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International 
OPEN ACCESS Journal 
Of Modern Engineering Research (IJMER) 
| IJMER | ISSN: 2249–6645 | www.ijmer.com | Vol. 4 | Iss.7| July. 2014 | 40| 
Free Vibration Analysis of Polyproplyne- Nanoclay Composite Beam with Crack Narra. Tilak Ratan1, Dr. G. Vijay Kumar2, M. Rajya Lakshmi3 1(Dept. of Mechanical Engineering, PVP Siddhartha Institute of Technology, India 2(Professor, Dept. of Mechanical Engineering PVP Siddhartha Institute of Technology, India 3(Asst. Professor, Dept. of Mechanical Engineering, PVP Siddhartha Institute of Technology, India 
I. INTRODUCTION 
Fiber Reinforced Plastics (FRP) are commonly used in aerospace, automotive and other engineering applications mainly because of their high strength-to-weight ratio, high stiffness, good resistance to fatigue, and corrosion resistance. Reinforced fibers are usually added in the form of continuous or chopped fibers in a polymer matrix. Each type of these reinforcement fibers has their benefits and limitations in applications. A short fiber reinforced composites can have better processing properties and can be moldable into complex shaped components. Long fiber reinforced composites, on the other hand, provide enhanced strength and stiffness properties as per the desired directions. Various types of synthetic and natural fibers reinforced plastics are presently studied in literature, namely, glass fiber, carbon fiber, boron, alumina, oxide/carbide and sisal/jute based fibers in a polymer matrix. In addition to these fiber reinforced composites, particle reinforced polymer composites are also widely investigated. In these particle filled composites, various types of nano- and micro-scale particles are used. Nano particle reinforced polymer composites gained special attention due to their superior and improved properties when compared to their corresponding micro-scale particles. Nano clays, carbon nano tubes and alumina/oxide based particles are widely used as nano particle reinforcements in polymer matrices. Polymer-Clay Nano composites (PCN) are a relatively new area of research in particle filled composites, and consists of Nano Clay (NC) as the reinforcement and a polymer serves as the matrix material. The addition of small amounts of clay (0 to 15% wt) in a polymer matrix leads to improved mechanical, thermal and barrier properties. The addition of nano clays in a polymer matrix may result in the formation of two types of nano composite structures, namely, intercalated and exfoliated nanostructures. In an intercalated structure, the host polymer matrix enters into the interlayer spacing of the nano clay and increases the interlayer spacing but maintains the parallel arrangement of the nano layers of clay in the matrix. If the nano layers of clays are randomly dispersed in the matrix, then the structure is called an exfoliated structure. In practice, exfoliated structures provide enhanced and improved properties due to their excellent dispersions and improved aspect ratio. The addition of the NC in the Ply Propylene (PP) matrix increases the thermal stability in air medium, increases physical properties (dimensional stability), improves flame retardant properties increased thermal- oxidative stability, and improves mechanical properties, fracture properties and gas barrier properties. Several studies were conducted with various types of clay concentrations and compatabilizers. The main applications of PP materials are home appliances such as, chairs and toys, clothing, medical, EPP toy air craft. Crack is initiation of the wrecking of material in some cases. Strength plays very key role for crack growth. If material has high strength, crack will grow slowly otherwise, crack will propagate quickly. And frequency analysis is one of the most promising techniques to detect crack depth. If crack depth increases, then, frequency will down in free vibration. In this paper, efforts have been going made through PP- NC composite beam for un-cracked and cracked with different crack to depth ratios. 
Abstract: Vibration analysis is one of the most promising techniques to detect the crack. In this paper, Poly Propylene - Nano Clay is analyzed for it’s free vibration. The proposed composite beam is modeled with crack. Analysis is done by using Finite element package ANSYS-14.5. The Nano Clay in composite is varied from 0 to 15 percentage (0,1,3,5,7,9,11,13,15) and crack depth to width ratios are chosen as, 0,0.25,0.5,0.8. Impact of varying percentage of NC and varying crack depths on natural frequency are analyzed using free vibration analysis. 
Keywords: Nano Clay-Poly Proplyne composite Cantilever beam, Free vibration Analysis.
