Next Article in Journal
Unveiling the Influential Factors and Heavy Industrial Applications of Graphene Hybrid Polymer Composites
Previous Article in Journal
New Accomplishments on the Equivalence of the First-Order Displacement-Based Zigzag Theories through a Unified Formulation
Previous Article in Special Issue
Thermal Balance of a Water Thermal Accumulator Based on Phase Change Materials
 
 
Font Type:
Arial Georgia Verdana
Font Size:
Aa Aa Aa
Line Spacing:
Column Width:
Background:
Article

Comparative Investigation of Thermal Properties Improvement of Nano-Enhanced Organic Phase Change Materials

by
Aravindh Madhavankutty Ambika
1,
Gopi Kannan Kalimuthu
2 and
Veerakumar Chinnasamy
3,*
1
Ministry of New and Renewable Energy, New Delhi 110003, India
2
Department of Mechanical Engineering, Indian Institute of Technology (Indian School of Mines), Dhanbad 826004, India
3
Department of Mechanical Engineering, Chosun University, 309 Pilmundaero, Dong-gu, Gwangju 61452, Republic of Korea
*
Author to whom correspondence should be addressed.
J. Compos. Sci. 2024, 8(5), 182; https://doi.org/10.3390/jcs8050182
Submission received: 15 March 2024 / Revised: 25 April 2024 / Accepted: 10 May 2024 / Published: 13 May 2024
(This article belongs to the Special Issue Composites for Energy Storage Applications, Volume II)

Abstract

:
Thermal energy storage (TES) using phase change materials (PCMs) is one of the potential solutions for stockpiling thermal energy and utilizing it for different applications, which results in effective energy usage. The main drawback of organic PCMs in practical applications is poor heat transfer due to low thermal conductivity (TC). Therefore, investigations into nano-enhanced PCMs are being explored to improve their thermophysical properties. In this work, the various thermophysical characteristics of nano-enhanced lauryl alcohol as a PCM were investigated using carbon-based and metallic nanoparticles. The results indicated that the addition of nanoparticles improved its thermal properties and affected other physical properties, such as viscosity. The latent heat was degraded with the addition of nanoparticles. The results revealed that by adding MWCNTs and CuO nanoparticles, a maximum of 82.6% and 49.6% improvement in TC was achieved, respectively. The maximum drop in latent heat during melting and freezing for the PCM with MWCNTs was about 10.1% and 9.3%, respectively, whereas for the PCM with CuO, they were about 11% and 10.3%, respectively. The lowest supercooling for the PCM with MWCNTs and CuO nanoparticles was 8.6 and 8.3 °C, respectively. The present work confirms that nano-enhanced PCMs can be a potential material for storing thermal energy for various applications.

