Evaluation of Mode-I Fracture Toughness for Composite Laminate - Epoxy-Glass Fiber

 

D. Srikanth Rao*, N. Gopikrishna, J. Manoj Kumar

Department Mechanical Engineering, S R Engineering College, Warangal. Telangana. India.

*Corresponding Author Email: ssydev95@gmail.com, ngk310@gmail.com, jmanoj4u@gmail.com,M

 

ABSTRACT:

The conventional materials fail to meet the requirements of high technology applications like space. Applications. In order to meet the requirements like high temperature and wear resistances new materials are being searched. The composite materials are the best alternative for those applications. The applications of composite materials have recently increased because of high strength/stiffness for lower weight, superior fatigue characteristics, facility to change fiber orientations, etc. At the same time, these materials pose new problems such as inter ply cracking, inter laminar de-lamination and fiber cracking. Composite materials failure can be reduced by increasing fracture toughness. Our aim is to evaluate the fracture toughness of glass fiber/epoxy composites. Composites were prepared with glass fiber reinforced with epoxy based polymer. The fracture toughness of the specimen was employed to conduct mode-I fracture test using special loading fixtures as per ASTM standards of DCB5528 specimen.

 

KEYWORDS: Glass fiber, epoxy resin, hardener, DCB testing, fracture toughness

 

 


1. INTRODUCTION:

The role of engineering materials in the development of modern technology need not be emphasized. It is materials through which a designer puts forward his ideas into practice. We use a variety of materials for our needs and comfort and have been developing new materials for meeting our technological requirements. As the levels of technology have become more and more sophisticated, the materials used also have to be correspondingly made more efficient and effective. Several performance characteristics are expected from these materials.

 

They are:The materials to be used for sophisticated applications like aircraft and space applications should have higher performance, efficiency and reliability. Materials have to be of light-weight for many applications so that the resulting products can be efficient and cost effective. Materials must have combinations of properties for specific uses since present day product of modern technological origins operate in environment that are special or Extreme like very high temperature (of order of 2500°K), cryogenic condition, vacuum (as in space), high hydrostatic pressure (as in deep sea) .

 

The conventional material may not always be capable of meeting the demand of such environments. Hence new materials being created for meeting these performance requirements and composite materials from one class of such

materials are developed.

 

Knowledge of a laminated composite materials resistance to inter laminar fracture is useful for product development and material selection. A recent survey on emerging technologies has given the composite materials one of the top ten fields in engineering. The increasing use of composite materials in structural and space applications generated considerable interest for the development of techniques to predict the response under various loading conditions.

The technology has progressed to a stage where never composite materials are being considered, on an experimental basis for numerous applications in various fields. Such as aircraft, satellite launching vehicles, racket missiles, railways, automobile, energy, construction, infrastructure, medical, biomedical, Marine, sports etc. The composite Laminates are constructed by stacking several unidirectional layers in specified sequence of orientation. Hence, the failure of a single layer does not give the total failure of the laminate. However, it leads to progressive failure of the laminate. The common modes of failure in the composite materials are crack growth, fiber breakage and delaminating. Hence the study of crack growth behaviors in composite laminate is of special significance.

 

2. LITERATURE REVIEW:

As stated above, researchers are working with the problems of inter ply cracking, de- lamination and fiber cracking. This work is aimed at predicting the extent of crack propagation in a FRP composite laminate that subjected to finite and known loads. Chamois presented the difference between fiber composites and traditional materials. Any predictive approach for simulating structural fracture in fiber composites needs To formally quantify: all possible fracture modes the types of flaws they initiate, and the coalescing and propagation of these flaws to critical dimensions for imminent fracture. O’Brien T K, and Martin R H. (1993).briefly explained Results of ASTM Round Robin Testing for Mode I Inter laminar Fracture Toughness of Composite Materials. D. Srikanth Rao and N. Gopikrishna (2017) evaluated Strain Energy Release Rate of Epoxy Glass Fibre Laminate (Mode - I). A B de Morais. (2003) Double cantilever beam testing of multidirectional laminates. Pereira A B, de Morais A B. (2004). Mode I interlaminar fracture of carbon/epoxy multidirectional laminates. Choi N S, Kinloch A J, Willams J G. (1999).De lamination fracture of multidirectional carbon-fiber / epoxy composites under mode I, mode II and mixed mode I/II loading. D. Srikanth Rao and N. Gopikrishna (2017) evaluated Mode – I fracture toughness Epoxy glass Fiber composite laminate. A J Brunner, B R K Blackman and P Davies. (2008) a status report on the de lamination resistance testing of polymer–matrix composites.

