Article


 

  AL-QADISIYAH JOURNALFORENGINEERING SCIENCES 14 (2021) 042–047 
 

   

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Al-Qadisiyah Journal for Engineering Sciences 

 
Journal homepage: http://qu.edu.iq/journaleng/index.php/JQES  

  

 

* Corresponding author. 

E-mail address: hasan.dawwood@qu.edu.iq (Hasan I. Dawood) 

 

https://doi.org/10.30772/qjes.v14i1.732  

2411-7773/© 2021 University of Al-Qadisiyah. All rights reserved.                                This work is licensed under a Creative Commons Attribution 4.0 International License. 

 

 

A Comparative Study On Stability And Thermal Properties Of Various 

Nanofluids 

Marwa S.J. , Hasan I. Dawood٭ 

Chemical Engineering Department -Faculty of Engineering – University of Al-Qadisiyah-Iraq. 

A R T I C L E  I N F O 

Article history: 

Received 13 January 2021 

Received in revised form 11 April 2021 

Accepted 15 April 2021 

 

Keywords: 

 Heat transfer Enhancement; 

Nanofluids;  

Thermal properties; 

Hybrid nanofluids; 

 Base fluids. 

 

 

A B S T R A C T            

The attention of researches in convective heat transfer by suspended nanoparticles in base fluids has grown 

lately to promote uncommon techniques for enhancing the thermal performance of fluids. In this study, the 

stability period and thermal properties of aluminium oxide (Al2O3), silicon dioxide (SiO2) and Al2O3–SiO2 

hybrid were investigated at volume concentration 0.1vol.% dispersed in Distilled Water (DW) as a base 

fluid. For the hybrid nanofluid, the samples were consisted of  (0.025 

vol.%Al2O3+0.075vol.%SiO2),(0.05vol.%Al2O3+0.05vol.%SiO2)and(0.075vol.%Al2O3+0.025vol.%SiO2). 

The two-step method was adopted to prepare the nanofluid samples by using Ultrasonic device. Three 

different ultrasonication times were fitted for preparing the samples (1hr,2 hr and 3 hr).The properties of 

single and hybrid nanofluids were evaluated at various temperatures (from 30 °C to 70 °C). The obtained 

results demonstrated that the dispersion of nanoparticles was homogeneous and more stable for a longer 

period for all samples that prepared at 3 hr of ultrasonication process. Among all samples of nanofluids, 

SiO2/DW was found to be the most stable coolant. For all nanofluids, with an increase of temperature, the 

thermal conductivity and specific heat were increased significantly while density and viscosity were 

decreased. 

©2021 University of Al-Qadisiyah. All rights reserved. 

1. Introduction

Improving warmth move rates by using nanofluids has drawn huge 

considerations from analysts around the globe. Ordinary strong 

nanoparticles, size of 1-100 nm with high warm conductivities, are 

suspended in the base liquids that have low warm conductivities. The 

nanofluids have demonstrated an upgrade in viable warm conductivities 

and the convective warmth move coefficients of the first base fluid[1]. 

Nano-fluid, a collection of nanomaterials in a continuous and saturated 

liquid, has been known to be capable of achieving significantly higher 

thermal conductivity than the associated base liquid, causing an 

enhancement  in heat transfer coefficients [2].Hybrid2nanofluid as an 

expansion of nanofluid is obtained by scattering composite nano-powder or 

two diverse nanoparticles in the base liquid. It is accepted that half breed 

nanofluid will offer great warm qualities when contrasted with the base 

liquid and nanofluid containing single nanoparticles because of synergistic 

impacts[3]. A blend of nanofluids happens only utilizing remarkable 

techniques like as one stage and two-advance strategies. Steady and quality 

nanofluids are integrated utilizing these strategies to use them for any 

warmth move and exploratory purposes. According to various authors, 

physical properties of nanofluids is influenced by several factors. 

