A REVIEW ON CARBON NANO -TUBES PRODUCTION AND ITS MECHANICAL PROPERTIES 1 Prakash Kumar Sen1, Shailendra Kumar Bohidar2 ,Chandan Sharma3, Vivek modi4 , Yagyanarayan Shrivas5, 1, 2 3, 4, 5 Faculty, Kirodimal institute of Technology, Raigarh, Chhattisgarh, India Student, Bachelor of Engg.,Kirodimal Institute of Technology, Raigarh,Chhattisgarh,India nanometers (approximately 50,000 times smaller than the width of a length. Abstract-The present paper give the survey of carbon nanotube technology through this paper an attempt has been made to visualize the carbon nanotube technology. Carbon nanotubes, popularly known as CNTs are molecular-scale tubes of graphitic carbon with outstanding properties. Carbon atoms in a carbon nanotube have a graphitic structure. The tubes can therefore be considered as rolled-up graphite sheets. The strength of the carbon-carbon bonds provides very high strength and modulus. The Young's modulus of the best Nanotubes can be as high as 1000 GPa, approximately 5 times higher than steel. The tensile strength of Nanotubes can be up to 65 GPa, around 50 times higher than steel. They also possess remarkably high electrical and thermal properties. Index Terms- Carbon Nanotubes, Tensile strength, Young’s Modulus. I. INTRODUCTION Carbon nanotubes (CNTs) are tubular cylinders of carbon atoms that have extraordinary mechanical, electrical, thermal, optical and chemical properties At the individual tube level, these unique structures exhibit: 200X the strength and 5X the elasticity of steel; 5X the electrical conductivity ("ballistic transport"), 15X the thermal conductivity and 1,000X the current capacity of copper; at almost half the density of aluminium. As a carbon based product, CNTs have almost none of environmental or physical degradation issues common to metals—thermal expansion and contraction, corrosion and sensitivity to radiation all of which result in greater system failure in performancesensitive applications. This article considers the mechanical properties of carbon nanotubes. Carbon nanotubes (CNTs) are allotropes of carbon. A carbon nanotube is a one-atom thick sheet of graphite (graphene) rolled up into a seamless cylinder with diameter of the order of a nanometre. This results in a nanostructure where the length-to-diameter ratio exceeds 10,000. Such cylindrical carbon molecules have novel properties that make them potentially useful in a wide variety of applications in mechanical, structural, thermal, electrical & electronics, optical, biomedical and other fields of science, engineering & medicine. They exhibit extraordinary strength and unique electrical properties, and are efficient conductors of heat. Their name is de-rived from their size, since the diameter of a nanotube is on the order of a few The first noticeable discovery of carbon nanotubes was reported by Ilijima [1] in 1991, when he found layers of carbo (graphene) rolled into tubular structure in the soot of arc discharge method. The nanotubes consisted of up to several tens of graphitic shells (so called multi-walled carbon nanotubes (MWNT)) with adjacent shell separation of 0.34 nm, diameters of 1 nm and high length/diameter ratio. Ili-jima’s discovery of carbon nanotubes in the insoluble material of arc-burned graphite rods created the buzz that greatly accelerated work on synthesis, production and properties of carbon nanotubes. It took two more years for Iijima and Ichihashi at NEC [2], and Bethune et al. [3] at IBM to synthesize SWNT by addition of transition metal catalysts to carbon in an arc discharge in 1993. Significant contributions to the race for devising method for production of carbon nanotubes were made by la-ser-ablation synthesis of bundles of aligned SWNT with small diameter distribution by Smalley and co- workers at Rice University in 1995 [4] and by catalytic growth of nanotubes by the chemical vapor decomposition (CVD) method by Yacaman et al. [5] II. LITERATURE REVIEW ON CARBON NANOTUBES The Carbon nanotubes (CNT) with carbon atoms, having diameter of nano meter order, and length is in micrometers. According to Qian D. et al. (2002)[6] explained exciting statements about CNTs. “CNT is 100 times stronger than stainless steel and six times lighter...” “CNT is as hard as diamond and its thermal capacity is twice that of pure diamond...” “CNT’s current-carrying capacity is 1000 times higher than that of copper...” “CNT is thermally stable up to 4000K...” “CNT can be metallic or semiconducting, depending on their diameter and chirality...”. Carbon nanotubes are the broad area, it can be used to produce nano composites Several research on mechanical properties on CNTs have been done, recent study on wear behaviour on CNT- Al nano composite have been done by U. Abdullahi et al.