Free Vibration Analysis Of Polyproplyne- Nanoclay Composite Beam With Crack 
| IJMER | ISSN: 2249–6645 | www.ijmer.com | Vol. 4 | Iss.7| July. 2014 | 41| 
A -Material Properties Material properties were extracted from research papers by J. Yan1[15] and density was calculated from Rule of mixture. Properties of material for different percentages of nano clay with Poly propylene are listed in table 1. Table 1: Mechanical properties of Poly Propylene - Nano Clay for different % of NC 
% of NC 
Yong’s Modulus (Gpa) 
Poisons ratio 
Density (Kg/m3) X 103 
0 
1.56 
0.35 
1.45 
1 
1.7 
0.34 
1.45 
3 
1.72 
0.28 
1.45 
5 
1.81 
0.28 
1.46 
7 
1.92 
0.29 
1.46 
9 
1.96 
0.31 
1.47 
11 
1.83 
0.36 
1.47 
13 
2.26 
0.36 
1.47 
15 
2.27 
0.33 
1.48 
B- Steps involved in detecting frequencies of cracked beam main steps involved to detect frequencies of cracked beam are, 
1) Natural frequencies of un-cracked beam for different composition are determined theoretically. 
2) Natural frequencies of un-cracked beam for different compositions are estimated in ANSYS 14.5. 
3) Theoretical results are compared with ANSYS 14.5 Results. 
4) Natural frequencies of composite beam for different % of NC are estimated using ANSYS 14.5 for different crack depths. 
II. THEORETICAL CALCULATIONS 
Theoretical calculations are made through the following formulae for four modes of natural frequencies and results are shown in table 2. Where, L=Length of the beam, E=Young’s modulus of material, I=Moment of inertia of cross section, A=Area of cross section, ρ=Density of material. Table 2: Variation of frequency with change in NC % with theory 
% of NC 
frequency of 1stmode(Hz) 
frequency of 2ndmode(Hz) 
frequency of 3rd mode(Hz) 
Frequency of 4th mode(Hz) 
0 
1.76 
11.0606 
31.0199 
60.833
Free Vibration Analysis Of Polyproplyne- Nanoclay Composite Beam With Crack 
| IJMER | ISSN: 2249–6645 | www.ijmer.com | Vol. 4 | Iss.7| July. 2014 | 42| 
1 
1.8474 
11.5262 
32.3818 
63.5041 
3 
1.8574 
11.6087 
32.5571 
63.8478 
5 
1.9054 
11.9087 
33.3984 
65.4978 
7 
1.9624 
12.265 
35.4775 
69.575 
9 
1.9819 
12.3868 
34.7393 
68.1274 
11 
1.915 
12.9687 
33.5667 
65.8278 
13 
2.1282 
13.3025 
37.3039 
73.1568 
15 
2.1319 
13.3243 
37.3686 
73.2836 
III. FINITE ELEMENT MODELING 
The ANSYS 14.5 finite element program was used for free vibration of the cracked beams. A 20-node three-dimensional structural solid element under SOLID 186 was selected to model the beam. The beam was discredited into 1045 elements with 2318 nodes. Geometrical shape of the beam is shown in figure 1. Cantilever boundary condition was considered by constraining all degrees of freedoms of the nodes located on the left end of the beam. The subspace mode extraction method was used to calculate the natural frequencies of the beam and mode shapes are shown in figure 2 and results are in table 3. 
Figure 1 : Geometrical model for un-cracked beam 2-a: 1st mode-1.7783Hz frequency 2-b: 2nd mode-11.14Hz frequency
Free Vibration Analysis Of Polyproplyne- Nanoclay Composite Beam With Crack 
| IJMER | ISSN: 2249–6645 | www.ijmer.com | Vol. 4 | Iss.7| July. 2014 | 43| 
2-c: 3rd mode-31.194Hz frequency 
2-d: 4th mode-61.142Hz frequency Figure 2: Mode Shapes of un-Cracked Beam for 0% Nanoclay Table 3: Variation of frequency with change in NC % with simulation 
% of NC 
frequency of 1stmode(Hz) 
frequency of 2ndmode(Hz) 
Frequency of 3rdmode(Hz) 
frequency of 4thmode(Hz) 
o 
1.77827 
11.1405 
31.1936 
61.142 
1 
1.85523 
11.623 
32.544 
63.785 
3 
1.8621 
11.666 
32.662 
64.004 
5 
1.9104 
11.963 
33.509 
65.665 
7 
1.968 
12.33 
34.52 
67.648 
9 
1.989 
12.461 
34.889 
68.376 
11 
1.925 
12.06 
33.768 
66.189 
13 
2.1391 
13.401 
37.523 
73.549 
15 
2.141 
13.413 
37.556 
73.607 
IV. Comparison of results After comparison of both theoretical and ANSYS-14.5 results, the difference between both results is negligible and comparison of frequency is shown in figure 3. Hence, the analysis of cracked beam is extended in ANSYS-14.5 package. Figure 3: Comparision of theoritical and ANSYS-14.5 results for different % of Nano Clay.
