orthotropic DCB specimens, Composites Science and Technology, Vol. 35, No. 4, pp. 367-376, 1989.

[11] J. Whitney, Stress analysis of the double cantilever beam specimen, Composites Science and Technology, Vol. 23, No. 3, pp. 201-219, 1985.

[12] M. M. Shokrieh, M. Heidari-Rarani, A comparative study for beams on elastic foundation models to analysis of mode-I delamination in DCB specimens, Structural Engineering and Mechanics, Vol. 37, No. 2, pp. 149- 162, 2011.

[13] M. Shokrieh, M. Heidari-Rarani, S. Rahimi, Influence of curved delamination front on toughness of multidirectional DCB specimens, Composite Structures, Vol. 94, No. 4, pp. 1359-1365, 2012.

[14] F. Ozdil, L. Carlsson, Beam analysis of angle-ply laminate DCB specimens, Composites Science and Technology, Vol. 59, No. 2, pp. 305-315, 1999.

[15] L. Banks-Sills, C. Ishbir, V. Fourman, L. Rogel, R. Eliasi, Interface fracture toughness of a multi-directional woven composite, International Journal of Fracture, Vol. 182, No. 2, pp. 187-207, 2013.

[16] Z. Jiang, S. Wan, Z. Zhong, M. Li, K. Shen, Determination of mode-I fracture toughness and non-uniformity for GFRP double cantilever beam specimens with an adhesive layer, Engineering Fracture Mechanics, Vol.

128, pp. 139-156, 2014.

[17] J. Monteiro, R. Campilho, E. Marques, L. da Silva, Experimental estimation of the mechanical and fracture properties of a new epoxy adhesive, Applied Adhesion Science, Vol. 3, No. 1, pp. 1-17, 2015.

[18] A. Shahani, M. Forqani, Static and dynamic fracture mechanics analysis of a DCB specimen considering shear deformation effects, International journal of solids and structures, Vol. 41, No. 14, pp. 3793-3807, 2004.

[19] G. Cowper, The shear coefficient in Timoshenko’s beam theory, Journal of applied mechanics, Vol. 33, No. 2, pp. 335-340, 1966.

[ Downloaded from mme.modares.ac.ir on 2023-12-06 ]

Referensi

Dokumen terkait

Monnier, Non-destructive evaluation of damage and failure of fibre reinforced polymer composites using ultrasonic waves and acoustic emission, Advanced engineering materials, Vol..

Li, Type synthesis, kinematic analysis, and optimal design of a novel class of Schönflies-Motion parallel manipulators, Automation Science and Engineering, IEEE Transactions on, Vol..

Modeling and optimization of the quasi-steady operation of Solar Power Plant equipped with thermal energy storage system Vahid Khalilzadeh Bavil, Javad Mahmoudimehr Department of

Melt Behavior and Shrinkage Force Effect of Al Melt in Al/Mg Bimetal Cast via Centrifugal Casting Morteza Sarvari, Mehdi Divandari School of Metallurgy and Materials Engineering, Iran

AZ31C The effect of pass numbers over microstructure and mechanical properties of magnesium alloy of AZ31C in the tubular channel angular pressing TCAP at temperature of 300°C

AZ31C The effect of pass numbers over microstructure and mechanical properties of magnesium alloy of AZ31C in the tubular channel angular pressing TCAP at temperature of 300°C