Variations in Specific Heat and Microstructure in Natural Rubber Filled with Different Fillers as Studied by Differential Scanning Calorimetry
1Physics Department, Visva-Bharati Central University, P.O.- Santiniketan, West Bengal, India
2Centre for Nanoscience and Nanotechnology, Mahatma Gandhi University, Kottayam, Kerala, India
The variation of specific heat (Cp) of natural rubber (NR) is studied by Differential Scanning Calorimetry (DSC). The NR samples are filled with different fillers (nanoclay, TiO2, and nanosilica) at different concentrations. The DSC measurements are done in N2 atmosphere with constant pressure of 0.3 bar to prevent any oxidation of the samples. The temperature has been varied up to 210°C from -40°C at a constant heating rate of 10°C \min throughout the experiment and Proteus analysis software is used to study the variation of specific heat (Cp) as function of both temperature and filler concentrations. The investigation shows that the Cp values increase with the increase of filler concentrations. Due to nanometer range diameter, these fillers fill up some of the free volume holes of NR sample. The fillers also make cross-link with NR chains causing an increase the molecular weight of NR as well as the Cp values. Thus the fillers act as active fillers for NR sample.
At a glance: Figures
Keywords: differential scanning calorimetry, natural rubber, fillers, specific heat, free volume
Journal of Polymer and Biopolymer Physics Chemistry, 2014 2 (1),
Received December 24, 2013; Revised March 18, 2014; Accepted March 20, 2014Copyright: © 2014 Science and Education Publishing. All Rights Reserved.
Cite this article:
- Mandal, Arunava, et al. "Variations in Specific Heat and Microstructure in Natural Rubber Filled with Different Fillers as Studied by Differential Scanning Calorimetry." Journal of Polymer and Biopolymer Physics Chemistry 2.1 (2014): 25-28.
- Mandal, A. , Pan, S. , Mukherjee, S. , Saha, A. K. , Thomas, S. , & Sengupta, A. (2014). Variations in Specific Heat and Microstructure in Natural Rubber Filled with Different Fillers as Studied by Differential Scanning Calorimetry. Journal of Polymer and Biopolymer Physics Chemistry, 2(1), 25-28.
- Mandal, Arunava, Sandip Pan, Subrata Mukherjee, Achintya K. Saha, Sabu Thomas, and Asmita Sengupta. "Variations in Specific Heat and Microstructure in Natural Rubber Filled with Different Fillers as Studied by Differential Scanning Calorimetry." Journal of Polymer and Biopolymer Physics Chemistry 2, no. 1 (2014): 25-28.
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In recent years in polymer research, a key problem is to relate the atomic scale free volume to the thermal and mechanical properties of polymer . These free volumes appear, in the amorphous region of the polymers due to their structural disorder, in form of many irregularly shaped cavities or holes of atomic and molecular dimension. The presence of free volume decreases the density of the polymer and effect remarkably on the mechanical and thermal properties. Free volume is affected by irradiation of ion beams, aging and by addition of various fillers [2-7].
Raw natural rubber (NR) undergoes curing process for it to be useful for any practical and industrial purpose. It is therefore compounded by mixing with varity of materials such as sulfur, zinc oxide, stearic acid etc. and then cure in a process called vulcanization . During this process, NR forms cross links with sulfur improving its quality and usefulness . Rubber is a class of polymeric materials, which is expected to show rubber elasticity when in use. Natural rubber is in use for its versatility as an elastomeric material. Polymeric materials such as natural rubber (NR), containing filler particles of nanometer size have excellent physical, mechanical, and thermal properties compared to their conventional micro composite counterparts [10, 11, 12]. The main aim of the addition of fillers into natural rubber is to improve the properties and to cheapen the material for use in material science and industry. Among many types of filler carbon black is the most important filler due to its high ability to improve the quality of NR. But it has a serious drawback. It originates from petroleum and makes the NR black due to pollution. Several groups have studied NR and its blend compounds with different methods such as viscosity measurements, differential scanning calorimetry, dynamic mechanical spectroscopy, positron annihilation spectroscopy etc. [5, 13, 14, 15, 16, 17]. The microstructure of free volume of NR filled with TiO2, Nanosilica(NS), Nanoclay(NC) have been studied by positron annihilation spectroscopy . In this paper an attempt is made to study microstructure and thermal properties NR filled with TiO2, NS, NC at different concentrations by Differential Scanning Calorimetry (DSC). DSC measures the change in thermal properties and microstructures of any sample as a function of temperature.