Free Vibration Analysis Of Polyproplyne- Nanoclay Composite Beam With Crack 
| IJMER | ISSN: 2249–6645 | www.ijmer.com | Vol. 4 | Iss.7| July. 2014 | 44| 
V. Results After comparison of the both theoretical and ANSYS-14.5 results, Procedure could be verified in ANSYS-14.5 from the journal [19] for Aluminum material. Same results were obtained from that procedure. Hence, the same procedure is adopted for extracting natural frequencies of cracked beam as shown in figure 4 and 5 and obtained results are shown in table 4. The comparisons for different mode frequencies with varying percentage of NC for different crack depth are shown in figures 6 to 9. 
Figure 4: Location of cracks on composite beam 
Figure 5: Geometrical model of crack Table 4: Natural frequencies of Different Cracks 
% of NC 
Crack Depth to Width Ratio (a/w) 
frequency of 1st mode(Hz) 
frequency of 2nd mode(Hz) 
Frequency of 3rd mode(Hz) 
Frequency of 4th mode(Hz) 
% of NC 
Crack Depth to Width Ratio (a/w) 
frequency of 1st mode(Hz) 
frequency of 2nd mode(Hz) 
Frequency of 3rd mode(Hz) 
Frequency of 4th mode(Hz) 
0 
0 
1.7783 
11.14 
31.194 
61.142 
1 
0 
1.8553 
11.623 
32.544 
63.785 
0.25 
1.7727 
11.108 
31.135 
60.85 
0.25 
1.8506 
11.596 
32.502 
63.522 
0.5 
1.7511 
10.977 
30.915 
59.674 
0.5 
1.8267 
11.452 
32.251 
62.245 
0.8 
1.6253 
10.307 
29.604 
54.129 
0.8 
1.6947 
10.746 
30.871 
56.429 
3 
0 
1.8621 
11.666 
32.662 
64.004 
5 
0 
1.9104 
11.969 
33.509 
65.665 
0.25 
1.8564 
11.633 
32.603 
63.702 
0.25 
1.9046 
11.935 
33.449 
65.355 
0.5 
1.8329 
11.49 
32.36 
62.429 
0.5 
1.8805 
11.789 
33.2 
64.051 
0.8 
1.6983 
10.767 
30.944 
56.518 
0.8 
1.7424 
11.047 
31.749 
57.989 7 0 1.968 12.33 34.52 67.648 9 0 1.989 12.461 34.889 68.376 0.25 1.9618 12.293 34.453 67.32 0.25 1.9832 12.427 34.83 68.061 0.5 1.937 12.143 34.198 65.98 0.5 1.9584 12.277 34.576 66.72 0.8 1.795 11.381 32.707 59.743 0.8 1.8157 11.513 33.081 60.443 11 0 1.925 12.06 33.768 66.189 13 0 2.1391 13.401 37.523 73.549 0.25 1.9189 12.025 33.704 65.872 0.25 2.132 13.36 37.446 73.185 0.5 1.8957 11.884 33.468 64.607 0.5 2.1061 13.203 37.183 71.777 0.8 1.7602 11.162 32.056 58.628 0.8 1.9554 12.4 35.613 65.129 15 0 2.141 13.413 37.556 73.607 15 0.5 2.1082 13.216 37.221 71.834 0.25 2.1346 13.376 37.49 73.264 0.8 1.9556 12.401 35.626 65.116
Free Vibration Analysis Of Polyproplyne- Nanoclay Composite Beam With Crack 
| IJMER | ISSN: 2249–6645 | www.ijmer.com | Vol. 4 | Iss.7| July. 2014 | 45| 
Figure 6: Comparison of Natural Frequency with different % of NC for 0 crack depth to width ratio Figure 7: Comparison of Natural Frequency with different % of NC for 0.25 crack depth to width ratio Figure 8: Comparison of Natural Frequency with different % of NC for 0.5 crack depth to width ratio Figure 9: Comparison of Natural Frequency with different % of NC for 0.8 crack depth to width ratio 
IV. Conclusions After studying different compositions of NC in the composite beam with different crack depths, the following conclusions are there. 