Temperature is the most important factor which plays a significant role in 

the nanofluid thermal performance. 

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MARWA S.J. , HASAN. I. DAWOOD /AL-QADISIYAH JOURNALFOR ENGINEERING SCIENCES 14(2021) 042–047                                43 

 

           [4] claimed that nano-fluids could be better than traditional working 

fluids like Ethylene Glycol (EG) and water due to the more beneficial and 

encouraging heat transfer properties of nano-fluids. [5]used  

Al2O3 nanoparticles with 4.3 vol.% and noted that an increase in the warm 

conductivity of water under fixed conditions by 32.4%. [6] thought about 

the warm conductivity between Cu-EG nanofluid and unadulterated EG. 

The outcome showed that 40% expansion in warm conductivity of Cu-EG 

nanofluid at volume portion of 0.3 vol%. As indicated by [7], a superior 

improvement in warm conductivity can be produced by hybridizing silver 

nano-particles with Multi-Walled Carbon Nanotube (MWCNT). 

Approximately half nanoparticles have demonstrated an astounding 

improvement regarding cooling adequacy contrasted with single 

nanoparticles and water. [8] arranged suspension of TiO2 and Al2O3 

nanoparticles by a two-advance technique by scattering 0.05 vol.% and 0.3 

vol.% in the blend of water and EG which was mixed for 30 min utilizing 

an attractive stirrer followed by ultrasonication utilizing an ultrasonication 

for 2 hr. They proposed that TiO2 more steady than Al2O3 in water/EG 

blend. [9]  Compared to nano-fluid that have single nanoparticles and water, 

hybrid nanoparticles have exhibited a significant  improvement in cooling 

system performance [10]. Stabilized Single Walled Carbon Nanotubes 

(SWCNT) functionalized with the carboxyl group (COOH) –water /EG by. 
The functionalized SWCNT with different solid volume fractions were 

added to the base fluid, using a two-step method. The finds obvioused that 

the nano-fluid samples was stable for two weeks and its had a long stability 

with no comprehensible precipitation. [11]inspected thermo-physical 

properties (warm conductivity, thickness, consistency and explicit warmth) 

of nanofluids containing Al2O3 nanoparticles in water/EG blend (50:50). 

The ascent in temperature demonstrated improvement in warm 

conductivity and specific heat while the density and viscosity were 

decreased.[12] estimated warm conductivity of ZnO-Ag (50 %:50 %)/water 

by considering different temperatures (25°C– 50°C) at 2 vol.%. The 

maximum thermal conductivity was achieved at 50°C. [13]analyzed the 

thermal behavior of a functionalized graphene nanoplateletplatinum (GNP-

Pt) hybrid nano-fluid at temperatures ranging from 20°C to 40 °C. They 

mentioned that the hybrid nano-fluid density was correlated with the 

temperature .  GNP-Pt/water hybrid nano-fluid density decreased with the 

rise in temperature from the observational investigation. From the findings 

of Yarmand et al[14]on the activated carbon/grapheme (ACG)/EGG hybrid 

nano-fluid. It was established that when the temperature increases 

significantly, the specific heat  of nano-fluids was greater than that of the 

base fluids. For thermal performance testing, nano-fluid viscosity is a 

parameter as important as thermal conductivity, density and specific heat. 

Dardan et al[15]demonstrated the viscosity relationship with respect to the 

difference of Al2O3-MWCNT/nano-fluid oil temperatures. And as per the 

results, with temperature, viscosity was dramatically decreased, with 

temperature increase. 

The main objective of this paper is to get a nanofluid with promising 

advantages by adding Al2O3 and SiO2nanoparticles to DW. Adopting the 

two-step method to prepare nanofluid samples and highlighting on the 

effect of ultrasonication time on the stability of nano-suspensions. The 

thermophysical properties of nanofluids were evaluated at temperatures 

from 30 °C to 70 °C. 

