OPINION article

Front. Energy Res., 14 July 2022

Sec. Process and Energy Systems Engineering

Volume 10 - 2022 | https://doi.org/10.3389/fenrg.2022.945360

Opinions on Fabrication of Phase Change Microcapsule Slurry and Its Application in Electronic Cooling

  • 1. Key Laboratory of Energy Thermal Conversion and Control of Ministry of Education, School of Energy and Environment, Southeast University, Nanjing, China

  • 2. Jiangsu Key Laboratory of Micro and Nano Heat Fluid Flow Technology and Energy Application, School of Physical Science and Technology, Suzhou University of Science and Technology, Suzhou, China

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Introduction

With the advent of the Information Age, the requirements for data processing have been on the rise. However, the miniaturization and integration of electronic components lead to increased heat generation. This huge energy consumption in cooling and heat transfer performance of existing coolants limits the development of electronic devices. An important solution is to enhance the heat absorption capacity of coolants. Phase change materials (PCMs) absorb and release a large amount of latent heat through a phase change, which is advantageous in preventing overheating of electronic components (Zhang et al., 2020). However, PCMs leak easily and are mostly corrosive (Moreno et al., 2014). Adding encapsulated phase change materials (EPCMs) into a base working fluid forms a PCM slurry (PCMS), which circumvents the defects of PCM and offers a feasible approach to thermal management. The invariant temperature during the phase change makes PCMS more competitive than conventional coolants in many cooling technologies, such as microchannel (Wang et al., 2016), jet and spray cooling (Wan et al., 2021), heat pipes (Heydarian et al., 2019), etc. In particular, when the heat flux is high, up to a 40% decrement in the internal wall temperature, a 50% increase in heat transfer coefficient (Sabbah et al., 2012), and a 67.5% decrement in the pumping power (Chen et al., 2008) can be achieved by the application of EPCM. However, encapsulation brings about additional heat resistance, which may weaken the heat transfer performance of PCMS or even deteriorate the cooling process. Furthermore, the high viscosity of PCMS leads to high pumping power, especially in conditions with a high concentration of EPCM, a low Re number, or narrow channels (Ghoghaei et al., 2020). Supercooling is another drawback of PCMS in that phase change is triggered at a higher temperature than pure PCM, resulting in uncertainty of heat transfer and increasing energy consumption. To improve the performance of PCMS, various attempts have been made and can be classified into two categories as improving the fabrication of PCM microcapsules (Hao et al., 2022) and coupling PCMS with other materials (Rajabifar, 2015).

Thus, given the urgent need for electronic cooling and the favorable heat transfer performance of PCMS, this opinion briefly expounds on the prospect and challenges of PCMS in thermal management. The fabrication of EPCM and the application of common cooling technology with typical optimization methods are summarized here, aiming to provide a quick and preliminary understanding of PCMS.

Fabrication of Encapsulated Phase Change Materials

Traditionally, EPCMs are produced through polymerization, coacervation, etc. Microfluidics with high capsulation efficiency provide an alternative approach to producing highly monodispersed EPCM in a controllable way. EPCMs produced by polymerization, complex coacervation, and microfluidics are shown in Figure 1.

FIGURE 1

FIGURE 1

Encapsulation methods: (A) polymerization, (a1) and (a2) are EPCM produced by in situ polymerization (Srinivasaraonaik et al., 2020) and interfacial polymerization (Zhao and Luo, 2022), respectively, (B) coacervation (Malekipirbazari et al., 2014), (C) microfluidic EPCM production (I: glass slide, II: dispensing needles, III: inner capillary, IV: outer capillary) (Hao et al., 2022).

Polymerization

Polymerization generally refers to in situ polymerization and interfacial polymerization, as shown in Figure 1 A. In the in situ polymerization, monomers of the shell material and catalyst are dissolved in the preemulsified core solution. When the environmental conditions, such as pH value or temperature, vary, a high molecular polymer of the shell, which is insoluble in the continuous phase, forms at the surface of the core emulsions that encapsulates the core materials into capsules (Srinivasaraonaik et al., 2020). The interfacial polymerization is similar to in situ polymerization where the polymerization occurs at the interface of core material emulsion. The formation of a shell is caused by the polymerization of reactants inside and outside the interface (Zhao and Luo, 2022). Polymerization methods have the advantages of rapid reaction, mild conditions, and simple operation. But, impurities in the products are inevitable.