 Frequency of beam increases with increase in NC %. 
 Frequency of beam decreases with increase in crack depth. 
 Percentage of change of frequency is almost all negligible for variation of NC at same crack depth. 
REFERENCES [1] J. Karger-Kocsis, T. Harmia and T. Czigany, “Comparison of the Fracture and Failure Behavior of Polypropylene Composites Reinforced by Long Glass Fibers and by Glass Mats,” Composites Science and Technology, Vol. 54, pp. 287-298,No. 3, 1995. [2] J. Liakus, B. Wang, R. Cipra and T. Siegmund, “Processing– Microstructure-Property Predictions for Short Fiber Reinforced Composite Structures Based on a Spray Deposition Process,” Composite Structures, Vol. 61, No. 4, pp. 363-374,2003. [3] G. Ben-Dor, A. Dubinsky and T. Elperin, “An Engineering Approach to Shape Optimization of Impactors against Fiber-Reinforced Plastic Laminates,” Composites Part B: Engineering, Vol. 40, pp. 181-188 , No. 3, 2009. [4] M. Bhattacharya and A. K. Bhowmick, “Polymer–Filler Interaction in Nanocomposites: New Interface Area Function to Investigate Swelling Behavior and Young’s Modulus,” Polymer, Vol. 49, pp. 4808- 4818 No. 22, 2008. [5] T. A. Rajesh and D. Kumar, “Recent Progress in the Development of Nano-Structured Conducting Polymers Nanocomposites for Sensor Applications,” Sensors and Actuators B: Chemical, Vol. 136, No. 1, 2009, pp. 275-286. [6] L. Kumari, T. Zhang, G. H. Du, W. Z. Li, Q. W. Wang, A. Datye and K. H. Wu, “Thermal Properties of CNTAlumina Nanocomposites,” Composites Science and Technology, Vol. 68, No. 9, pp. 2178-2183, 2008. [9] D. Sikdar, D. R. Katti, K. S. Katti and R. Bhowmik, “Insight into Molecular Interactions between Constituentsin Polymer Clay Nanocomposites,” Polymer, Vol. 47, No. 14, pp. 5196-5205, 2006.
Free Vibration Analysis Of Polyproplyne- Nanoclay Composite Beam With Crack 
| IJMER | ISSN: 2249–6645 | www.ijmer.com | Vol. 4 | Iss.7| July. 2014 | 46| 
[10] J. G. Zhang, D. D. Jiang and C. A. Wilkie, “Polyethyl ene and Polypropylene Nanocomposites Based upon an Oligomerically Modified Clay,” Thermochimica Acta, Vol. 430, No. 1-2, pp. 107-113, 2005. [11] Y. Dong and D. Bhattacharyya, “Mapping the Real Micro/Nanostructures for the Prediction of Elastic Moduli of Polypropylene/Clay Nanocomposites,” Polymer, Vol. 51, pp. 816-824, No. 3, 2010. [12] L. Cauvin, D. Kondo, M. Brieu and N. Bhatnagar, “Mechanical Properties of Polypropylene Layered Silicate Nanocomposites: Characterization and Micro- Macro Modelling,” Polymer Testing, Vol. 29,pp. 245-250,No. 2, 2010. [13] N. A. Siddiqui, R. S. C. Woo, J.-K. Kim, C. C. K. Leung and A. Munir, “Mode I Interlaminar Fracture Behavior and Mechanical Properties of CFRPs with Nanoclay-Filled Epoxy Matrix,” Composites Part A: Applied Science and Manufacturing, Vol. 38, pp. 449-460, No. 2, 2007. [14] B. Cotterell, J. Y. H. Chia and K. Hbaieb, “Fracture Mechanisms and Fracture Toughness in Semicrystalline Polymer Nanocomposites,” Engineering Fracture Mechanics, Vol. 74, pp. 1054-1078, No. 7, 2007. [15] vibration analysis of cracked cantilever beam withsuitable boundary conditions-J. Yan1 , J. C. Lee2, C. W. Lee2, D. W. Kang2, Y. J. Kang2,andS.H.Ahn1. [16] https://www.efunda.com/materials/polymers/properties/polymer_datasheet.cfm?MajorID=P-TP&MinorID=1. [17] M. N. Bureau, M.-T. T.-T. and F. Perrin-Sarazin, “Essential Work of Fracture and Failure Mechanisms of Polypropylene-Clay Nanocomposites,” Engineering Fracture Mechanics, Vol. 73, pp. 2360- 2374, No, 16, 2006. [18] http://en.wikipedia.org/wiki/Polypropylene [19] Vibration Analysis of Cracked beam byMogal Shyam Prabhakar, Master of Technology In Machine Design and AnalysisNational Institute of Technology ,Rourkela.