 

2. Experimental steps : 

2.1. Nanofluids preparation:          

  Two kinds of oxide nanoparticles were utilized for this investigation: 

Al2O3 nanoparticles produced by ( Hongwu, Universal Group.Ltd) and 

SiO2 manufactured by US Exploration Nanomaterial's, Inc. 

(NovaScientific Assets (M) Sdn. Bhd). Both nanofluids were readied with 

DWas base fluid. The properties of these nanoparticles are shown in Table 

1. 

Table 1:Physical, morphological and thermo- properties of Al2O3 and 

SiO2 nanoparticles. 

Properties11  (Al2O3)  (SiO2) 

Color11 White White 

Particle size  50 nm  50 nm  

Purity  99.99% 99.8% 

Morphology1of2Particles  Spherical Spherical 

Form11 Powder Powder 

Density (g.cm-3)  3.9 2.4 

Thermal conductivity (K) 

(W.m−1 .K−1) 

40 [16] 1.4 [17] 

Specific heat (cp) (J / kg.k) 773 [16] 745 [17] 

 

The particles shape and microstructure that studied with scanning electron 

microscope (SEM) are explain in Fig. 1a-b. The examination was 

conducted in the Scientific Research Department / Ministry of Higher 

Education and Scientific Research. 

 The nanoparticle suspensions in DW were subjected to ultrasonic 

vibration for 1hr,2hr and 3hr at room temperature as in Fig. 2. The weight 

of Al2O3and SiO2 nanoparticles that used to prepare the nanofluid samples 

are explained in Table 2. 

Table 2:The weights in gm of Al2O3and SiO2 nanoparticles in the 

samples. 
No. sample Weight  

1 0.1 vol.% Al2O3 39.04 

2 0.1 vol.% SiO2 24.04 

3 0.05 vol.% Al2O3 + 0.05 vol.% SiO2 31.49 

4 0.075 vol.% Al2O3 + 0.025 vol.% SiO2 35.24 

5 0.025 vol.% Al2O3 + 0.075 vol.% SiO2 27.79 

  The next step, adequate quantities of DW were added to the underlying 

suspensions and altogether blended to accomplish the expected nanofluids. 

The volume concentrations of single and hybrid nanofluids are evaluated 

from the following equations[18]: 

Volume concentration (𝜑) = [

𝑊𝑛𝑝

𝜌𝑛𝑝 
𝑊𝑛𝑝

𝜌𝑛𝑝  
   +  

𝑊𝑏𝑓

𝜌𝑏𝑓

] × 100                                     (1) 

Nomenclature 
  

DW Distillate water 𝑛𝑝 nanoparticles 

k thermal conductivity (W m-1 K-1) 𝑤 the weight(  Kg ) 

𝐶 specific heat (J kg-1 K-1) 𝜇  viscosity in mpa.s 

𝑏𝑓 base2fluid3 𝜌    the density of the nanoparticles  ( Kg . m
-3) 

𝑛𝑓 nanofluid 𝜑 Volume concentration 



44 MARWA S.J. , HASAN. I. DAWOOD /AL-QADISIYAH JOURNALFOR ENGINEERING SCIENCES 14 (2021) 042–047 

 

𝜑 = [
[

𝑊𝑛𝑝

𝜌𝑛𝑝
]

𝐴𝑙2𝑂3
   + [

𝑊𝑛𝑝

𝜌𝑛𝑝
]

𝑆𝑖𝑂2

[
𝑊𝑛𝑝

𝜌𝑛𝑝
]

𝐴𝑙2𝑂3
   + [

𝑊𝑛𝑝

𝜌𝑛𝑝
]

𝑆𝑖𝑂2
   +  

𝑊𝑏𝑓

𝜌𝑏𝑓

] × 100                                                 (2) 