Complex Coacervation

Complex coacervation, as shown in Figure 1B, uses two or more types of polymers with opposite charges as the composite of shell. Under certain temperature and salinity, the electrostatic attraction between polymers leads to polymerization at the surface of dispersed core material. Phase separation occurs spontaneously with decreasing solubility, and microcapsules form eventually (Malekipirbazari et al., 2014). The coacervation is easy to operate with the advantage of high throughput. However, the selection of the shell materials is tricky, and impurities are inevitable.

Microfluidic

Studies have proven the significance of accurate and controllable encapsulation of EPCM for the cooling performance of PCMS (Li et al., 2019). Based on microfluidic chips, micro/nanoscale single and double emulsions with perfect sphericity can be prepared, and the capsule size can be controlled easily by changing the flow rate of phases, which has drawn extensive attention. Axisymmetric microfluidic chips, such as flow focusing (Akamatsu et al., 2019) and coflowing (Fu et al., 2014) are usually used for preparing EPCM. The liquid-state core and shell materials are injected as the innermost and the middle phase, respectively, during the formation of double emulsions in microfluidics. Subsequently, EPCM with smooth surface and regular size are obtained by curing the emulsion templates. The EPCM produced by Hao et al. (2022) with coflowing microfluidic device is shown in Figure 1C1, which suggests that EPCM prepared by microfluidic have significantly higher monodispersity than those prepared by other methods.

A 100% encapsulation efficiency and controllability make microfluidic a promising fabrication method for EPCM. However, there are several issues limiting the industrial application of microfluidic: 1) The controllability of microfluidic relies on fully understanding the hydrodynamic mechanism of droplet formation (Chen et al., 2013; Chen and Deng, 2017; Wang et al., 2022). 2) The fluid to be emulsified is determined by the wettability of the chip; hence, surface modification is usually required (Wang et al., 2018). 3) The throughput of microfluidic is relatively low in a single microfluidic channel. Recently, step emulsification (Shi et al., 2020), parallel microchannel (Eberhardt et al., 2019), and droplet splitting (Park et al., 2018) are proposed to facilitate the throughput of microfluidics. However, complex hydrodynamics are inevitable in high-throughput microfluidics that the monodispersity is slightly worse than a single-channel microfluidic.

Applications in Electronic Cooling

EPCM shows great potential in effective cooling with reduced energy consumption attributable to its high specific surface area and favorable characteristic of constant temperature during the phase transition process. However, there are some unsolved problems that limit the prevalence of EPCM in cooling technologies.

Microchannel

Microchannel is one of the most commonly used liquid cooling devices. Compared with traditional coolant, PCMS has been proven to have enhanced cooling performance. Adding 0.7% EPCM can achieve a 37% increment in heat transfer efficiency compared to single-phase coolant (deionized water). However, when the concentration of EPCM increases from 0.25% to 1.5%, the viscosity increases by 15%–22%, which directly leads to high pressure drop and pumping power (Joseph and Sajith, 2019). To optimize the performance of PCMS, some methods aiming to enhance the heat transfer are proposed, such as adding nanoparticles in the slurry (Rajabifar, 2015), using carbon nanotubes as the shell to increase the thermal conductivity, and adding liquidity-enhancing active agent (Sinha-Ray et al., 2014). The applicable temperature of PCMS can be extended from 40°C–80°C to 40°C–120°C with carbon nanotube shells and active agent, which is of great significance for cooling in high-heat flux narrow channels.

Jet Impingement Cooling

The heat transfer coefficient of jet impingement cooling increases by 50%–70% after the working fluid is loaded with EPCM, and the capsules can maintain complete structure after multiple cycles (Wu et al., 2011). However, a high pressure drop and heat transfer resistance of EPCM were also observed (Wan et al., 2021). What is more, the PCMS exhibit greater cooling efficiency than single-phase coolants only when the jet inlet temperature is in a certain range related to the PCM melting point. Although the disadvantage of PCMS can be counteracted by increasing the flow rate, excessive flow velocity causes incomplete phase transition and invalidity of PCMS.

Heat Pipe

The PCMS is also utilized in pulsating heat pipes. The PCM melts and solidifies when it passes through the heating and cooling section, respectively. The experiments of Heydarian et al. show that the PCMS can enhance heat transfer by 6%–44%, thus contributing to its large latent heat and disturbance to the fluid flow (Heydarian et al., 2019). Moreover, PCMS can effectively prevent the dry-out compared to single-phase coolants, which stabilizes the operation of heat pipes under the high heat flux. However, the EPCM leads to higher thermal resistance and viscosity, so there is an optimal concentration at which the thermal resistance of the slurry is the highest. Once the concentration exceeds this optimal concentration, boiling deterioration is observed.