1. Introduction

Reducing energy consumption through more responsible and effective use of energy resources is known as energy conservation. It entails cutting down on energy waste and using practices and technology that reduce energy use while preserving the required comfort or service levels. In addition to being an essential part of sustainable development, energy saving also helps to mitigate climate change, lower greenhouse gas emissions, and encourage environmental stewardship. Various technologies are being practiced for efficient energy usage, and thermal energy storage (TES) is crucial [1]. TES systems have a wide range of industrial applications, offering benefits such as increased energy efficiency, reduced energy costs, and improved process flexibility. TES is used in district heating and cooling networks to store surplus thermal energy during off-peak hours for later use during peak demand periods. It helps balance supply and demand, reduces energy costs, and improves system reliability and stability [2,3]. TES systems are integrated into building HVAC (heating, ventilation, and air conditioning) systems to store thermal energy for space heating or cooling. They help reduce energy consumption, shift energy demand away from peak hours, and improve building comfort and temperature control. TES systems can be classified based on the storage medium, operation principle, and temperature range. Sensible heat storage systems store energy by changing the temperature of a material without changing its phase. Latent heat thermal energy storage (LHTES) systems store energy by changing the phase of a material (solid to liquid or vice versa) while keeping the temperature constant. Thermochemical storage systems store energy through reversible chemical reactions that absorb or release heat. These types of thermal energy storage offer flexibility in terms of storage capacity, operating temperature range, and application suitability, allowing for tailored solutions to meet diverse energy storage needs. Among the different strategies of TES, phase change material (PCM)-based LHTES is more advantageous due to its ability to accumulate more thermal energy and maintain constant temperature storage and retrieval [4]. The PCM undergoes physical phase transformation during the stockpile and retrieval of thermal energy. PCMs can be classified based on several criteria, including their chemical composition, phase change mechanism, temperature range of operation, and application. Generally, PCMs are categorized as organic, inorganic, and eutectic. Organic PCMs are composed of organic compounds, such as paraffins, fatty acids, and esters. Organic PCMs often have high latent heat storage capacity and are typically used in moderate-temperature applications. Even though the PCM-based TES has several advantages, there are certain practical difficulties in applying it for applications, such as poor thermal conductivity (TC), compatibility with the container materials, volume of expansion and stability, etc. The heat transfer ability is a crucial property of a PCM for fast heat storage and retrieval. Various techniques are available for heat transfer enhancement of PCMs, and employing nanoparticles is a novel strategy that is widely used [5,6]. Techniques such as fins, encapsulation [7], shape stabilization [8], and nanoparticle inclusion are adopted to improve the thermal properties. Researchers have shown interest in different PCMs and nano-inclusions to enhance PCM thermophysical properties, which results in an efficient TES system. Using nanoparticles to increase PCMs’ TC is a viable way to improve the material’s overall efficiency and heat transfer capabilities in thermal energy storage applications. Significant increases in TC can be attained by adding nanoparticles to PCM matrices and fine-tuning their dispersion and interaction. This will improve heat transfer performance and efficiency in thermal energy storage applications.
Rashid et al. [9] presented a critical review on recent advances in PCM-based cold TES. This review investigated the experimental and numerical investigations of the heat transfer properties using PCM, factors influencing the TC, nanoparticle inclusion, and encapsulation of PCMs. The same authors reviewed the recent developments and challenges of using PCMs in concrete for TES and utilization [10]. Pereira et al. [11] presented an overview of thermal energy harvesting using NEPCMs. This critical survey provides information on energy harvesting and conversion using PCMs enhanced with nanostructures. Anand et al. [12] prepared a capric acid nano-enhanced (NE) PCM using manganese dioxide nanoparticles at different concentrations and reported that the LH was in the 145–164 kJkg−1 range. Metallic nanoparticle nano-inclusions are beneficial since they have less of an impact on the PCM’s ability to store energy. Ouikhalfan et al. [13] used four distinct nanoparticles (TiO2, CuO, Al2O3, and ZnO) at varying concentrations to create a nanocomposite PCM of myristic acid. The PCM nanocomposites were studied using several characterization methods. The findings showed that myristic acid containing 2 wt% Al2O3 and 2 wt% ZnO is appropriate for use in solar TES applications. Han et al. [14] described a eutectic mixture of KNO3 and NaNO3 with 1 wt% of Al2O3 nanoparticles at various sizes, including 80, 135, 200, 300, and 1000 nm. Their findings demonstrated that the ideal Al2O3 thickness for improving liquid-specific heat at temperatures between 235 and 300 °C was 300 nm. Santosh et al. [15] examined the thermal performance of an Al2O3 nano-dispersed PCM and a surface-roughened PCM and reported his findings. Arshad et al. [16,17] researched the thermophysical properties of nanocomposites containing mono and hybrid nanoparticles. According to their findings, the hybrid nanocomposite PCMs produced have better thermal properties and can be applied to electronic device thermal management. Muzhanje et al. [18] prepared an NE-PCM and studied the physical and thermal characterization. The melting rate was improved threefold with 5 wt% of metallic nanoparticles. Karthikeyan