2.2.Evaluation of the physical properties for nanofluids           

The thermal conductivity of nanofluids is a significant property when 

evaluating warm proficiency. Estimations were performed with 

temperature assorted variety between 30 °C and 70 °C. To evaluate the 

warm conductivity of nanofluids, KD2 Ace Warm Properties Analyzer 

(Decagon Gadgets, USA) was used as in Fig. 3a-b. The examination was 

conducted at the University of Babylon / College of Engineering / 

Department of Chemical Engineering .The KD2 was adjusted by utilizing 

DW at the room temperature before estimations, and the exactness of these 

estimations was fated to be inside 1%. The measurements of Physico-

thermal properties for nanofluids (density, specific heat and 

 

Figure 1:a. General shape of Al2O3 and SiO2particles  b. SEM of 

nanoparticles 

 

 

 

Figure 2: Ultrasonic device 

 viscosity) are necessary to apply for practical applications. Appropriate 

correlations to assess the density of single nanofluids were provided by 

Pakand Chu [19]that have been identified as follows: 

𝜌𝑛𝑓 =  𝜑𝜌𝑛𝑝 +  (1 − 𝜑)𝜌𝑏𝑓                                                                     (3) 

Specific heat of single nanofluids was calculated using Xuan and Roetzel’s 

[20] equation: 

 

(𝜌𝐶)𝑛𝑓 =  𝜑(𝜌𝐶)𝑛𝑝 +  (1 − 𝜑)(𝜌𝐶)𝑏𝑓                                                   (4) 

 

Figure 3:a. Thermo- Properties Analyzer  b. schematic diagram of 

thermal conductivity measuring. 

To measure the densities and specific heat of hybrid suspensions of 

Al2O3and SiO2nanoparticles, the theoretical formulasthat predicted by Ho 

et al.[21]were used as follows: 

𝜌𝑛𝑓 = [𝜑𝜌𝑛𝑝 ]𝐴𝑙2𝑂3 +  [𝜑𝜌𝑛𝑝 ]𝑆𝑖𝑂2 + (1 − 𝜑𝐴𝑙2𝑂3 −  𝜑𝑆𝑖𝑂2)𝜌𝑏𝑓               (5)                                                                                              

(𝜌𝐶)𝑛𝑓 = [ 𝜑𝜌𝐶]𝐴𝑙2𝑂3 +  [ 𝜑𝜌𝐶]𝑆𝑖𝑂2 + (1 − 𝜑𝐴𝑙2𝑂3 −  𝜑𝑆𝑖𝑂2)(𝜌𝐶)𝑏𝑓   (6) 

To predict the viscosity of nanofluids, the formula derived by Brinkman  

[22]was used.All samples that used in this study which have different 

component fractions of Al2O3 and SiO2were considered to have the same 

viscosity because of particle’s spherical shape and the volume fraction of 

samples between 0.01 vol.% and 2 vol.% [23]. 

𝜇𝑛𝑓 =
𝜇𝑏𝑓

(1−𝜑)2.5
                                                                                           (7) 

3. Results and discussion 

       Tests were performed with DW and various samples of nano-fluids 
which were prepared with different ultrasonication times (1hr,2 hr and 3 



MARWA S.J. , HASAN. I. DAWOOD /AL-QADISIYAH JOURNALFOR ENGINEERING SCIENCES 14(2021) 042–047                                45 

 

hr). The study was carried out with the range of temperature (30,40,50,60 

and 70°C) at 0.1vol.%. The observation obtained from the present 

investigation is discussed below: 

3.1.  Dependability time of nanofluids 

 The impact of ultrasonication times on resting period as appeared in 

Table 3. Due to the little size of nanoparticles, it has a high propensity to 

shape groups or agglomerates because of van der Waals powers. 