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Free Vibration Analysis of Polyproplyne- Nanoclay Composite Beam with Crack

  • 1. International OPEN ACCESS Journal Of Modern Engineering Research (IJMER) | IJMER | ISSN: 2249–6645 | www.ijmer.com | Vol. 4 | Iss.7| July. 2014 | 40| Free Vibration Analysis of Polyproplyne- Nanoclay Composite Beam with Crack Narra. Tilak Ratan1, Dr. G. Vijay Kumar2, M. Rajya Lakshmi3 1(Dept. of Mechanical Engineering, PVP Siddhartha Institute of Technology, India 2(Professor, Dept. of Mechanical Engineering PVP Siddhartha Institute of Technology, India 3(Asst. Professor, Dept. of Mechanical Engineering, PVP Siddhartha Institute of Technology, India I. INTRODUCTION Fiber Reinforced Plastics (FRP) are commonly used in aerospace, automotive and other engineering applications mainly because of their high strength-to-weight ratio, high stiffness, good resistance to fatigue, and corrosion resistance. Reinforced fibers are usually added in the form of continuous or chopped fibers in a polymer matrix. Each type of these reinforcement fibers has their benefits and limitations in applications. A short fiber reinforced composites can have better processing properties and can be moldable into complex shaped components. Long fiber reinforced composites, on the other hand, provide enhanced strength and stiffness properties as per the desired directions. Various types of synthetic and natural fibers reinforced plastics are presently studied in literature, namely, glass fiber, carbon fiber, boron, alumina, oxide/carbide and sisal/jute based fibers in a polymer matrix. In addition to these fiber reinforced composites, particle reinforced polymer composites are also widely investigated. In these particle filled composites, various types of nano- and micro-scale particles are used. Nano particle reinforced polymer composites gained special attention due to their superior and improved properties when compared to their corresponding micro-scale particles. Nano clays, carbon nano tubes and alumina/oxide based particles are widely used as nano particle reinforcements in polymer matrices. Polymer-Clay Nano composites (PCN) are a relatively new area of research in particle filled composites, and consists of Nano Clay (NC) as the reinforcement and a polymer serves as the matrix material. The addition of small amounts of clay (0 to 15% wt) in a polymer matrix leads to improved mechanical, thermal and barrier properties. The addition of nano clays in a polymer matrix may result in the formation of two types of nano composite structures, namely, intercalated and exfoliated nanostructures. In an intercalated structure, the host polymer matrix enters into the interlayer spacing of the nano clay and increases the interlayer spacing but maintains the parallel arrangement of the nano layers of clay in the matrix. If the nano layers of clays are randomly dispersed in the matrix, then the structure is called an exfoliated structure. In practice, exfoliated structures provide enhanced and improved properties due to their excellent dispersions and improved aspect ratio. The addition of the NC in the Ply Propylene (PP) matrix increases the thermal stability in air medium, increases physical properties (dimensional stability), improves flame retardant properties increased thermal- oxidative stability, and improves mechanical properties, fracture properties and gas barrier properties. Several studies were conducted with various types of clay concentrations and compatabilizers. The main applications of PP materials are home appliances such as, chairs and toys, clothing, medical, EPP toy air craft. Crack is initiation of the wrecking of material in some cases. Strength plays very key role for crack growth. If material has high strength, crack will grow slowly otherwise, crack will propagate quickly. And frequency analysis is one of the most promising techniques to detect crack depth. If crack depth increases, then, frequency will down in free vibration. In this paper, efforts have been going made through PP- NC composite beam for un-cracked and cracked with different crack to depth ratios. Abstract: Vibration analysis is one of the most promising techniques to detect the crack. In this paper, Poly Propylene - Nano Clay is analyzed for it’s free vibration. The proposed composite beam is modeled with crack. Analysis is done by using Finite element package ANSYS-14.5. The Nano Clay in composite is varied from 0 to 15 percentage (0,1,3,5,7,9,11,13,15) and crack depth to width ratios are chosen as, 0,0.25,0.5,0.8. Impact of varying percentage of NC and varying crack depths on natural frequency are analyzed using free vibration analysis. Keywords: Nano Clay-Poly Proplyne composite Cantilever beam, Free vibration Analysis.