 

3. EXPERIMENTAL METHODS TO DETERMINE FRACTURE TOUGHNESS

3.0. Specimen Preparation and Testing -- Preparation of Specimen

A. MATERIALS:

i. E-Glass Fiber:

Fiber glass has a white color and is available as a dry fiber fabric as shown in Fig.1. It has good strength & electrical resistivity. It is used in circuit boards of computers to provide stiffness and electrical resistance. Because of electrical resistance it is suited for applications where radio-signal transparency is desired in aircraft redoes and antenna. It has a specific gravity 2.54g/cc and a melting point 1555°F (846°C). Refract. Index is 1.547.

 

 

Fig. 1 Glass fiber

 

ii. Epoxy resin:

Epoxy polymers are made by reacting epichlorohydrin with bisphenol-A in an alkaline solution which absorbs the HCl released during the condensation polymerisation reaction. Each chain has a molecular weight between 900 and 3000 with an within the polymer chain. The epoxy is cured by adding a hardener in equal amounts and being heated to about 120°C. The hardeners are usually short chain diamines such as ethylene diamine.

 

Epoxy resins are much more expensive than polyester resins because of the high cost of the precurs or chemicals most noticably epi chloro hydrin. However, the increased complexity of the 'epoxy' polymer chain and the potential for a greater degree of control of the cross linking process gives a much improved matrix in terms of strength and ductility.

 

Most epoxies require the resin and hardener to be mixed in equal proportions and for full strength require heating to complete the curing process. This can be advantageous as the resin can be applied directly to the fibers and curing need only take place only at a time of manufacture. And known as pre-preg or pre impregnated fibre.

 

iii. Hardener:

A substance added to control the degree of hardness of the cured film. It is also a substance or mixture added to plastic composition to promote or control the curing action by taking part in it.

 

 

Fig. 2 Epoxy resin and hardener

 

3.2 Preparation of Specimen:

The required mixture of resin & hardener (as shown in Fig.2) were made by mixing them in (10:1) parts in a beaker. When the epoxy resins modified with different contents of particles were prepared through vacuum assisted hand lay-up procedures, they were diffused into unidirectional fibers to form the glass fiber/epoxy composites. The process is that the final mixture epoxy resin with the H-100 curing agent was poured on one dry glass fiber layer and then impregnated into the dry fibers with the assistance of a hand roller until the fiber bundles were permeated completely by the resin. Then, another ply of dry fiber was stacked on it. The repeating process continued until the 12 layers of glass fibers were fabricated (as shown in Fig. 3). Since the interlaminate fracture toughness of composites was measured from the double cantilever beam (DCB) specimens, during the process, a porous film was inserted in the mid-plane of the laminates for the creation of pre-crack. The entire stacking was then sandwiched between two steel plates with porous Teflon fabric on the surfaces and then sealed within a vacuum bag. The whole laminates were cured in a hot press with a suggested temperature profile under vacuum conditions.

 

 

Fig. 3a – Tray (on left), 3b - Prepared Glass fiber laminates (on right) Fig. 4 Prepared specimens of Glass Epoxy Laminate after cutting

 

The specimens were cut into the required dimensions as per ASTMD5528 standards for fracture toughness test shown in the Fig. 4.

 

3.4 Test Procedure: Fracture toughness was evaluated from the specimens that were made of ply laminates with a porous film inserted in the mid-plane during the layup process for creating the initial crack.. Symmetric loadings applied in opposite directions were transferred into the cracked end of the specimens through a pair of hinges bonded on the specimen surfaces resulting in the mode I crack extension. Prior to the fracture tests, specimens were pulled out such that the precrack can extend around 4 mm penetrating the resin enriched area and reach the “true” crack tip where the fracture toughness begin to be measured. All specimen preparations and experimental procedures were performed based on ASTM standard D5528 (as shown in Fig. 5).

 

 

Fig. 5 DCB Testing

 

4. RESULTS:

Mode 1 Fracture Toughness test as per ASTM D 5528 standard have been carried out on Fracture toughness testing machine Fig. 5. The Results from the test have been evaluated as per ASTM D 5528 and computed and recorded.The following are the results of the experiment

 

Table: 1 For specimen ‘C’ with orientation

S. No.

Maximum Load, P (N)

Crack length, a(mm)

Young’s Modulus, E (Mpa)

Tensile stress at 0°-45° Maximum Load, σ (Mpa)

Tensile strain at  45°- 0° Maximum load, e (mm/mm)

Fracture toughness, KIC (J/m2)

1

97.89925

49.724

597.61580

65.26617

0.49724

18.24026

2

76.43932

42.166

718.44433

50.95955

0.42166

13.11495

3

68.94221

81.331

185.57687

45.96148

0.81331

16.42789

4

140.75590

91.733

224.78349

93.83727

0.91733

35.62034

Avg

96.00917

66.239

431.60512

64.00611

0.66239

20.85086

Graph: 1- Load (N) Vs Extension (mm)

 

Model Calculations for Table 1:

The formulae used for fracture toughness, KIC = (EGIC) 1/2

Griffith’s criterion, GIC = σ2ᴨa/2E

Evaluation of Fracture Toughness for sample using the above values:

 

GIC = σ2ᴨa/2E = (65.266172*)/(2*597.61580) = 0.55672.