The heat capacity of a substance can be defined as the amount of heat required to change its temperature by unity. A more useful quantity is the specific heat capacity, which is the heat capacity per unit molecular weight of the substance. The heat capacity of a polymer can be classified into two categories: one is for the “solid” state of the polymer, may be denoted as Cps and the other one is for the “liquid” state of the polymer, may be denoted as Cpl. The behavior of the heat capacities of polymer samples with temperature may be attributed to the localized motion of its molecular segments i.e. it may not be bothered about the presence or the absence of any periodic molecular arrangements [18, 19]. Therefore it can be concluded that the values of Cps for both the amorphous and the crystalline states are closely the same.
A minute study on the variation of the specific heat of the natural rubber (NR) samples with both the fillers concentration and temperature are done in this paper.
2. Experimental2.1. Samples
Natural rubber used for the study was procured from the Rubber Research Institute of India, Kottayam..The molecular weight of NR obtained by light scattering is Mn= 2.68 ×105 g/mol, Mw= 8.38×105 g/mol. All other ingredients used were of commercial grade and were kindly supplied by LANXESS.
NR samples are filled with TiO2 (10 phr, 20 phr, 30 phr, 40 phr), Nanosilica (5 phr, 10 phr, 20 phr) and Nanoclay (2 phr, 5 phr, 10 phr) for the measurements. The filler titanium dioxide, TiO2 (KEMOX RC 800 PG), was kindly supplied by Kerala Minerals and Metals Limited (KMML) Kollam, India. The surface modified nanosilica (AEROSIL R 8200) and nanoclay are obtained from Degussa, Germany. The characteristics of the fillers are given in Table 1, Table 2 and Table 3 respectively.
Formulation of composite mixes is shown in Table 4. Compounding was performed in an open two-roll mixing mill (laboratory size). NR was first masticated on the two-roll mill for about two to three minutes followed by addition of the ingredients. Curing properties were analysed using an Oscillating disc rheometer (Monsanto R-100) at a temperature of 150°C. The composites were cured at their respective cure times in a hydraulic press under a pressure of about 120 bar at 150°C.2.3. Differential Scanning Calorimetry
The Differential Scanning Calorimetry (DSC) measurements carried out by employing 2000 F3 model of DSC with intra-cooler 70 versions that is capable of lowering the temperature up to –70°C and enhancing the temperature up to 600°C. The experiment is performed in N2 atmosphere with constant pressure of 0.3 bar to prevent any oxidation of the samples. The temperature has been varied up to 210°C from -40°C at a constant heating rate of 10°C \min throughout the experiment. The heat difference between the two pans (reference and sample pan respectively) upon heating is determined with respect to the temperature enhancement. Proteus analysis software is used to study the variation of specific heat (Cp) with temperature.
3. Results and Discussion
DSC measures the specific heat (Cp) of any sample by following a very simple and straight forward theory. Since the DSC is at constant pressure, heat flow is equivalent to enthalpy changes
In DSC measurement the specific heat (Cp) of the sample can be determined by comparing it to that of a known sample. In our experiment we have considered sapphire as the standard known sample. The heat that flows into the sample is directly proportional to the specific heat. The heat flow into the sample is given by,
Where dH/dt is the heat flow rate measured in calories/seconds, m is the mass of the sample measured in grams, Cp is the specific heat measured in Calories/gram/°K, dT/dt is the rate of change of temperature in °K/second.