Flow in Pipe

As an important component of numerous heat exchangers, enhancing the heat transfer of flow in the pipe/tube by PCMS is of great potential. By comparing the heat transfer of PCMS and water in tubes under different working conditions, Zhang et al. found that the disadvantage of PCMS’s high viscosity plays a dominant role in the laminar flow condition. Thus, the heat transfer coefficient of PCMS in the pipe is even lower than that of single-phase coolant at the low Re number. In the turbulent flow, although the heat transfer can be improved by PCMS, the enhancement shows a strong correlation with the flow rate, which is dominated by the heat load. Although the high viscosity increases the pumping power required for pipe flow, the required flow rate is reduced, the pump energy can be reduced by more than 60% (Chen et al., 2008). However, with the continuous increase of Re, insufficient time for phase transition of PCM is observed, and the heat absorption capacity of PCMS is weakened (Zhang et al., 2018; Zhang et al., 2021).

Summary

The PCMS shows great potential in effective cooling having a huge advantage of maintaining a stable temperature. Some advantages and common challenges of PCMS for liquid cooling can be summed up according to the present literature. The PCMS can thus enhance the heat transfer greatly by storing the absorbed energy as latent heat, especially under high heat flux conditions. But, the performance is limited by the working condition. On the one hand, the competition among high specific surface area, high thermal resistance, and high viscosity attributing to encapsulation lead to an optimum concentration of EPCM in the base fluid. Although the optimal value is mainly determined by experiments, further theoretical studies are needed. Moreover, the application of PCMS in narrow channels and laminar flow is hindered by high thermal resistance and high viscosity, and the heat transfer deteriorates in some conditions. Although the thermal conductivity and fluidity of PCMS can be improved by nanoparticles and active agents, this approach is limited because nanoparticles also increase the viscosity of the slurry (Zhang et al., 2018). On the other hand, the heat absorption of EPCM depends on the phase change process that occurs only under certain temperature conditions. Thus, the choice of PCMS depends on specific working conditions, and the prediction of the heat transfer coefficient is a challenge.

Conclusion

Current studies have proven that PCMS can achieve higher efficiency than single-phase coolants in heat dissipation, especially under high heat flux conditions, which is of great significance in solving the problem of heat dissipation of electronic devices while reducing the energy consumption. However, PCMS is valid only under a certain range of flow velocity, temperature, and concentration due to additional thermal resistance, high viscosity, and supercooling. Several approaches have been proposed to enhance the performance of PCMS. From the aspect of fabrication, microfluidics with a 100% encapsulation efficiency represents a promising route for producing high quality EPCM in a controllable way. From the aspect of an application, nanoparticles and an active agent can improve the thermal conductivity and fluidity of PCMS, respectively. There are three possible directions for the future development of PCMS. First, a high-throughput and controllable microfluidic method for the fabrication of EPCM can improve the quality and stability of PCMS. Second, an efficient and compatible base fluid with high thermal conductivity and liquidity is beneficial in the extensive application of PCMS. Finally, the prediction of an optimal working condition based on experimental tests and theoretical analysis is essential for the design of cooling devices utilizing PCMS.

Statements

Author contributions

FY contributed to the conception of the study. HC wrote the first draft of the manuscript. All authors contributed to the manuscript revision, and have read and approved the submitted version.

Funding

This work is supported by the National Natural Science Foundation of China (No. 51906170).

Conflict of interest

The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.

Publisher’s note

All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors, and the reviewers. Any product that may be evaluated in this article, or claim that may be made by its manufacturer, is not guaranteed or endorsed by the publisher.