  • 2. Free Vibration Analysis Of Polyproplyne- Nanoclay Composite Beam With Crack | IJMER | ISSN: 2249–6645 | www.ijmer.com | Vol. 4 | Iss.7| July. 2014 | 41| A -Material Properties Material properties were extracted from research papers by J. Yan1[15] and density was calculated from Rule of mixture. Properties of material for different percentages of nano clay with Poly propylene are listed in table 1. Table 1: Mechanical properties of Poly Propylene - Nano Clay for different % of NC % of NC Yong’s Modulus (Gpa) Poisons ratio Density (Kg/m3) X 103 0 1.56 0.35 1.45 1 1.7 0.34 1.45 3 1.72 0.28 1.45 5 1.81 0.28 1.46 7 1.92 0.29 1.46 9 1.96 0.31 1.47 11 1.83 0.36 1.47 13 2.26 0.36 1.47 15 2.27 0.33 1.48 B- Steps involved in detecting frequencies of cracked beam main steps involved to detect frequencies of cracked beam are, 1) Natural frequencies of un-cracked beam for different composition are determined theoretically. 2) Natural frequencies of un-cracked beam for different compositions are estimated in ANSYS 14.5. 3) Theoretical results are compared with ANSYS 14.5 Results. 4) Natural frequencies of composite beam for different % of NC are estimated using ANSYS 14.5 for different crack depths. II. THEORETICAL CALCULATIONS Theoretical calculations are made through the following formulae for four modes of natural frequencies and results are shown in table 2. Where, L=Length of the beam, E=Young’s modulus of material, I=Moment of inertia of cross section, A=Area of cross section, ρ=Density of material. Table 2: Variation of frequency with change in NC % with theory % of NC frequency of 1stmode(Hz) frequency of 2ndmode(Hz) frequency of 3rd mode(Hz) Frequency of 4th mode(Hz) 0 1.76 11.0606 31.0199 60.833
  • 3. Free Vibration Analysis Of Polyproplyne- Nanoclay Composite Beam With Crack | IJMER | ISSN: 2249–6645 | www.ijmer.com | Vol. 4 | Iss.7| July. 2014 | 42| 1 1.8474 11.5262 32.3818 63.5041 3 1.8574 11.6087 32.5571 63.8478 5 1.9054 11.9087 33.3984 65.4978 7 1.9624 12.265 35.4775 69.575 9 1.9819 12.3868 34.7393 68.1274 11 1.915 12.9687 33.5667 65.8278 13 2.1282 13.3025 37.3039 73.1568 15 2.1319 13.3243 37.3686 73.2836 III. FINITE ELEMENT MODELING The ANSYS 14.5 finite element program was used for free vibration of the cracked beams. A 20-node three-dimensional structural solid element under SOLID 186 was selected to model the beam. The beam was discredited into 1045 elements with 2318 nodes. Geometrical shape of the beam is shown in figure 1. Cantilever boundary condition was considered by constraining all degrees of freedoms of the nodes located on the left end of the beam. The subspace mode extraction method was used to calculate the natural frequencies of the beam and mode shapes are shown in figure 2 and results are in table 3. Figure 1 : Geometrical model for un-cracked beam 2-a: 1st mode-1.7783Hz frequency 2-b: 2nd mode-11.14Hz frequency
  • 4. Free Vibration Analysis Of Polyproplyne- Nanoclay Composite Beam With Crack | IJMER | ISSN: 2249–6645 | www.ijmer.com | Vol. 4 | Iss.7| July. 2014 | 43| 2-c: 3rd mode-31.194Hz frequency 2-d: 4th mode-61.142Hz frequency Figure 2: Mode Shapes of un-Cracked Beam for 0% Nanoclay Table 3: Variation of frequency with change in NC % with simulation % of NC frequency of 1stmode(Hz) frequency of 2ndmode(Hz) Frequency of 3rdmode(Hz) frequency of 4thmode(Hz) o 1.77827 11.1405 31.1936 61.142 1 1.85523 11.623 32.544 63.785 3 1.8621 11.666 32.662 64.004 5 1.9104 11.963 33.509 65.665 7 1.968 12.33 34.52 67.648 9 1.989 12.461 34.889 68.376 11 1.925 12.06 33.768 66.189 13 2.1391 13.401 37.523 73.549 15 2.141 13.413 37.556 73.607 IV. Comparison of results After comparison of both theoretical and ANSYS-14.5 results, the difference between both results is negligible and comparison of frequency is shown in figure 3. Hence, the analysis of cracked beam is extended in ANSYS-14.5 package. Figure 3: Comparision of theoritical and ANSYS-14.5 results for different % of Nano Clay.