[7] According to which The composite were fabricated using pure aluminium (Al) (99.7%), with particle size of 78 μm which has nearly spherical shape with 2 some satellite sub-particles obtained from Innovative Pultrusion Sdn Bhd, a local supplier for the aluminium powder was used as a matrix material. The multi walled carbon nano tubes (MWCNTs) with a nominal diameter of 10 nm, length of 5-15 μm, and surface area of 230-280 m2g1 was also obtained from the same supplier in Malaysia and used as a reinforcement. Ethanol was used as a process control agent (PCA) during the ball milling of CNT and Al powders. And the result of wear behaviour shows that CNTs Al nano composite shows lower wear rate than pure aluminium and wear rate of all the tested materials increases with increase in normal applied load. Wear rate decrease with increase in CNTs content from 0-1.5 wt% and increase slightly from 1.5-2 wt%, then increase rapidly after this range of CNT content. A distinctive abrasive and adhesive wear were observed from the morphological image of the worn surface. Hardness increases with increase in CNTs content from 0-1.5 wt% and decreased gradually from 2.0 wt%. Wear resistance increase also within the range of 0-1.5 wt% CNT and decrease subsequently with increasing of CNT content. Smith and Luzzi. 2000 et al.[8] Although various fullerenes can be produced using different ways of vaporizing carbon followed by condensation of the tiny clusters, the presence of an electric field in the arc discharge seems to promote the growth of the long tubules. In addition, a small amount of transition metal powder (i.e. cobalt, nickel, or iron) seems to favor growth of SWNTs. Here the metal clearly serves as a catalyst, preventing the growing tubular structurefrom wrapping around and closing into a smaller fullerene cage. The presence of the catalyst also allows one to lower the operating temperature. The carbon atoms in an NT, neglecting the ends, have 99.4% of the cohesive energy that they would have in perfect crystalline graphite. This is far better than the amount of cohesive energy that would be found in C60. If feeding a cheap hydrocarbon such as ethylene to the NT ever becomes possible, buckyropes will grow, and grow inexpensively in industrial laboratories. Fig 1 Show double wall CNTs Fig.2 shows multiwall CNTs III. MANUFACTURING METHODS OF CARBON NANOTUBES Carbon nano-tubes are very difficult to manufacture although there are several methods Like arc discharge, chemical vapour deposition, laser ablation, flame synthesis, high pressure carbon monoxide (HiPco), electrolysis, which uses different chemical , physical and electrical properties to manufacture the same, which can be summerized by the given figure. Fig.3 Showing the classification of techniques of manufacturing CNTs These all the classification can be understood in three basic broad area which are as follows:1. 2. 3. Physical process Chemical process Miscellaneous process A. PHYSICAL PROCESS Muhammad Musaddique Ali Rafique et al. [9] They are the processes, which makes the use of physical principles of carbon that convert it into nanotubes. Arc discharge and laser ablation are some of the technics under these. They are popular process of carbon nanotubes production. Due to their wide spread popularity they are by far the most widely 3 used processes for nanotubes production for experimental purposes. ARC DISCHARGE METHOD This is one of the oldest methods of carbon nanotube production. First utilized by Iijima [1] in 1991 at NEC’s Fundamental Research Laboratory to produce new type of finite carbon structures consisting of needle-like tubes. The tubes were produced using an arc discharge evaporation method similar to that used for the fullerene synthesis. The carbon needles, ranging from 4 to 30 nm in diameter and up to 1 mm in length, were grown on the negative end of the carbon electrode used for the direct current (DC) arcdischarge evaporation of carbon. During the process Iijima used a pressurized chamber filled with a gas mixture of 10 Torr methane and 40 Torr argon. Two vertical thin electrodes were installed in the center of the chamber (Figure 3.1.1). The lower electrode (cathode) contained a small piece of iron in a shallow dip made purposefully to hold iron. LASER ABLATION PROCESS In the laser ablation process, a pulse laser is made to strike at graphite target in a high temperature reactor in the presence of inert gas such as helium which vaporizes a graphite target. The nanotubes develop on the cooler surfaces of the reactor, as the vaporized carbon condenses. A water-cooled surface is also included in the most practical systems to collect the nanotubes (Fig.5) Fig.5. Showing laser Ablation Process Fig.4. Arc discharge method for production of CNTs The arc was generated by running a DC current of 200A at 20V between the electrodes. The use of the three components, namely argon, iron and methane, was critical for the synthesis of SWNT. Carbon soot produced as result of arc-discharge settled and nanotubes grew on the iron catalysts contained in negative cathode. The