Ultrasonication technique helps to break these bonds between the 

nanoparticles and increase the random motion of the nanoparticles that 

suspended in the base fluid.The augmentation in ultrasonication time lead 

to an increment in the random motion of this nano-powder and will create 

a slip speed between the particles and the liquid medium[24]. The 

experimental results show a  good agreement with the previous articles [25, 

26]. Besides, the challenge of how to effectively prevent nanoparticles from 

agglomeration or aggregation, the key issue is the weight of nanoparticles 

that are used to form more stable nanofluids.The  best consequences were 

gotten  for the sample 0.1 vol.% SiO2, where it recorded the longest period 

of stability which was about 15 day with ultrasonication time 3 hr.The 

reason is due to the total weight of nanoparticles that used in 0.1 vol.% SiO2 

is less than weights that utilized in other samples to prepare them with the 

same volume concentration, which ensures the possibility of better 

distribution and a longer sedimentation time[25].Fig. 4 explain the 

sedimentation time for the sample 0.1vol.%of SiO2 after 15day. 

Table 3: Stability period (day) of nanofluid samples at room 

temperature 

 

Samples Ultrasonication time 

1hr 2 hr 3 hr 

0.1 vol.% Al2O3 7 9 11 

0.1 vol.% SiO2 9 11 15 

0.05 vol.% Al2O3 + 0.05 vol.% SiO2 8 10 13 

0.075 vol.% Al2O3 + 0.025 vol.% SiO2 7 9 12 

0.025 vol.% Al2O3 + 0.075 vol.% SiO2 8 10 13 

 

 

Figure 4:  Sedimentation time for the sample 0.1vol.%of SiO2 after 

15day 

3.2.Effect of temperature on physical properties 

3.2.1.Thermal conductivity 

       Fig. 5 introduces the variation of nanofluid thermal conductivity as 

a function of temperature for DW and all the studied nanofluid samples. By 

observing the results, the warm conductivity of the nanofluids increments 

with increment in temperature. With the ascent in temperature, while 

loosening the intermolecular bonds, the randombehaviour of nanoparticles 

- liquid collision will increase [6]. This is known asBrownian motion which 

suggested by Xuan and Roetzel [20]. Moreover, these results agree with the 

literature [27]. The spontaneous behavior of suspended nanoparticles in 

liquid media will increase as temperature goes up ,and weakening 

molecular bonds [28]. That is called a Brownian motion as proposed by 

Xuan and Roetzel [29].  Besides,  the increase in vol.% of Al2O3 at the 

component of nanofluids, the thermal conductivity will increase. Due to the 

high thermal conductivity of Al2O3 nanoparticles, as compared to SiO2 

nanoparticles, it leads to an important role for the better enhancement in the 

physical properties of base fluid [16]. 

 

 

Figure 5: Thermal conductivity of DW and various nanofluids as a 

function of temperature. 

3.2.2.Density 

 

  The physical properties of nanofluid  is specified by each of 

nanoparticles and  base fluid. The density of nanofluid is one of these 

properties  that changes  according to the density of nanoparticles and the 

base fluid. Since the solid have a density greater  than the liquid, the adding 

of the nanoparticles will raise the density of the base fluid. Fig. 6 presents 

the experimental data of densities that measured for DW andnano fluids 

(single and hybrid phase) with different temperatures.The figure shows that 

the Al2O3/DW  has a higher density than other nanofluids at all 

temperatures, because of the high density of Al2O3 nanoparticles[16]. For 

the hybrid nanofluids, density increased with increase in the quantity of 

Al2O3 nanoparticles due to its high density compared to SiO2 

nanoparticles[21]. It is shown also that density decreases with the increase 

of temperature to 70 °C for all samples and the decreasing tendency was 

slight. With the rise in temperature, the volume usually increases because 

the faster-moving molecules are further apart, which is cause a slightly 

decreasing in the density [21]. 