et al. [19] developed a binary eutectic PCM using hybrid nanoparticles, and its thermal properties were investigated using various techniques. The NE-PCM showed a maximum TC improvement of 55.7%. Rashid et al. [20] investigated and reviewed the recent advancement in solidification enhancement of PCM using fins and nanoparticles. The heat recovery potential improvement of an NE-PCM was investigated by Mahdi and Nsofor [21]. The results elucidated that nano-PCMs have improved heat recovery performance and that the degraded concentration of nanoparticles accelerated the PCM solidification. Venkatraman et al. [22] made an investigational study on improved PCM discharging performance using steatite nanoparticles at different concentrations. The discharge performance was significantly improved, and heat was stored and maintained without external energy. Baskakov et al. [23] investigated paraffin with reduced graphene oxide as a thermal battery material. The TC of the paraffin was increased, which resulted in a temperature rise up to 72 °C with two minutes of microwave heating. Xie [24] studied the thermal property enhancement of a salt hydrate PCM with copper nanoparticles and investigated its ability in battery thermal management. Li et al. [25] investigated the improvement of TC using modified carbon nanotubes. The modification strategy improved the dispersion stability significantly. Qiu et al. [26] performed an experimental study on TC enhancement of PCM using modified fly ash. As a result, the LH and TC were improved by 51.7% and 67.7%, respectively.
Carbon-based nanostructures, including carbon nanotubes (CNTs), graphene, and carbon nanofibers (CNFs), offer unique properties that can significantly enhance the thermal properties of materials when incorporated into composites. Carbon-based nanostructures have exceptionally high thermal conductivities due to their one-dimensional (CNTs), two-dimensional (graphene), or three-dimensional (CNFs) structures. When incorporated into composite materials, these nanostructures form conductive networks that facilitate the efficient transfer of heat, resulting in enhanced thermal conductivity of the composite. In applications where heat dissipation is critical, such as electronic devices and thermal management systems, carbon-based nanostructures can help dissipate heat more effectively. The high surface area and TC of nanostructures enable rapid heat transfer away from heat-generating components, reducing operating temperatures and improving device reliability. Carbon-based nanostructures can be functionalized or integrated with PCMs to enhance their TES properties. The high surface area and thermal conductivity of nanostructures facilitate the efficient transfer of heat between the PCM and the surrounding environment, improving the charging and discharging rates of TES systems. Mayilvelnathan and Valan Arasu [27] studied the performance of a TES system using an erythritol PCM with graphene and reported that the TES system efficiency using NE-PCM was increased by 16.29% and 28.48% during stockpiling and retrieval, respectively. Bahiraei et al. [28] experimentally investigated the performance improvement of carbon-based NE-PCM. The graphite-based nanocomposites showed a significant TC improvement for 7.5 and 10 wt% concentration. The thermal efficiency of the eutectic PCM was improved by adding expanded graphite, as studied by Panda et al. [29]. With the 3 wt% of expanded graphite, the TC improved by 232.24%. N-octadecane and graphene nanoparticles at 2 wt% and 5 wt% were used by Zarma et al. [30] to develop a nano-enhanced PCM. The concentrated photovoltaic system’s cell temperature was lowered using the generated nano-enhanced PCM, and the PCM containing 5 wt% graphene had a higher solar mean temperature. Lin et al. [31] created a composite PCM of palmitic acid, including graphene nanoplatelets (GNPs) and SiO2 nanoparticles. According to the results, the composite PCM containing 5 wt% GNPs improved TC by 1.65 times and was advised for thermal energy storage. Sahan et al. [32] investigated the paraffin PCM containing carbon nanotubes and activated carbon. According to the findings, PCM containing carbon nanotubes and activated carbon had increased thermal conductivities by 34.1% and 39.1%, respectively. Moreover, PCM containing carbon nanotubes increased its thermal energy storage capacity by 9.6%, but activated carbon saw no change in this regard. Xu et al. [33] produced a PCM material including water, sodium polyacrylate, and multi-walled carbon nanotubes (MWCNTs). They found that adding 0.1 wt% of MWCNTs enhanced the TC by 19.17%. Bharathiraja et al. [34] investigated the thermal properties of MWCNTs and SiO2 nano-enhanced paraffin wax as a thermal storage medium. By increasing the MWCNT and SiO2 concentration, the melting point was increased slightly, and thermal conductivity was increased. Xu et al. [35] prepared 1-Hexadeol NE-PCM using nano-TiO2, nano-ZnO2, nano-Ag, and graphene nanoplates and investigated their properties. Thermal conductivity was improved significantly by graphene nanoplates.
Fatty acids and fatty alcohols are of great interest among the different PCMs due to their good stability, high thermal storage density, and low corrosiveness. Exploring the improvement using various nanoparticles under different conditions and comparative investigations enables us to improve the thermal efficiency of a TES system. Both carbon-based and metallic nanoparticles contribute equally to improving the PCM thermal characteristics. In this study, two different NE-PCMs were developed using different concentrations of carbon-based MWCNTs and metallic CuO nanoparticles and fatty alcohol as a PCM. Their various thermophysical properties were comparatively examined using several characterization methods, and the findings are displayed. It is anticipated that the findings of this study will contribute to our understanding of the thermophysical modifications in PCMs due to the addition of nanoparticles and provide possible information on the NE-PCM with MWCNTs and CuO nanoparticles to be used as potential TES materials.