nano-tubes had diameters of 1 nm with a broad diameter distribution between 0.7 and 1.65 nm. In a similar process Bethune et al. used thin electrodes with bored holes as anodes, which were filled with a mixture of pure powdered metals (Fe, Ni or Co) (catalysts) and graphite. The electrodes were vaporized with a current of 95 - 105 A in 100 - 500 Torr of Helium. SWNT were also produced by the variant of arc-technique by Journet et al. [10] as well. In his variant, the arc was generated between two graphite electrodes in a reaction chamber under helium atmosphere (660 mbar). This method also gave large yield of carbon nanotubes. Ebbesen and Ajayan, [11] however, reported large-scale synthesis of MWNT by a variant of the standard arc discharge technique as well. This method was first discovered by Smally and coworkers at Rive University in 1995 [4]. At the time of discovery they were studying the effect of laser impingment on metals. They produced high yields (>70%) of Single walled Carbon Nanotubes by laser ablation of graphite rods containing small amounts of Ni and Co at 1200°C. In this method two-step laser ablation was used. Initial laser vaporization pulse was followed by second pulse to vaporise target more rapidly. The two step process minimizes the amount of carbon deposited as soot. Tubes grow in this method on catalysts atoms and continued to grow many catalyst atoms aggregate at the end of the tube. The tubes produced by this method are in the form of mat of ropes 10 20 nm in diameter and up to 100 micron or more in length. By varying temperature, catalyst composition and other process parameters average diameter and length of car-bon nanotube could be varied. B. CHEMICAL PROCESS Chemical Vapour Deposition Chemical vapour deposition (CVD) is the best technique to synthesize CNTs. Rajesh Purohit et al.[12] according to his study In this method, the decomposition of the carbon precursor & CNT formation take place on the surface of catalyst particles. The two most important CVD techniques for synthesis of CNT are the thermal CVD & plasma enhanced CVD (PECVD). CNTs can be produced at relatively low temperatures and their size can be controlled by varying the size of catalyst particles. CVD is used for the large scale production of CNTs. It is achieved by taking a carbon source in the gas phase & using an energy source, such a resistively heated coil, to impart energy to a gaseous carbon molecule. Commonly used carbon sources include 4 methane, carbon monoxide, acetylene etc. This will result in the formation of CNTs, if the proper parameters are maintained. The CNT synthesis using CVD is essentially a two steps process. A catalyst preparation step is the first step followed by actual synthesis of nanotube. The catalyst is generally prepared by sputtering, physical vapour deposition (PVD), dip coating etc. The next step is heating up the substrate in a carbon rich gaseous environment. Temperature for the synthesis of nanotubes in this technique is generally 500 to 1000°C. When compared with the previous two methods, CVD is a simple and economic technique for synthesizing CNTs at relatively low temperature and ambient pressure, but at the cost of crystallinity. It is a versatile process as it harnesses a variety of hydrocarbons in any state (solid, liquid or gas), enables the use of various substrates and allows CNT growths in a variety of forms, such as powder, thin or thick films, aligned or entangled, straight or coiled, or even a desired architecture of nanotubes at predefined sites on a patterned substrate. It also offers better control over growth parameters. Fig.6 diameter. Hence, metal nanoparticles of controlled size can be used to grow CNTs of controlled diameter. Thin films of catalyst coated onto various substrates have also been proved successful in achieving uniform CNT deposits. In addition, the material, morphology and textural properties of the substrate greatly affect the yield and quality of the resulting CNTs. Fig.6. Scheme of chemical vapour deposition method for production of CNTs Fig. shows a schematic diagram of the setup used for CNT growth by CVD in its simplest form. The process involves passing a hydrocarbon vapour (typically for 15-60 minutes) through a tube furnace in which a catalyst material is present at sufficiently high temperature (600-1200°C) to decompose the hydrocarbon. CNTs grow over the catalyst and are collected when the system is cooled to room temperature. When a liquid hydrocarbon (benzene, alcohol, etc.) is being employed, it is heated in a flask and an inert gas is purged through it to carry the vapour into the reaction furnace. The design of the CVD reactor depends on whether the carbon precursors are liquid or gas. Liquid carbon precursors often use a bubbler to vaporize the reactants, and a carrier gas (reactive gases such as H2 or inert gas such as N2 or Ar) to transport the vaporized reactants into