This equation is used in order to derive the final equation which determines the specific heat of the sample given by,
Where Cp′ and m′ are the specific heat and mass of the standard, y and y′ are the ordinate deflections due to the sample and standard respectively measured in centimeters Heat capacity is one of the most important thermal parameter because its macroscopic behavior can be linked with the microstructure of a substance and hence can be treated as an entity capable of illuminating the physical endeavor of atoms or molecules within a substance to maneuver themselves upon heating [18, 19, 20].
Figure 1 Shows the variation of specific heat with both temperature and nanoclay (NC) filler concentrations. Two important observations may be come out from Figure 1. Firstly it is found that specific heat (Cp) of all samples, irrespective of filler concentrations, increase with temperature from a certain temperature -30°C to near about 200°C. Beyond 200°C Cp values shows a sharp decrease due to the onset melting process. The specific heat values also increase below -30°C. Secondly Cp values show a remarkable increase with the nanoclay filler concentration. These two interesting phenomenon can be explained in the light of structural change of NR due to both temperature change and addition of increasing filler concentrations.
The Cp variation of TiO2 filled NR at different concentrations including the reference sample with both temperature and filler concentrations are shown in Figure 2. The variation of Cp values with temperature follows the same pattern as Figure 1. The Cp values increase with TiO2 filler concentration remarkably up to 20 phr. Above 20 phr Cp values are almost same below temperature 75°C and begin to increase with filler concentrations above 75°C.
Figure 3 shows the variation of specific heat of nanosilica filled rubber. The variations of Cp with temperature for this filler also follow same pattern as the previous two. But the variation of Cp values with nanosilica filler concentrations has some different interesting features than the previous two fillers. For nanosilica Cp values increase in a regular way with filler concentrations but rate of increase of Cp values with temperature are greater for 10 phr and 20 phr nanosilica than 5 phr and reference sample. Again the values of Cp of nanosilica filled natural rubber are highest among the above mention three types of fillers. Table 5. shows the values of highest and lowest value of Cp at different concentrations of filler and the reference sample.
In our previous paper it is found that the size of free volume holes of NR sample decreases and the molecular weight increases upon addition of nanoclay, TiO2, and nanosilica fillers. These fillers particles have diameter of nanometer order so they fill up the free volume holes of NR and well interact with NR chain, i.e. cross linking is established causing increase in molecular weight and decrease in amount of free volume of NR sample upon addition of these three fillers. As a result of this cross-linking between NR chain and filler particles Cp values should be increase with the increase of filler concentrations which is well observed. From Table 5. It is also clear that the increase of Cp values highest upon addition of nanosilica. So the role of nanoclay, titanium dioxide and nanosilica as active fillers for NR is confirmed and well fitted to our previous results .
The variations of specific heat of natural rubber filled with different fillers are studied by DSC and the results have been correlated to the microstructure of free volume holes of rubber sample. It is observed that the Cp values increase as the filler concentrations increases for the above mentioned fillers. The variations of Cp clearly reflects that upon loading these three fillers particles, amount of free volume in the rubber sample reduces and molecular weight increases in terms of cross-linking. Hence the segmental motion of the molecules decreases and the Cp value becomes higher. So these fillers act as active fillers for natural rubber and among them nanosilica is the most active filler.
The work is sponsored by SERC Division, D.S.T., Govt. of India, project No. SR/S2/CMP-57/2007.