2. Materials and Methods

Lauryl alcohol (LA), also called 1-Dodecanol, is a long-chain fatty alcohol that appears to be a clear transparent liquid at 30 °C. It is immiscible in water but soluble in organic solvents. LA (purity: 99%) supplied by Sigma-Aldrich, India, was used as PCM. Copper oxide nanoparticles and MWCNTs supplied by Sigma-Aldrich, India, were used as nano-inclusions. Sodium dodecyl sulphate (SDS) (purity: 95%) from Loba Chemie, India, was employed to stabilize the nanoparticles in the PCM. The properties of the nanoparticles and surfactant are presented in Table 1. All the materials were used for the experiment as supplied without any further processing.
The NE-PCM was formulated through physical mixing followed by an ultrasonic dispersion technique. Ultrasonic dispersion techniques are commonly employed for the synthesis and dispersion of nanoparticles within various matrices, including PCMs. When applied to nano-enhanced PCMs, ultrasonic dispersion techniques facilitate the uniform distribution of nanoparticles throughout the PCM matrix, resulting in enhanced thermal properties and performance. Ultrasonic dispersion involves the application of high-frequency acoustic waves (ultrasound) to a liquid medium containing nanoparticles and the PCM matrix. The ultrasonic waves create cavitation bubbles in the liquid, which collapse violently near the nanoparticles. This leads to localized high temperatures and pressures, promoting the dispersion of nanoparticles and their interaction with the PCM matrix. Ultrasonic dispersion techniques can be easily scaled up for industrial production, making them suitable for large-scale synthesis of nano-enhanced PCMs. As a first step in the process, LA was heated to 45 °C, and a suitable proportion of SDS surfactant was added to it and mixed well through a magnetic stirrer and hot plate. Then, an appropriate amount of MWCNTs and CuO nanoparticles was added to the PCM and surfactant mixture and stirred for 30 min. Then, the mixture was probe sonicated at a frequency of 20 kHz for 1 h, and the temperature was maintained at a constant throughout the process. Finally, the resultant NE-PCM was cooled to room temperature. In the preparation process, 1, 3, and 5 wt% of nanoparticles were used, and the surfactant to the nanoparticle concentration was 1:10.
The thermophysical properties of the prepared NE-PCMs were examined through various characterization techniques. Differential scanning calorimetry (DSC) is a thermal analysis technique used to measure the heat flow into or out of a sample as a function of temperature or time. It is commonly employed in various fields to study the thermal properties of materials, including phase transitions, purity determination, reaction kinetics, and stability. The basic principle of DSC is based on comparing the heat flow to a sample and a reference material as they undergo a controlled temperature program. Any energy difference between the sample and reference is recorded as a function of temperature or time. A typical DSC instrument consists of a sample holder with two compartments: one for the sample and one for the reference material. Both compartments are placed in separate furnaces and are maintained at the same temperature throughout the experiment. As the temperature changes, the instrument measures the heat flow required to keep both compartments at the same temperature. The phase change temperatures and LHs were estimated through DSC analysis using NETZSCH DSC 204 F1 Phoenix. The equipment has a measurement temperature range of −180 °C to 700 °C, and the accuracy of the enthalpy measurement is <1%. The equipment was calibrated with indium as standard material before conducting the measurement. The measurement was performed between −10 and 60 °C at a heating rate of 10 °C.min−1 under a nitrogen atmosphere. Before conducting the analysis, the equipment was calibrated with the standard reference material. Thermogravimetric analysis (TGA) is a thermal analysis technique used to study the weight changes in a sample as a function of temperature (or time) under controlled atmosphere conditions. It is widely used in various fields, including materials science, chemistry, pharmaceuticals, and environmental science, to investigate thermal stability, decomposition kinetics, composition, and purity of materials. The basic principle of TGA involves measuring the weight of a sample as it is subjected to a programmed temperature ramp or isothermal conditions. Any weight loss or gain is indicative of changes occurring within the sample. A typical TGA instrument consists of a sample holder, a balance, a furnace, and a temperature controller. The sample is placed in a crucible or pan, which is then loaded onto a balance. The balance continuously measures the weight of the sample as the temperature changes. The TGA was performed using NETZSCH STA 449 F3 Jupiter. The equipment has a measurement temperature range of −150 °C to 2400 °C, and the resolution of the mass loss measurement is 0.1 µg. The measurement was performed from 25 to 280 °C at a heating rate of 10 °C.min−1. The sample was placed in an open pan to estimate the decomposition temperature.
The KD2 Pro thermal property analyzer is an advanced instrument used for measuring the thermal properties of various solid and liquid materials. The KD2 Pro operates on the transient line source (TLS) technique. In this method, a needle-like probe, which serves as both a heat source and a temperature sensor, is inserted into the material of interest. A known amount of heat is applied to the probe for a short duration, and the resulting temperature change is measured. By analyzing the rate of temperature change over time, the KD2 Pro calculates the thermal properties of the material. The TC was determined through a KD2 Pro thermal property analyzer. The TC at the solid phase is measured using the SH-1 sensor with 10% measurement error, and at the liquid phase, the KS-1 sensor with 5% measurement error was used. During the measurement, the temperature of the sample was controlled by placing it in a double jacket container through which water from the constant thermal bath was circulated. The sample temperature was maintained at 10, 30, and 40 °C, and respective thermal conductivities were measured. The viscosity was measured using Anton Paar SVM 1001 viscometer. The equipment has a viscosity measurement repeatability and reproducibility of 0.1% and 0.35%, respectively. The Anton Paar SVM 1001 viscometer is a sophisticated instrument used for measuring viscosity, a crucial property in various industrial applications. The SVM 1001 is designed to provide accurate and reliable viscosity measurements across a wide range of sample types and viscosities. The SVM 1001 viscometer operates on the rotational viscometry principle. It measures viscosity by rotating a spindle immersed in the sample fluid. The resistance to the spindle rotation is proportional to the viscosity of the fluid. By measuring the torque required to rotate the spindle at a constant speed, the instrument calculates the viscosity of the sample. In order to measure the viscosity of the NE-PCM in its liquid phase, the measurement was executed at 30 °C at all concentrations. The measurement error was about 0.1%, and it was repeated 3 times to ensure the repeatability.