the CVD reactor. The three main parameters which affect CNT growth in CVD are the hydrocarbon, catalyst and growth temperature. Generally, low-temperature CVD (600-900°C) yields MWNTs, whereas a higher temperature (900 1200°C) reaction favors SWNT growth, indicating that SWNTs have a higher energy of formation, probably owing to their small diameters, which results in high curvature and high strain energy. The catalyst particle size has been found to dictate the nanotube V. CONCLUSION IV. ESSENTIAL PROPERTIES OF CNTs On the basis of study on above different techniques for production of CNTs, it is observed that The arc discharge method and laser ablation method are having difficulty in availability of raw material where as chemical vapour deposition are having abundantly availability of raw material. Energy requirement in arc discharge and laser ablation are high where as chemical vapour deposition is moderate. It is difficult to control the process in arc discharge and laser ablation where as in chemical vapour depotion it is easy due to full automation. The design aspect of arc discharge and laser ablation are quite complicated where as in chemical deposition reactor can be made as much large as possible. Production rate of arc discharge and laser ablation comparatively lower than chemical vapour deposition. There is no prior requirement of refining treatment(post treatment) in chemical vapour deposition whereas, required by arc discharge and laser ablation.[12] On discussion part after this study several conclusions were made, The Significant improvement in current stage of electronics can be achieved, if the proper growth parameters could be regulated for the production of CNTs. In the relative phenomena’s of CNT, its mechanical properties and unique electronic properties make them both interesting as well as potentially very useful in future technologies. Both the laser ablation technology method and arc discharge technology method surfer from the disadvantages of being highly expensive and costly and un-economical methods of production of carbon nano-tubes on large scale, despite they yield high quality carbon nanotubes with reasonable high yield. In this process the Chemical Vapour Deposition can be considered as economical method of production of high purity Single Walled Carbon Nanotubes (SWNT) on large scale. Significant improvement in current stage of electronics can be achieved, if the proper growth parameters could be regulated for the production of CNT. CNTs possess exceptionally high stiffness, strength and resilience, as well as superior electrical and thermal properties, which makes it the ultimate reinforcing material for the nano Composites. 5 VI. REFERENCES S. Iijima, “Helical Microtubules of Graphitic Carbon,” Nature, Vol. 354 1991, p. 56-58. doi:10.1038/354056a0 [2]. S. Iijima, T. Ichihashi, “Single-Shell Carbon Nanotubes of 1-Nm Diameter,” Nature, Vol. 363, 1993, pp. 603-605. [3]. D. S. Bethune, C. H. Kiang, M. S. De Vries, G. Gorman, R. Savoy, J. Vazquez and R. Beyers, “Cobalt-Catalysed Growth of Carbon Nanotubes with Single-Atomic-Layer Walls,” Nature, Vol. 363, 1993, pp. 605-607. [4]. T. Guo, P. Nikolaev, A. Thess, D. T. Colbert and R. E. Smalley, “Catalytic Growth of Single-Walled Nanotubes by Laser Vaporization,” Chemical Physics Letters, Vol. 243, No. 1-2, 1995, pp. 49-54 [5]. M. J. Yacaman, M. M. Yoshida, L. Rendon and J. G. Santiesteban, “Catalytic Growth of Carbon Microtubules with Fullerene Structure,” Applied Physics Letters, Vol. 62, No. 2, 1993, pp. 202-204 [6]. Qian D., Wagner GJ., Liu WK., Yu M-F., Ruoff RS, 2002. “Mechanics of Carbon Nanotubes”. Appl. Mech. Rev. 55: 480-545. Rohsenow WM., Hartnett JP. Ganic EN., 1985. “Handbook of heat transfer fundamentals”; MacGraw-Hill book Co.; New York. [7]. U.Abdullahia, M.A. Malequea*, and U. Nirmalb “Wear mechanisms map of CNT-Al nanocomposite” The Malaysian International Tribology Conference 2013, MITC2013. [8]. Smith, B. and D. Luzzi (2000). “Formation mechanism of fullerene peapods and coaxial tubes: a path to large scale synthesis.” Chemical Physics Letters 321: 169-174 [9]. Muhammad Musaddique Ali Rafique*, Javed Iqbal, “production of nano composite by different routes – A Review” Journal of Encapsulation and Adsorption Sciences, 2011, 1, 29-34. [10]. C. Journet, W. K. Maser, P. Bernier, A. Loiseau, M. Lamy De La Chapelle, S. Lefrant, P. Deniard, R. Lee and J.E. Fischer, “Large Scale Production of Single Walled Carbon Nanotubes by the Electric Arc Technique,” Nature, Vol. 388, 1997, pp. 756-758. [11]. T. W. Ebbesen, P. M. Ajayan, “Large Scale Synthesis of Carbon Nanotubes,” Nature, Vol. 358, 1992, pp. 220-222 [12]. Rajesh Purohita, Kuldeep Purohita, Saraswati Rana, R. S. Ranaa and Vivek Patel, “Carbon Nanotubes and Their Growth Methods” 3rd International Conference on Materials Processing and Characterisation (ICMPC 2014), Procedia Materials Science 6 (2014) 716 – 728 [1].