References

  • 1

    AkamatsuK.OgawaM.KatayamaR.YonemuraK.NakaoS.-i. (2019). A Facile Microencapsulation of Phase Change Materials within Silicone-Based Shells by Using Glass Capillary Devices. Colloids Surfaces A Physicochem. Eng. Aspects567, 297303. 10.1016/j.colsurfa.2019.01.076

  • 2

    ChenB.WangX.ZengR.ZhangY.WangX.NiuJ.et al (2008). An Experimental Study of Convective Heat Transfer with Microencapsulated Phase Change Material Suspension: Laminar Flow in a Circular Tube under Constant Heat Flux. Exp. Therm. Fluid Sci.32 (8), 16381646. 10.1016/j.expthermflusci.2008.05.008

  • 3

    ChenY.DengZ. (2017). Hydrodynamics of a Droplet Passing Through a Microfluidic T-Junction. J. Fluid Mech.819, 401434. 10.1017/jfm.2017.181

  • 4

    ChenY.LiuX.ShiM. (2013). Hydrodynamics of Double Emulsion Droplet in Shear Flow. Appl. Phys. Lett.102 (5), 051609. 10.1063/1.4789865

  • 5

    EberhardtA.BoškovićD.LoebbeckeS.PanićS.WinterY. (2019). Customized Design of Scalable Microfluidic Droplet Generators Using Step‐Emulsification Methods. Chem. Eng. Technol.42 (10), 21952201. 10.1002/ceat.201900143

  • 6

    FuZ.SuL.LiJ.YangR.ZhangZ.LiuM.et al (2014). Elastic Silicone Encapsulation of N-Hexadecyl Bromide by Microfluidic Approach as Novel Microencapsulated Phase Change Materials. Thermochim. Acta590, 2429. 10.1016/j.tca.2014.06.008

  • 7

    GhoghaeiM. S.MahmoudianA.MohammadiO.ShafiiM. B.Jafari MoslehH.ZandiehM.et al (2020). A Review on the Applications of Micro-/Nano-encapsulated Phase Change Material Slurry in Heat Transfer and Thermal Storage Systems. J. Therm. Anal. Calorim.145 (2), 245268. 10.1007/s10973-020-09697-6

  • 8

    HaoG.YuC.ChenY.LiuX.ChenY. (2022). Controlled Microfluidic Encapsulation of Phase Change Material for Thermo-Regulation. Int. J. Heat Mass Transf.190, 122738. 10.1016/j.ijheatmasstransfer.2022.122738

  • 9

    HeydarianR.ShafiiM. B.Rezaee Shirin-AbadiA.GhasempourR.Alhuyi NazariM. (2019). Experimental Investigation of Paraffin Nano-Encapsulated Phase Change Material on Heat Transfer Enhancement of Pulsating Heat Pipe. J. Therm. Anal. Calorim.137 (5), 16031613. 10.1007/s10973-019-08062-6

  • 10

    JosephM.SajithV. (2019). An Investigation on Heat Transfer Performance of Polystyrene Encapsulated N-Octadecane Based Nanofluid in Square Channel. Appl. Therm. Eng.147, 756769. 10.1016/j.applthermaleng.2018.10.120

  • 11

    LiS.ZhangH.ChengJ.LiX.CaiW.LiZ.et al (2019). A State-Of-The-Art Overview on the Developing Trend of Heat Transfer Enhancement by Single-phase Flow at Micro Scale. Int. J. Heat Mass Transf.143, 118476. 10.1016/j.ijheatmasstransfer.2019.118476

  • 12

    MalekipirbazariM.SadrameliS. M.DorkooshF.SharifiH. (2014). Synthetic and Physical Characterization of Phase Change Materials Microencapsulated by Complex Coacervation for Thermal Energy Storage Applications. Int. J. Energy Res.38 (11), 14921500. 10.1002/er.3153

  • 13

    MorenoP.MiróL.SoléA.BarrenecheC.SoléC.MartorellI. (2014). Corrosion of Metal and Metal Alloy Containers in Contact with Phase Change Materials (PCM) for Potential Heating and Cooling Applications. Appl. Energy125, 238-245. 10.1016/j.apenergy.2014.03.022

  • 14

    ParkJ.JungJ. H.ParkK.DestgeerG.AhmedH.AhmadR.et al (2018). On-Demand Acoustic Droplet Splitting and Steering in a Disposable Microfluidic Chip. Lab. Chip18 (3), 422432. 10.1039/c7lc01083d

  • 15

    RajabifarB. (2015). Enhancement of the Performance of a Double Layered Microchannel Heatsink Using PCM Slurry and Nanofluid Coolants. Int. J. Heat Mass Transf.88, 627635. 10.1016/j.ijheatmasstransfer.2015.05.007

  • 16

    SabbahR.Seyed-YagoobiJ.Al-HallajS. (2012). Heat Transfer Characteristics of Liquid Flow with Micro-encapsulated Phase Change Material: Experimental Study. J. Heat Transf.134 (4), 044501. 10.1115/1.4005311