3. Results

The DSC measurement results are shown in Figure 1a,b. The onset melting and solidification points for LA were 22 and 20 °C, respectively. The LH of melting and solidification were 217 and 213 Jg−1, respectively. The DSC results of NE-PCMs are shown in Figure 1. The data consolidated from the DSC analysis of PCMs at different concentrations of MWCNTs and CuO nanoparticles are presented in Table 2. According to the findings, the phase change temperature was reduced to a smaller extent for all concentrations of two distinct nanoparticles, but the changes are not significant. Similarly, the LHs are also reduced with the inclusion of nanoparticles. Here, it is noted that the excessive inclusion of nanoparticles has an adverse effect on the heat storage capacity. The melting occurs as a single-step endothermic process. The solidification process occurs with two peaks due to the two-stage exothermic phase change process. This phenomenon is generally observed in long-chain fatty alcohols [36]. When PCMs with both nanoparticles were compared, more LH reduction was observed in the case of CuO than in the MWCNTs, but the difference is not significant. The drop in LH with the rise in nanoparticle concentration is due to the reduction in LA quantity per unit mass of NE-PCM, as the LH is directly proportional to the PCM mass. Moreover, the degree of supercooling decreased for the NE-PCM compared to the pure PCM. The nanoparticles improve the heat transfer and promote the crystallization process, which reduces supercooling.
The thermogravimetric analysis results are shown in Figure 2a,b. The findings elucidate that the decomposition temperature of the NE-PCMs has no significant alteration in both cases of MWCNTs and CuO nanoparticles. For NE-PCMs with MWCNT nanoparticles, there was a minor reduction in the decomposition temperature with the increase in MWCNT concentration. For LA, the decomposition occurs at 178 °C, and it was reduced to 162 °C for 5 wt% MWCNT concentration. In the case of CuO nanoparticles, the decomposition temperature somewhat increased to 182 °C. These changes are negligible and will not affect the phase change process.
The TC estimated in both solid and liquid phases of the PCM and NE-PCMs are presented in Figure 3a,b. The TC was observed more in the solid phase than in the liquid phase due to the closely packed PCM and nanoparticles. Furthermore, the NE-PCM with MWCNTs showed higher TC than the NE-PCM with CuO nanoparticles. This is owing to the higher TC of MWCNTs. The nanoparticles enable microconvection between the PCM molecules and improve heat transfer. The maximum improvement in TC for the MWCNT-enhanced PCM was 82.6% and 79.1% in the solid and liquid phases, respectively. Similarly, the TC improved by 49.3% and 33.5% for the CuO-enhanced PCM in the solid and liquid phases, respectively.
The viscosity measurement results at different nanoparticle concentrations are shown in Figure 4. The viscosity upsurges with a rise in the concentration of nanoparticles. In the case of MWCNTs, the PCM impregnates into the tubular structure. The carbon network acts as a support structure for the PCM. Therefore, the viscosity was observed to be higher when compared to metallic CuO nanoparticles. The network structure of MWCNTs resists the flow of the NE-PCM, thereby increasing the viscosity. Furthermore, the surfactant added is responsible for the increase in viscosity. The surfactant is added in proportion to the nanoparticle concentration. With the increase in nanoparticle concentration, the surfactant quantity also increases. The surfactant forms a network-like structure that resists the PCM’s flow and increases viscosity.

4. Conclusions

In this work, two types of NE-PCMs were prepared using MWCNTs and CuO as nanoparticles and lauryl alcohol as the PCM. The findings elucidated that the LH was reduced with the rise in nanoparticle concentration, and more reduction was observed in the case of metallic nanoparticles than the MWCNTs. There is no significant alteration in the decomposition temperature. In the PCM with MWCNTs, the highest latent heat drop during melting and freezing was approximately 10.1% and 9.3%, respectively; in the PCM with CuO, the maximum latent heat drop was around 11% and 10.3%, respectively. The lowest supercooling for the PCM containing MWCNTs and CuO nanoparticles was 8.6 °C and 8.3 °C, respectively. The TC was improved by a maximum of 82.6% and 49.6%, in the case of MWCNT- and CuO-nanoparticle-based PCMs. Greater improvement was observed for carbon-based nanostructure. Furthermore, the viscosity was measured as higher for MWCNTs than CuO, and it tends to upsurge with the rise in nanoparticle concentration. Overall, it can be concluded that MWCNTs provide more favorable results for the thermal property enhancement of PCMs than CuO metallic nanoparticles. Therefore, an MWCNT-based NE-PCM could be a promising TES material for heat storage applications.

Author Contributions

Conceptualization, A.M.A. and V.C.; methodology, A.M.A., G.K.K. and V.C.; formal analysis, A.M.A. and V.C.; investigation, A.M.A. and V.C.; data curation, A.M.A., G.K.K. and V.C.; writing—original draft preparation, A.M.A., G.K.K. and V.C.; writing—review and editing, A.M.A. and V.C.; supervision, V.C. All authors have read and agreed to the published version of the manuscript.

Funding

This research received no external funding.

Data Availability Statement

The data that support the findings of this study are available upon request to corresponding author (V.C. email: [email protected]).

Conflicts of Interest

The authors declare no conflicts of interest.