|||Dlubek, G., Sengupta, A., Pionteck, J., Krause-Rehberg, R., Kaspar Harald and Helmut Lochhaas, K., “Temperature Dependence of the Free Volume in Fluoroelastomers from Positron Lifetime and PVT Experiments”, Macromolecules, 37. 6606-6618. 2004|
|||Vleeshouwers, S., Kluin, J. E., McGervey, J. D., Jamieson, A. M., and Simha, R., “Monte Carlo calculations of hole size distribution: simulation of positron annihilation spectroscopy” J. Polym. Sci., Part B. Polym. Phys., 30. 1429. 1992.|
|||Schmitz, H. and Muller- Plathe, F., “Calculation of the lifetime of positronium in polymers via molecular dynamics simulations”, J. Chem. Phys., 11. 1040. 2000.|
|||Wang, J., Vincent, J. and Quarles, C. A., “Review of positron annihilation spectroscopy studies of rubber with carbon black filler”, Nuclear Instruments and Methods in Physics Research B, 241. 271-275. 2005.|
|||Mandal, A., Mukherjee, S., Pan, S. and Sengupta, A., “positron lifetime measurements in natural rubber with different fillers” Int. Journal of Modern Physics, 22. 112-117. 2013.|
|||Mandal, A., Mukherjee, S., Pan, S., Saha, A. K. and Sengupta, A., “PALS and DSC studies in high energy electron irradiated semicrystalline polypropylene” Int. Conf. on Recent Trends in Applied Physics and Ma terial Science. AIP Conf. Proc. 1536. 839. 2013.|
|||Mandal, A., Pan, S., Mukherjee, S., Saha, A. K. Ranganathaiah, C. and Sengupta, A. “High energy electron irradiated polystyrene: free volume and thermal properties studied by PALS and DSC”, Journal of Polymer and Biopolymer Physics Chemistry, 1. No. 1, 26-30. 2013.|
|||Mogensen, O. E, Positron Annihilation in Chemistry, Springer-Verlag, Barlin, vol. 58, 1995.|
|||Dallas D. Parker , J. L. Koenig , Makio Mori, “Correlation of 13 C NMR Analysis and Physical Testing Results of Natural Rubber” Rubber Chem. Technol. 68. 551. 1995.|
|||Nesterov, A. E. and Lipatov, Y. S., “Compatibilizing effect of filler in binary polymer mixtures” Polymer, 40. 1347-1349. 1999.|
|||Saad A. L. G., El-Sabbagh S.: Compatibility studieson some polymer blend systems by electrical and mechanical techniques. Journal of Applied Polymer Science, 79, 60- 71 2001.|
|||Sae-oui1, P., Sirisinha, C. and Hatthapanit, K., “Effect of blend ratio on aging, oil and ozone resistance of silica-filled chloroprene rubber/natural rubber (CR/NR) blends” Express Polymer Letters 1, No. 1. 8-14. 2007.|
|||Ramesan M. T., Alex R., Khanh N. V., “Studies on the cure and mechanical properties of blends of natural rubber with dichlorocarbene modified styrene-butadi-ene rubber and chloroprene rubber”. Reactive & Functional Polymers, 62, 41-50 2005.|
|||Ismail H., Leong H. C., “Curing characteristics and mechanical properties of natural rubber/chloroprene rubber and epoxidized natural rubber/chloroprene rub-ber blends”, Polymer Testing, 20, 509- 516, 2001.|
|||Kueseng, P.; Sae-oui, P. and Rattanasom, N., “Mechanical and electrical properties of natural rubber and nitrile rubber blends filled with multi-wall carbon nanotube,” Polymer Testing. 32, 731- 738, 2013.|
|||Zhang, P., Shi, X., Yu, G. and Zhao, S., “The structure change of dynamically fatigued unfilled natural rubber vulcanizates,” Journal of Applied Polymer Science, 115. No. 6. 3535- 3541, 2010.|
|||Yehia, A. A.; Mansour, A. A. and Stoll, B. J. “Detection of compatibility of some rubber blends by DSC.” J Thermal Analysis. 48. 1299. 1997.|
|||Pyda, M., “Conformational Heat Capacity of Interacting Systems of Polymer and Water”, Macromolecules, 35. 4009-4016. 2002.|
|||Reading, M. and Hourston, D. J., “Modulated Temperature Differential Scanning Calorimetry: Theoretical and Practical Application in Polymer characterization”, Springer, 2006.|
|||O’Neill, M. J., “Measurement of Specific Heat Functions by Differential Scanning Calorimetry”, Analytical Chemistry, 38 (10). 1331. 1966.|