  • 17

    ShiZ.LaiX.SunC.ZhangX.ZhangL.PuZ.et al (2020). Step Emulsification in Microfluidic Droplet Generation: Mechanisms and Structures. Chem. Commun.56 (64), 90569066. 10.1039/d0cc03628e

  • 18

    Sinha-RayS.Sinha-RayS.SriramH.YarinA. L. (2014). Flow of Suspensions of Carbon Nanotubes Carrying Phase Change Materials through Microchannels and Heat Transfer Enhancement. Lab. Chip14 (3), 494508. 10.1039/c3lc50949d

  • 19

    SrinivasaraonaikB.SinghL. P.TyagiI.RawatA.SinhaS. (2020). Microencapsulation of a Eutectic PCM Using In Situ Polymerization Technique for Thermal Energy Storage. Int. J. Energy Res.44 (5), 38543864. 10.1002/er.5182

  • 20

    WanH.HeG. Q.XueZ. R.LiW. Q. (2021). Numerical Study and Experimental Verification on Spray Cooling with Nanoencapsulated Phase-Change Material Slurry (NPCMS). Int. Commun. Heat Mass Transf.123, 105187. 10.1016/j.icheatmasstransfer.2021.105187

  • 21

    WangJ.-X.YuW.WuZ.LiuX.ChenY. (2022). Physics-Based Statistical Learning Perspectives on Droplet Formation Characteristics in Microfluidic Cross-Junctions. Appl. Phys. Lett.120 (20), 204101. 10.1063/5.0086933

  • 22

    WangJ.GaoW.ZhangH.ZouM.ChenY.ZhaoY. (2018). Programmable Wettability on Photocontrolled Graphene Film. Sci. Adv.4 (9), eaat7392. 10.1126/sciadv.aat7392

  • 23

    WangY.ChenZ.LingX. (2016). An Experimental Study of the Latent Functionally Thermal Fluid with Micro-encapsulated Phase Change Material Particles Flowing in Microchannels. Appl. Therm. Eng.105, 209216. 10.1016/j.applthermaleng.2016.05.159

  • 24

    WuW.BostanciH.ChowL. C.DingS. J.HongY.SuM.et al (2011). Jet Impingement and Spray Cooling Using Slurry of Nanoencapsulated Phase Change Materials. Int. J. Heat Mass Transf.54 (13-14), 27152723. 10.1016/j.ijheatmasstransfer.2011.03.022

  • 25

    ZhangC.LiJ.ChenY. (2020). Improving the Energy Discharging Performance of a Latent Heat Storage (LHS) Unit Using Fractal-Tree-Shaped Fins. Appl. Energy259, 114102. 10.1016/j.apenergy.2019.114102

  • 26

    ZhangG.CuiG.DouB.WangZ.GoulaM. A. (2018). An Experimental Investigation of Forced Convection Heat Transfer with Novel Microencapsulated Phase Change Material Slurries in a Circular Tube under Constant Heat Flux. Energy Convers. Manag.171, 699709. 10.1016/j.enconman.2018.06.029

  • 27

    ZhangJ. J.YangC. H.JinZ. G.MaS. X.ZhangJ. S.PangX. M. (2021). Experimental Study of Jet Impingement Heat Transfer with Microencapsulated Phase Change Material Slurry. Appl. Therm. Eng.188, 116588. 10.1016/j.applthermaleng.2021.116588

  • 28

    ZhaoY.LuoY. (2022). Encapsulation of Phase Change Materials via Interfacial Miniemulsion Polymerization for High Thermal Energy Storage Density. Macro React. Eng.2022, 2100049. 10.1002/mren.202100049

Summary

Keywords

PCM, encapsulation, phase change microcapsule slurry, microfluidic, electronic cooling

Citation

Cao H and Yao F (2022) Opinions on Fabrication of Phase Change Microcapsule Slurry and Its Application in Electronic Cooling. Front. Energy Res. 10:945360. doi: 10.3389/fenrg.2022.945360

Received

16 May 2022

Accepted

03 June 2022

Published

14 July 2022

Volume

10 - 2022

Edited by

Xiao Chen, Beijing Normal University, China

Reviewed by

Takaichi Watanabe, Okayama University, Japan

Updates

Copyright

*Correspondence: Feng Yao,

This article was submitted to Process and Energy Systems Engineering, a section of the journal Frontiers in Energy Research

Disclaimer

All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors and the reviewers. Any product that may be evaluated in this article or claim that may be made by its manufacturer is not guaranteed or endorsed by the publisher.

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