Abbreviations

CSPConcentrated solar power
CNTCarbon nanotube
CNFCarbon nanofiber
DSCDifferential scanning calorimetry
GNFGraphene nanoplatelet
LHLatent heat
LHTESLatent heat thermal energy storage
LALauryl alcohol
MWCNTMulti-walled carbon nanotube
NE-PCMNano-enhanced phase change material
PCMPhase change material
SDSSodium dodecyl sulfate
TESThermal energy storage
TCThermal conductivity
TGAThermogravimetric analysis
TLSTransient line source

References

  1. Dincer, I.; Rosen, M. Thermal Energy Storage: Systems and Applications, 3rd ed.; Wiley: Hoboken, NJ, USA, 2021; ISBN 9781119713159. [Google Scholar]
  2. Shaghaghi, A.; Eskandarpanah, R.; Gitifar, S.; Zahedi, R.; Pourrahmani, H.; Keshavarzzade, M.; Ahmadi, A. Energy consumption reduction in a building by free cooling using phase change material (PCM). Future. Energy 2024, 3, 31–36. [Google Scholar] [CrossRef]
  3. Geels, J. Electrical power consumption reduction in the bitcoin mining process using phase change material. Future. Energy 2022, 1, 12–15. [Google Scholar] [CrossRef]
  4. Cabeza, L.F. (Ed.) Advances in Thermal Energy Storage Systems: Methods and Applications, 2nd ed.; Woodhead Publishing (Elsevier): Cambridge, UK, 2021; ISBN 978-0-12-819888-9. [Google Scholar]
  5. Tauseef-ur-Rehman; Ali, H.M.; Janjua, M.M.; Sajjad, U.; Yan, W.-M. A critical review on heat transfer augmentation of phase change materials embedded with porous materials/foams. Int. J. Heat Mass Transf. 2019, 135, 649–673. [Google Scholar] [CrossRef]
  6. Ibrahim, N.I.; Al-Sulaiman, F.A.; Rahman, S.; Yilbas, B.S.; Sahin, A.Z. Heat transfer enhancement of phase change materials for thermal energy storage applications: A critical review. Renew. Sustain. Energy Rev. 2017, 74, 26–50. [Google Scholar] [CrossRef]
  7. Joybari, M.M.; Haghighat, F.; Seddegh, S.; Al-Abidi, A.A. Heat transfer enhancement of phase change materials by fins under simultaneous charging and discharging. Energy Convers. Manag. 2017, 152, 136–156. [Google Scholar] [CrossRef]
  8. Chinnasamy, V.; Heo, J.; Jung, S.; Lee, H.; Cho, H. Shape stabilized phase change materials based on different support structures for thermal energy storage applications—A review. Energy 2023, 262, 125463. [Google Scholar] [CrossRef]
  9. Rashid, F.L.; Al-Obaidi, M.A.; Dulaimi, A.; Bernardo, L.F.; Redha, Z.A.; Hoshi, H.A.; Mahood, H.B.; Hashim, A. Recent Advances on The Applications of Phase Change Materials in Cold Thermal Energy Storage: A Critical Review. J. Compos. Sci. 2023, 7, 338. [Google Scholar] [CrossRef]
  10. Rashid, F.L.; Al-Obaidi, M.A.; Dulaimi, A.; Bernardo, L.F.; Eleiwi, M.A.; Mahood, H.B.; Hashim, A. A Review of Recent Improvements, Developments, Effects, and Challenges on Using Phase-Change Materials in Concrete for Thermal Energy Storage and Release. J. Compos. Sci. 2023, 7, 352. [Google Scholar] [CrossRef]
  11. Pereira, J.; Moita, A.; Moreira, A. An Overview of the Nano-Enhanced Phase Change Materials for Energy Harvesting and Conversion. Molecules 2023, 28, 5763. [Google Scholar] [CrossRef] [PubMed]
  12. Anand, A.; Srivastava, V.; Singh, S.; Shukla, A.; Choubey, A.K.; Sharma, A. Development of nano-enhanced phase change materials using manganese dioxide nanoparticles obtained through green synthesis. Energy Storage 2022, 4, e344. [Google Scholar] [CrossRef]
  13. Ouikhalfan, M.; Sari, A.; Chehouani, H.; Benhamou, B.; Biçer, A. Preparation and characterization of nano-enhanced myristic acid using metal oxide nanoparticles for thermal energy storage. Int. J. Energy Res. 2019, 43, 8592–8607. [Google Scholar] [CrossRef]
  14. Han, Z.; Ram, M.K.; Kamal, R.; Alamro, T.; Goswami, D.Y.; Jotshi, C. Characterization of molten salt doped with different size nanoparticles of Al2O3. Int. J. Energy Res. 2019, 43, 3732–3745. [Google Scholar] [CrossRef]
  15. Santosh, R.; Kumaresan, G.; Paranthaman, V.; Swaminathan, M.R.; Velraj, R. Comparative investigation on heat transfer enhancement of surface-roughened and nano-dispersed phase change material for thermal energy storage. Int. J. Energy Res. 2021, 45, 15992–16005. [Google Scholar] [CrossRef]
  16. Arshad, A.; Jabbal, M.; Yan, Y. Preparation and characteristics evaluation of mono and hybrid nano-enhanced phase change materials (NePCMs) for thermal management of microelectronics. Energy Convers. Manag. 2020, 205, 112444. [Google Scholar] [CrossRef]
  17. Arshad, A.; Jabbal, M.; Yan, Y. Thermophysical characteristics and application of metallic-oxide based mono and hybrid nanocomposite phase change materials for thermal management systems. Appl. Therm. Eng. 2020, 181, 115999. [Google Scholar] [CrossRef]
  18. Muzhanje, A.T.; Hassan, M.A.; El-Moneim, A.A.; Hassan, H. Preparation and physical and thermal characterizations of enhanced phase change materials with nanoparticles for energy storage applications. J. Mol. Liq. 2023, 390, 122958. [Google Scholar] [CrossRef]
  19. Karthikeyan, K.; Mariappan, V.; Kalidoss, P.; Mohana Jai Ganesh, J.; Nanda Kishore, P.V.R.; Prathiban, S.; Anish, R. Characterization and thermal properties of lauryl alcohol-capric acid binary mixture with hybrid-nanoparticles as phase change material for vaccine storage applications. J. Energy Storage 2023, 74, 109442. [Google Scholar] [CrossRef]
  20. Rashid, F.L.; Eisapour, M.; Ibrahem, R.K.; Talebizadehsardari, P.; Hosseinzadeh, K.; Abbas, M.H.; Mohammed, H.I.; Yvaz, A.; Chen, Z. Solidification enhancement of phase change materials using fins and nanoparticles in a triplex-tube thermal energy storage unit: Recent advances and development. Int. Commun. Heat Mass Transf. 2023, 147, 106922. [Google Scholar] [CrossRef]