 



46 MARWA S.J. , HASAN. I. DAWOOD /AL-QADISIYAH JOURNALFOR ENGINEERING SCIENCES 14 (2021) 042–047 

 

 

Figure 6: Densities  of DW and various nanofluids as a function of 

temperatures 

3.2.3.Specific heat 
 

Heat transfer is significantly influenced by specific heat. Specific heat 

of nanofluid as the other physical properties depends on suspended 

nanoparticles and the base fluid .Fig. 7 shows the changes in specific heat 

for all nanofluids samples at various temperatures. Moreover, as shown in 

this figure, the specific heat of DW ishigher than other samples. The lower 

specific heat of nanoparticles is the reason that explains why the specific 

heat value of the mixture becomes lower than that of base fluid ( 4179.6 J / 

kg.k) [11].According to the data of this study, with an increase in 

temperature, the specific heat israised steadily and linearly.As the substance 

warms up, the normal dynamic vitality of the atoms increments. The 

crashes give enough vitality to permit turn to happen, at that point adds to 

the inside vitality and raises the particular warmth[30]. It seems that  

specific heat of  produced nanofluid  depends on the type of dispersants 

where  with increase the volume fraction of SiO2 to Al2O3in base fluid , the 

specific heat will decrease . That because of the specific heat capacity of  

SiO2 nanoparticles less than Al2O3 nanoparticles[31]. 

3.2.4.Viscosity 

Viscosities of tried examples were estimated in the temperature scope 

of 30 °C–70 °C and plotted in Fig. 8. [6, 32] indicated that there is an 

immediate connection among temperature and consistency of all trials in 

all conditions contrasted with the base liquid. It is observed that expanding 

temperature of the nanofluid diminishes its thickness. As the temperature 

expands the vitality level of fluid particles increments and the separation 

between the atoms increments and causes an abatement in intermolecular 

fascination between lessening inconsistency [16]. 

 

 

 

Figure 7: Specific heat of  DW and various samples as a function of 

temperatures. 

 

Figure 8: Results of DW and 0.1vol.% sample viscosities relative to 

temperatures. 

4. Conclusions 

In the present experimental study, the stability period of aluminium 

oxide(Al2O3), silicon dioxide(SiO2) and Al2O3–SiO2 hybrid was 

investigated at various ultrasonication times. Also, thethermal propertiesof 

DW and samples have been estimated at five different temperatures. The 

conclusions of the study are elaborated below: 

The stability period increases with increasing the ultrasonication time 

for all samples. 

The SiO2 nanofluid was found to be the most stable coolant, while Al2O3 

was found the lowest stable nanofluid.For the hybrid samples, the stability 

period increases with the increasing volumetric concentration of 

SiO2nanoparticles in the nanofluid. 

The thermal properties of nanofluids dependent directly on the 

temperature. Moreover, with increasing temperature, the thermal 

conductivity and specific heat of nanofluid increase,while density and 

viscosity decrease. 

The outcome of physical properties (thermal conductivity, density and 

specific heat) show that 0.1 vol.% Al2O3/DW has good results when 

compared to other working fluids.This means that the Al2O3 nanoparticles 

had a preferable thermal performance than SiO2 suspensions. For the hybrid 

nanofluids, the thermal properties showed good results with expanding the 

volume part of Al2O3 nanoparticles in the base fluid. 

REFERENCES 

 

  

[1] M.U. Sajid, H.M. Ali, Recent advances in application of nanofluids in heat transfer 

devices: a critical review, Renewable and Sustainable Energy Reviews, 103 

(2019) 556-592. 

[2] T. Alam, M.-H. Kim, A comprehensive review on single phase heat transfer 

enhancement techniques in heat exchanger applications, Renewable and 

Sustainable Energy Reviews, 81 (2018) 813-839. 

[3] N.A.C. Sidik, I.M. Adamu, M.M. Jamil, G. Kefayati, R. Mamat, G. Najafi, Recent 

progress on hybrid nanofluids in heat transfer applications: a comprehensive 

review, International Communications in Heat and Mass Transfer, 78 (2016) 68-

79. 

[4] S. Atashrouz, M. Mozaffarian, G. Pazuki, Viscosity and rheological properties of 

ethylene glycol+ water+ Fe 3 O 4 nanofluids at various temperatures: 

Experimental and thermodynamics modeling, Korean Journal of Chemical 

Engineering, 33(9) (2016) 2522-2529. 