KIC = (EGIC) ½ = 597.61580*0.55672) = 18.2402 J/m2.

 

Table: 2 For specimen ‘D’ with orientation 45° -45°             45° -45°.

S.N o.

Maximum Load, P (N)

Crack length, a(mm)

Young’s Modulus, E (Mpa)

Tensile stress at Maximum Load,σ (Mpa)

Tensile strain at Maximum load,e (mm/mm)

Fracture toughness, KIC (J/m2)

1

146.77113

44.1

381.98206

97.84742

0.441

25.75304

2

57.09154

88.233

329.20892

38.06103

0.88233

14.16954

3

82.90364

68.733

219.67567

52.2691

0.68733

18.16038

4

58.48447

29.411

296.07033

38.98965

0.29411

8.38038

Avg

86.3127

57.619

306.73424

57.5418

0.57619

16.61583

 

Table: 3 For specimen ‘E’ with orientation 45° 90° 45° 90°

S.N o.

Maximum Load,P (N)

Crack length, a (mm)

Young’s Modulus, E (Mpa)

Tensile stress at Maximum Load, σ (Mpa)

Tensile strain at Maximum load,e (mm/mm)

Fracture toughness,KIC (J/m2)

1

54.94004

20.486

532.61716

36.62669

0.20486

6.57031

2

67.60565

18.428

594.41461

45.07043

0.18428

7.66815

3

68.07683

17.966

650.52032

45.38455

0.17966

7.62418

4

35.71883

43.366

122.67509

23.81256

0.43366

6.21499

Av

56.58534

25.061

475.0568

37.72356

0.25061

7.0194

 

Table: 4 for specimen ‘F’ with orientation 0°90° 0° 90°

S.No.

Maximum Load,P (N)

Crack length,a (mm)

Young’s Modulus,E (Mpa)

Tensile stress at Maximum Load,σ (Mpa)

Tensile strain at Maximum load, e (mm/mm)

Fracture toughness, KIC (J/m2)

1

63.78637

223.342

448.27454

42.52425

2.23342

25.18731

2

91.34468

24.867

356.70901

60.89645

0.24867

12.03548

3

206.53829

26.933

521.26168

137.69220

0.26933

28.32119

4

155.64854

61.967

1200.64183

103.76569

0.61967

32.37382

Av

129.32947

84.277

631.72176

86.21965

0.84277

24.47945

5. CONCLUSION:

Fracture toughness is more for specimen ‘F’, which indicates that the crack growth is less for this sample (i.e.,) for orientation 0° 90° 0° 90°. That indicates that the above oriented specimen is preferable among all the other oriented specimens. The crack propagation decreases with the increase of fracture toughness. In the fracture test the sample bears maximum stress up to some limit and then it starts decreasing before it gets failed.

 

6. REFERENCES:

1.     O’Brien T K , and Martin R H. (1993).Results of ASTM Round Robin Testing for Mode I Inter laminar Fracture Toughness of Composite Materials. Journal of Composites Technology and Research. 15(4): 269 – 281.

2.     D. Srikanth Rao and N. Gopikrishna - International education & Research Journal - Jan, 2017. 3(1)44-46.

3.     A B de Morais. (2003) Double cantilever beam testing of multidirectional laminates. Composite Part A: Applied Science. A34(12): 1135–1142.

4.     Pereira A B, de Morais A B. (2004). Mode I interlaminar fracture of carbon/epoxy multidirectional laminates. Composite Science and Technology.64: 2261–2270.

5.     Choi N S, Kinloch A J, Willams J G. (1999).De lamination fracture of multidirectional carbon-fiber / epoxy composites under mode I, mode II and mixed mode I/II loading. Journal of Composite Material. 33(1): 73–100.

6.     D. Srikanth Rao and N. Gopikrishna - International Journal of Innovative Research in Science, Engineering and Technology Vol : 6 (1) Pp 925-931, Jan, 2017.

7.   A J Brunner, B R K Blackman and P Davies. (2008) A status report on de lamination resistance testing of polymer–matrix composites. Engineering Fracture Mechanics.75: 2779–2794.

 

 

 

 

 

 

 

 

 

 

 

Received on 13.10.2017            Accepted on 10.01.2018      

©A&V Publications all right reserved

Research J. Engineering and Tech. 2018;9(1): 70-74

DOI: 10.5958/2321-581X.2018.00011.9