  21. Mahdi, J.M.; Nsofor, E.C. Maximizing the heat-recovery potential of nano-modified phase-change materials through gradual degradation of nanoparticle concentration. J. Energy Storage 2024, 75, 109711. [Google Scholar] [CrossRef]
  22. Venkatraman, S.; Jidhesh, P.; Rathnaraj, J.D.; Selvam, C. Experimental studies on the enhancement in discharging characteristics of phase change material with steatite nanoparticles. J. Energy Storage 2023, 73, 109103. [Google Scholar] [CrossRef]
  23. Baskakov, S.A.; Baskakova, Y.V.; Kabachkov, E.N.; Dvoretskaya, E.V.; Vasilets, V.N.; Li, Z.; Shulga, Y.M. Fast Charging of a Thermal Accumulator Based on Paraffin with the Addition of 0.3 wt. % rGO. J. Compos. Sci. 2023, 7, 193. [Google Scholar] [CrossRef]
  24. Xie, C. Nano-enhanced phase change material using salt hydrate and cooper nanoparticles for battery thermal management system: Buoyancy-driven approach. J. Energy Storage 2023, 74, 108788. [Google Scholar] [CrossRef]
  25. Li, M.; Guo, Q.; Su, Y. The thermal conductivity improvements of phase change materials using modified carbon nanotubes. Diam. Relat. Mater. 2022, 125, 109023. [Google Scholar] [CrossRef]
  26. Qiu, F.; Song, S.; Li, D.; Liu, Y.; Wang, Y.; Dong, L. Experimental investigation on improvement of latent heat and thermal conductivity of shape-stable phase-change materials using modified fly ash. J. Clean. Prod. 2020, 246, 118952. [Google Scholar] [CrossRef]
  27. Mayilvelnathan, V.; Valan Arasu, A. Performance investigation of shell and helical tube heat energy storage system with graphene dispersed erythritol PCM. Energy Storage 2020, 2, e198. [Google Scholar] [CrossRef]
  28. Bahiraei, F.; Fartaj, A.; Nazri, G.-A. Experimental and numerical investigation on the performance of carbon-based nanoenhanced phase change materials for thermal management applications. Energy Convers. Manag. 2017, 153, 115–128. [Google Scholar] [CrossRef]
  29. Panda, D.; Dilip Saraf, S.; Gangawane, K.M. Expanded graphite nanoparticles-based eutectic phase change materials for enhancement of thermal efficiency of pin–fin heat sink arrangement. Therm. Sci. Eng. Prog. 2024, 48, 102417. [Google Scholar] [CrossRef]
  30. Zarma, I.; Emam, M.; Ookawara, S.; Ahmed, M. Thermal management of concentrator photovoltaic systems using nano-enhanced phase change materials-based heat sink. Int. J. Energy Res. 2020, 44, 7713–7733. [Google Scholar] [CrossRef]
  31. Lin, Y.; Cong, R.; Chen, Y.; Fang, G. Thermal properties and characterization of palmitic acid/nano silicon dioxide/graphene nanoplatelet for thermal energy storage. Int. J. Energy Res. 2020, 44, 5621–5633. [Google Scholar] [CrossRef]
  32. Şahan, N.; Fois, M.; Paksoy, H. The effects of various carbon derivative additives on the thermal properties of paraffin as a phase change material. Int. J. Energy Res. 2016, 40, 198–206. [Google Scholar] [CrossRef]
  33. Xu, X.; Zhang, X.; Liu, S. Experimental study on cold storage box with nanocomposite phase change material and vacuum insulation panel. Int. J. Energy Res. 2018, 42, 4429–4438. [Google Scholar] [CrossRef]
  34. Bharathiraja, R.; Ramkumar, T.; Selvakumar, M. Studies on the thermal characteristics of nano-enhanced paraffin wax phase change material (PCM) for thermal storage applications. J. Energy Storage 2023, 73, 109216. [Google Scholar] [CrossRef]
  35. Xu, C.; Fu, T.; Wang, W.; Fang, G. 1-Hexadeol/nano titanium dioxide composite phase change material with different nano-additives: Fabrication and enhanced thermal properties. J. Energy Storage 2023, 72, 108259. [Google Scholar] [CrossRef]
  36. Yin, D.; Ma, L.; Geng, W.; Zhang, B. Microencapsulation of n-hexadecanol by in situ polymerization of melamine–formaldehyde resin in emulsion stabilized by styrene–maleic anhydride copolymer Dezhong. Int. J. Energy Res. 2014, 39, 23–40. [Google Scholar] [CrossRef]
Figure 1. DSC thermograph of LA with nanoparticles (a) with MWCNTs and (b) with CuO.
Figure 1. DSC thermograph of LA with nanoparticles (a) with MWCNTs and (b) with CuO.
Jcs 08 00182 g001
Figure 2. TGA result of LA with nanoparticles (a) with MWCNTs and (b) with CuO.
Figure 2. TGA result of LA with nanoparticles (a) with MWCNTs and (b) with CuO.
Jcs 08 00182 g002
Figure 3. TC result of LA with nanoparticles (a) with MWCNTs and (b) with CuO.
Figure 3. TC result of LA with nanoparticles (a) with MWCNTs and (b) with CuO.
Jcs 08 00182 g003
Figure 4. Viscosity of LA with nanoparticles.
Figure 4. Viscosity of LA with nanoparticles.
Jcs 08 00182 g004
Table 1. Properties of the nanoparticles and surfactant.
Table 1. Properties of the nanoparticles and surfactant.
MaterialProperties
CuO nanoparticlesSize: 80 nm
Surface area: 18 m2g−1
MWCNTsDensity: 0.28 gcm−3
Length: 10–30 µm
Outside diameter: 20–30 nm
Inside diameter: 5–10 nm
Purity: >95 wt%
SDSDensity: 1.01 gcm−3
Table 2. Results from the DSC measurement.
Table 2. Results from the DSC measurement.
SampleMeltingSolidificationDegree of Supercooling
(°C)
Onset (°C)Peak (°C)LH (Jg−1)Onset (°C)Peak (°C)LH (Jg−1)
LA2227217201621311
LA + 1 wt% MWCNTs21.526.121220.517.52108.6
LA + 3 wt% MWCNTs21.626.3202.520.717.42018.9
15.6
LA + 5 wt% MWCNTs21.626.519520.717.51939
15.8
LA + 1 wt% CuO21.925.620020.317.11988.5
14.9
LA + 3 wt% CuO21.825.619720.317.31958.3
14.4
LA + 5 wt% CuO21.925.819320.417.31918.5
13.8
Disclaimer/Publisher’s Note: The statements, opinions and data contained in all publications are solely those of the individual author(s) and contributor(s) and not of MDPI and/or the editor(s). MDPI and/or the editor(s) disclaim responsibility for any injury to people or property resulting from any ideas, methods, instructions or products referred to in the content.