MARWA S.J. , HASAN. I. DAWOOD /AL-QADISIYAH JOURNALFOR ENGINEERING SCIENCES 14(2021) 042–047                                47 

 

[5] M.H. Hamzah, N.A.C. Sidik, T.L. Ken, R. Mamat, G. Najafi, Factors affecting the 

performance of hybrid nanofluids: a comprehensive review, International Journal 

of Heat and Mass Transfer, 115 (2017) 630-646. 

[6] M. Gupta, V. Singh, S. Kumar, S. Kumar, N. Dilbaghi, Z. Said, Up to date review 

on the synthesis and thermophysical properties of hybrid nanofluids, Journal of 

cleaner production, 190 (2018) 169-192. 

[7] B. Ilhan, H. Ertürk, Experimental characterization of laminar forced convection of 

hBN-water nanofluid in circular pipe, International Journal of Heat and Mass 

Transfer, 111 (2017) 500-507. 

[8] M.H. Ahmadi, A. Mirlohi, M.A. Nazari, R. Ghasempour, A review of thermal 

conductivity of various nanofluids, Journal of Molecular Liquids, 265 (2018) 

181-188. 

[9] E. Sadeghinezhad, M. Mehrali, R. Saidur, M. Mehrali, S.T. Latibari, A.R. Akhiani, 

H.S.C. Metselaar, A comprehensive review on graphene nanofluids: recent 

research, development and applications, Energy Conversion and Management, 

111 (2016) 466-487. 

[10] R.A. Dehkordi, M.H. Esfe, M. Afrand, Effects of functionalized single walled 

carbon nanotubes on thermal performance of antifreeze: an experimental study 

on thermal conductivity, Applied Thermal Engineering, 120 (2017) 358-366. 

[11] M. Elias, I. Mahbubul, R. Saidur, M. Sohel, I. Shahrul, S. Khaleduzzaman, S. 

Sadeghipour, Experimental investigation on the thermo-physical properties of 

Al2O3 nanoparticles suspended in car radiator coolant, International 

Communications in Heat and Mass Transfer, 54 (2014) 48-53. 

[12] N.N. Esfahani, D. Toghraie, M. Afrand, A new correlation for predicting the 

thermal conductivity of ZnO–Ag (50%–50%)/water hybrid nanofluid: an 

experimental study, Powder Technology, 323 (2018) 367-373. 

[13] H. Yarmand, S. Gharehkhani, S.F.S. Shirazi, M. Goodarzi, A. Amiri, W.S. 

Sarsam, M.S. Alehashem, M. Dahari, S. Kazi, Study of synthesis, stability and 

thermo-physical properties of graphene nanoplatelet/platinum hybrid nanofluid, 

International Communications in Heat and Mass Transfer, 77 (2016) 15-21. 

[14] H. Yarmand, S. Gharehkhani, S.F.S. Shirazi, A. Amiri, E. Montazer, H.K. Arzani, 

R. Sadri, M. Dahari, S. Kazi, Nanofluid based on activated hybrid of biomass 

carbon/graphene oxide: synthesis, thermo-physical and electrical properties, 

International Communications in Heat and Mass Transfer, 72 (2016) 10-15. 

[15] E. Dardan, M. Afrand, A.M. Isfahani, Effect of suspending hybrid nano-additives 

on rheological behavior of engine oil and pumping power, Applied Thermal 

Engineering, 109 (2016) 524-534. 

[16] Z. Said, M.E.H. Assad, A.A. Hachicha, E. Bellos, M.A. Abdelkareem, D.Z. 

Alazaizeh, B.A. Yousef, Enhancing the performance of automotive radiators 

using nanofluids, Renewable and Sustainable Energy Reviews, 112 (2019) 183-

194. 