  • 5. Free Vibration Analysis Of Polyproplyne- Nanoclay Composite Beam With Crack | IJMER | ISSN: 2249–6645 | www.ijmer.com | Vol. 4 | Iss.7| July. 2014 | 44| V. Results After comparison of the both theoretical and ANSYS-14.5 results, Procedure could be verified in ANSYS-14.5 from the journal [19] for Aluminum material. Same results were obtained from that procedure. Hence, the same procedure is adopted for extracting natural frequencies of cracked beam as shown in figure 4 and 5 and obtained results are shown in table 4. The comparisons for different mode frequencies with varying percentage of NC for different crack depth are shown in figures 6 to 9. Figure 4: Location of cracks on composite beam Figure 5: Geometrical model of crack Table 4: Natural frequencies of Different Cracks % of NC Crack Depth to Width Ratio (a/w) frequency of 1st mode(Hz) frequency of 2nd mode(Hz) Frequency of 3rd mode(Hz) Frequency of 4th mode(Hz) % of NC Crack Depth to Width Ratio (a/w) frequency of 1st mode(Hz) frequency of 2nd mode(Hz) Frequency of 3rd mode(Hz) Frequency of 4th mode(Hz) 0 0 1.7783 11.14 31.194 61.142 1 0 1.8553 11.623 32.544 63.785 0.25 1.7727 11.108 31.135 60.85 0.25 1.8506 11.596 32.502 63.522 0.5 1.7511 10.977 30.915 59.674 0.5 1.8267 11.452 32.251 62.245 0.8 1.6253 10.307 29.604 54.129 0.8 1.6947 10.746 30.871 56.429 3 0 1.8621 11.666 32.662 64.004 5 0 1.9104 11.969 33.509 65.665 0.25 1.8564 11.633 32.603 63.702 0.25 1.9046 11.935 33.449 65.355 0.5 1.8329 11.49 32.36 62.429 0.5 1.8805 11.789 33.2 64.051 0.8 1.6983 10.767 30.944 56.518 0.8 1.7424 11.047 31.749 57.989 7 0 1.968 12.33 34.52 67.648 9 0 1.989 12.461 34.889 68.376 0.25 1.9618 12.293 34.453 67.32 0.25 1.9832 12.427 34.83 68.061 0.5 1.937 12.143 34.198 65.98 0.5 1.9584 12.277 34.576 66.72 0.8 1.795 11.381 32.707 59.743 0.8 1.8157 11.513 33.081 60.443 11 0 1.925 12.06 33.768 66.189 13 0 2.1391 13.401 37.523 73.549 0.25 1.9189 12.025 33.704 65.872 0.25 2.132 13.36 37.446 73.185 0.5 1.8957 11.884 33.468 64.607 0.5 2.1061 13.203 37.183 71.777 0.8 1.7602 11.162 32.056 58.628 0.8 1.9554 12.4 35.613 65.129 15 0 2.141 13.413 37.556 73.607 15 0.5 2.1082 13.216 37.221 71.834 0.25 2.1346 13.376 37.49 73.264 0.8 1.9556 12.401 35.626 65.116
  • 6. Free Vibration Analysis Of Polyproplyne- Nanoclay Composite Beam With Crack | IJMER | ISSN: 2249–6645 | www.ijmer.com | Vol. 4 | Iss.7| July. 2014 | 45| Figure 6: Comparison of Natural Frequency with different % of NC for 0 crack depth to width ratio Figure 7: Comparison of Natural Frequency with different % of NC for 0.25 crack depth to width ratio Figure 8: Comparison of Natural Frequency with different % of NC for 0.5 crack depth to width ratio Figure 9: Comparison of Natural Frequency with different % of NC for 0.8 crack depth to width ratio IV. Conclusions After studying different compositions of NC in the composite beam with different crack depths, the following conclusions are there.  Frequency of beam increases with increase in NC %.  Frequency of beam decreases with increase in crack depth.  