Share and Cite

MDPI and ACS Style

Ambika, A.M.; Kalimuthu, G.K.; Chinnasamy, V. Comparative Investigation of Thermal Properties Improvement of Nano-Enhanced Organic Phase Change Materials. J. Compos. Sci. 2024, 8, 182. https://doi.org/10.3390/jcs8050182

AMA Style

Ambika AM, Kalimuthu GK, Chinnasamy V. Comparative Investigation of Thermal Properties Improvement of Nano-Enhanced Organic Phase Change Materials. Journal of Composites Science. 2024; 8(5):182. https://doi.org/10.3390/jcs8050182

Chicago/Turabian Style

Ambika, Aravindh Madhavankutty, Gopi Kannan Kalimuthu, and Veerakumar Chinnasamy. 2024. "Comparative Investigation of Thermal Properties Improvement of Nano-Enhanced Organic Phase Change Materials" Journal of Composites Science 8, no. 5: 182. https://doi.org/10.3390/jcs8050182

APA Style

Ambika, A. M., Kalimuthu, G. K., & Chinnasamy, V. (2024). Comparative Investigation of Thermal Properties Improvement of Nano-Enhanced Organic Phase Change Materials. Journal of Composites Science, 8(5), 182. https://doi.org/10.3390/jcs8050182

Article Metrics

Back to TopTop