[17] A.M. Hussein, R. Bakar, K. Kadirgama, Study of forced convection nanofluid 

heat transfer in the automotive cooling system, Case Studies in Thermal 

Engineering, 2 (2014) 50-61. 

[18] G.A. Oliveira, E.M.C. Contreras, E.P. Bandarra Filho, Experimental study on the 

heat transfer of MWCNT/water nanofluid flowing in a car radiator, Applied 

Thermal Engineering, 111 (2017) 1450-1456. 

[19] B.C. Pak, Y.I. Cho, Hydrodynamic and heat transfer study of dispersed fluids 

with submicron metallic oxide particles, Experimental Heat Transfer an 

International Journal, 11(2) (1998) 151-170. 

[20] Y. Xuan, W. Roetzel, Conceptions for heat transfer correlation of nanofluids, 

International Journal of heat and Mass transfer, 43(19) (2000) 3701-3707. 

[21] C. Ho, J. Huang, P. Tsai, Y. Yang, Preparation and properties of hybrid water-

based suspension of Al2O3 nanoparticles and MEPCM particles as functional 

forced convection fluid, International Communications in Heat and Mass 

Transfer, 37(5) (2010) 490-494. 

[22] H. Brinkman, The viscosity of concentrated suspensions and solutions, The 

Journal of Chemical Physics, 20(4) (1952) 571-571. 

[23] S.A. Ahmed, M. Ozkaymak, A. Sözen, T. Menlik, A. Fahed, Improving car 

radiator performance by using TiO2-water nanofluid, Engineering science and 

technology, an international journal, 21(5) (2018) 996-1005. 

[24] Z. Said, A. Allagui, M.A. Abdelkareem, H. Alawadhi, K. Elsaid, Acid-

functionalized carbon nanofibers for high stability, thermoelectrical and 

electrochemical properties of nanofluids, J. Colloid Interface Sci., 520 (2018) 50-

57. 

[25] W. Rashmi, A. Ismail, I. Sopyan, A. Jameel, F. Yusof, M. Khalid, N. Mubarak, 

Stability and thermal conductivity enhancement of carbon nanotube nanofluid 

using gum arabic, Journal of Experimental Nanoscience, 6(6) (2011) 567-579. 

[26] W. Rashmi, M. Khalid, S. Ong, R. Saidur, Preparation, thermo-physical 

properties and heat transfer enhancement of nanofluids, Materials Research 

Express, 1(3) (2014) 032001. 

[27] V. Egan, P. Walsh, E. Walsh, On viscosity measurements of nanofluids in micro 

and mini tube flow, Journal of Physics D: Applied Physics, 42(16) (2009) 

165502. 

[28] J.K. Mannekote, S.V. Kailas, K. Venkatesh, N. Kathyayini, Environmentally 

friendly functional fluids from renewable and sustainable sources-A review, 

Renewable and sustainable energy reviews, 81 (2018) 1787-1801. 

[29] Z. Said, M. Sajid, R. Saidur, G. Mahdiraji, N. Rahim, Evaluating the optical 

properties of TiO2 nanofluid for a direct absorption solar collector, Numerical 

Heat Transfer, Part A: Applications, 67(9) (2015) 1010-1027. 

[30] T.-P. Teng, C.-C. Yu, Heat dissipation performance of MWCNTs nano-coolant 

for vehicle, Experimental Thermal and Fluid Science, 49 (2013) 22-30. 

[31] G.M. Moldoveanu, G. Huminic, A.A. Minea, A. Huminic, Experimental study on 

thermal conductivity of stabilized Al2O3 and SiO2 nanofluids and their hybrid, 

International Journal of Heat and Mass Transfer, 127 (2018) 450-457. 

[32] M. Gupta, V. Singh, R. Kumar, Z. Said, A review on thermophysical properties 

of nanofluids and heat transfer applications, Renewable and Sustainable Energy 

Reviews, 74 (2017) 638-670.