Percentage of change of frequency is almost all negligible for variation of NC at same crack depth. REFERENCES [1] J. Karger-Kocsis, T. Harmia and T. Czigany, “Comparison of the Fracture and Failure Behavior of Polypropylene Composites Reinforced by Long Glass Fibers and by Glass Mats,” Composites Science and Technology, Vol. 54, pp. 287-298,No. 3, 1995. [2] J. Liakus, B. Wang, R. Cipra and T. Siegmund, “Processing– Microstructure-Property Predictions for Short Fiber Reinforced Composite Structures Based on a Spray Deposition Process,” Composite Structures, Vol. 61, No. 4, pp. 363-374,2003. [3] G. Ben-Dor, A. Dubinsky and T. Elperin, “An Engineering Approach to Shape Optimization of Impactors against Fiber-Reinforced Plastic Laminates,” Composites Part B: Engineering, Vol. 40, pp. 181-188 , No. 3, 2009. [4] M. Bhattacharya and A. K. Bhowmick, “Polymer–Filler Interaction in Nanocomposites: New Interface Area Function to Investigate Swelling Behavior and Young’s Modulus,” Polymer, Vol. 49, pp. 4808- 4818 No. 22, 2008. [5] T. A. Rajesh and D. Kumar, “Recent Progress in the Development of Nano-Structured Conducting Polymers Nanocomposites for Sensor Applications,” Sensors and Actuators B: Chemical, Vol. 136, No. 1, 2009, pp. 275-286. [6] L. Kumari, T. Zhang, G. H. Du, W. Z. Li, Q. W. Wang, A. Datye and K. H. Wu, “Thermal Properties of CNTAlumina Nanocomposites,” Composites Science and Technology, Vol. 68, No. 9, pp. 2178-2183, 2008. [9] D. Sikdar, D. R. Katti, K. S. Katti and R. Bhowmik, “Insight into Molecular Interactions between Constituentsin Polymer Clay Nanocomposites,” Polymer, Vol. 47, No. 14, pp. 5196-5205, 2006.
  • 7. Free Vibration Analysis Of Polyproplyne- Nanoclay Composite Beam With Crack | IJMER | ISSN: 2249–6645 | www.ijmer.com | Vol. 4 | Iss.7| July. 2014 | 46| [10] J. G. Zhang, D. D. Jiang and C. A. Wilkie, “Polyethyl ene and Polypropylene Nanocomposites Based upon an Oligomerically Modified Clay,” Thermochimica Acta, Vol. 430, No. 1-2, pp. 107-113, 2005. [11] Y. Dong and D. Bhattacharyya, “Mapping the Real Micro/Nanostructures for the Prediction of Elastic Moduli of Polypropylene/Clay Nanocomposites,” Polymer, Vol. 51, pp. 816-824, No. 3, 2010. [12] L. Cauvin, D. Kondo, M. Brieu and N. Bhatnagar, “Mechanical Properties of Polypropylene Layered Silicate Nanocomposites: Characterization and Micro- Macro Modelling,” Polymer Testing, Vol. 29,pp. 245-250,No. 2, 2010. [13] N. A. Siddiqui, R. S. C. Woo, J.-K. Kim, C. C. K. Leung and A. Munir, “Mode I Interlaminar Fracture Behavior and Mechanical Properties of CFRPs with Nanoclay-Filled Epoxy Matrix,” Composites Part A: Applied Science and Manufacturing, Vol. 38, pp. 449-460, No. 2, 2007. [14] B. Cotterell, J. Y. H. Chia and K. Hbaieb, “Fracture Mechanisms and Fracture Toughness in Semicrystalline Polymer Nanocomposites,” Engineering Fracture Mechanics, Vol. 74, pp. 1054-1078, No. 7, 2007. [15] vibration analysis of cracked cantilever beam withsuitable boundary conditions-J. Yan1 , J. C. Lee2, C. W. Lee2, D. W. Kang2, Y. J. Kang2,andS.H.Ahn1. [16] https://www.efunda.com/materials/polymers/properties/polymer_datasheet.cfm?MajorID=P-TP&MinorID=1. [17] M. N. Bureau, M.-T. T.-T. and F. Perrin-Sarazin, “Essential Work of Fracture and Failure Mechanisms of Polypropylene-Clay Nanocomposites,” Engineering Fracture Mechanics, Vol. 73, pp. 2360- 2374, No, 16, 2006. [18] http://en.wikipedia.org/wiki/Polypropylene [19] Vibration Analysis of Cracked beam byMogal Shyam Prabhakar, Master of Technology In Machine Design and AnalysisNational Institute of Technology ,Rourkela.