An experimental investigation on the effects of surfactants on the thermal performance of hybrid nanofluids in helical coil heat exchangers

An experimental investigation on the effects of surfactants on the thermal performance of hybrid nanofluids in helical coil heat exchangers

ICHMT-03520; No of Pages 6 International Communications in Heat and Mass Transfer xxx (2016) xxx–xxx Contents lists available at ScienceDirect Inter...

2MB Sizes 3 Downloads 51 Views

ICHMT-03520; No of Pages 6 International Communications in Heat and Mass Transfer xxx (2016) xxx–xxx

Contents lists available at ScienceDirect

International Communications in Heat and Mass Transfer journal homepage: www.elsevier.com/locate/ichmt

3Q1

F. Hormozi, B. ZareNezhad ⁎, H.R. Allahyar Faculty of Chemical, Petroleum and Gas Engineering, Semnan University, Semnan, Iran

6

a r t i c l e

i n f o

a b s t r a c t

In the present study, the effects of surfactants on the thermal performance of the hybrid nanofluid (Alumina–Silver) at constant wall temperature and laminar flow have been experimentally studied in a helical coil heat exchanger. Different surfactants such as anionic Sodium Dodecyl Sulfate (SDS) and nonionic Poly Vinyl Pyrrolidone (PVP) in the concentration of range of 0.1–0.4 wt.% are employed. It is found that the thermal performance can be maximized by using the 0.2 vol.% hybrid nanofluid and 0.1 wt.% SDS anionic surfactant in the helical coil. The maximum thermal performance in the presence of hybrid Alumina–Silver nanofluid and SDS anionic surfactant is 16% higher than that of the pure distilled water. The presented results can have potential application in process intensification and optimum design of heat exchangers. © 2016 Published by Elsevier Ltd.

Available online xxxx

D

P

Keywords: Thermal performance Hybrid nanofluid Anionic surfactant Nonionic surfactant Helical coil Heat exchanger

43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58

C

E

R

41 42

R

39 40

Effect of curved pipes on the thermal performance enhancement of fluids and nanofluids has been investigated for design of new heat exchangers in recent years. Most results have shown that the fluid thermal performance is improved because of creating more contact surface and centrifugal force [1–4]. For the first time in 1995, Choi [5] discussed the effect of nanofluid on thermal conductivity. After that, a lot of researches who have investigated the thermo-physical properties of nanofluid, reported the thermal conductivity enhancement in comparison with the base fluid [6–11]. Suresh et al. [11,12] have investigated the thermal performance of alumina and copper oxide nanofluid using the twisted tape inserts in tube under constant heat flux and laminar flow conditions. They have concluded that under constant thermal conditions in the twisted tape, copper oxide nanofluid shows better performance as compared to the alumina nanofluid. In addition, copper oxide nanofluid imposes higher pressure drop as compared to the alumina nanofluid and the use of twisted tape increases this pressure drop to a greater extent. Hybrid nanofluid is a new class of nanofluid which is made of two or more particles in combination with different percentages. The topic has attracted many researchers' attention in recent years. Most of them have found out that using nanocomposites in the base fluid results in improving thermal performance [12–16]. Lots of researches have also investigated the effects of surfactants on the stability of the nanoparticles [17–22].

N C O

37 38

1. Introduction

U

35 36

T

33 31 30 32 34

14 13 15 16 17 18 19 20 21

E

7 8 10 9 12 11 23 24 25 26 27 28 29 22

R O

4 5

O

F

2

An experimental investigation on the effects of surfactants on the thermal performance of hybrid nanofluids in helical coil heat exchangers☆

1

☆ Communicated by W.J. Minkowycz. ⁎ Corresponding author. E-mail address: [email protected] (B. ZareNezhad).

Since there are limited information on the effect of surfactants on thermal performance of hybrid nanofluids in the helical coil heat exchangers, the variations of Nusselt number, pressure drop and thermal performance in the presence of different compositions of SDS anionic and PVP nonionic surfactants are experimentally investigated in this work.

59 60

2. Experimental

65

2.1. Set-up and instruments

66

According to Fig. 1, testing devices include stainless steel tank and temperature and pressure control systems. The tank is fully insulated with rock wool in order to avoid heat loss and a 2 kW heater is immersed in the tank to supply the required heat. In order to measure the inlet and outlet pressure, a very sensitive pressure transmitter has been used (SENSYS, 0.5BCIA PSCH). Two accurate thermocouples of T-type have been used for accurate measurement of the inlet and outlet temperatures. In addition, six thermocouples of K- type have been installed at various locations to measure the surface temperatures of the helical coil. Flow rate is estimated by an ultrasonic system with the accuracy of about 0.05 l per minutes. The used coil is made of copper, which its physical features are shown in Table 1. The device is first calibrated with pure water and then the main testing is started with hybrid nanofluid at different concentrations. As soon as the temperature reaches to a saturation state (constant temperature of 95 °C), we started to collect data including inlet and outlet temperature, inlet and outlet pressure as well as the surface temperature. An experiment has been repeated at least two times to ensure that the date is accurate. The employed hybrid nanofluid contains Alumina(97.5%)–Silver(2.5%)

67

http://dx.doi.org/10.1016/j.icheatmasstransfer.2016.09.022 0735-1933/© 2016 Published by Elsevier Ltd.

Please cite this article as: F. Hormozi, et al., An experimental investigation on the effects of surfactants on the thermal performance of hybrid nanofluids in helical coil heat exchangers, Int. Commun. Heat Mass Transf. (2016), http://dx.doi.org/10.1016/j.icheatmasstransfer.2016.09.022

61 62 63 64

68 69 70 71 72 73 74 75 76 77 78 79 80 81 82 83 84 85

2

F. Hormozi et al. / International Communications in Heat and Mass Transfer xxx (2016) xxx–xxx

Cp d D h K L Nu Re T U

T1:13 T1:14 T1:15 T1:16 T1:17 T1:18 T1:19

Greek letters ΔP Axial pressure drop (Pa) η Thermal performance factor ρ Density (kg·m−3) μ Dynamic viscosity (Pa·s) φ Nanoparticle volume fraction (%)

T1:20 T1:21 T1:22 T1:23 T1:24 T1:25 T1:26 T1:27 T1:28 T1:29 T1:30

Subscripts C Coiled tube ex Experimental f Base fluid nf Nanofluid nfs Nanofluid with surfactant p Particle S Straight tube th Theoretical w Wall

Specific heat (J·kg−1·K−1) Inside diameter of tube (m) Diameter of coil (m) Heat transfer coefficient (W·m−2·K−1) Thermal conductivity (W·m−1·K−1) Length of tube (m) Average Nusselt number Reynolds number Temperature (K) Average velocity (m·s−1)

Tube

d

t

L

D

λ

N

t1:3

Helical coil

5

1

2600

65

15

10

t1:4

presented in Tables 2 and 3. The measurement accuracies of different 101 instruments are given in Table 4 as well. 102

The thermophysical characteristics of the nanofluid are calculated 104 according to the following equations: [23–25]. 105 ρnf ¼ ð1− φÞ  ρ f þ φ  ρP μf ð1− φÞ2:5

R O

μ nf ¼

P

 knf kP þ 2k f − 2 k f − kP  φ  : ¼ kf kP þ 2kf þ k f − kP  φ

97 98 99 100

111 113

ð4Þ

D

116

E

The experimental convective heat transfer coefficient and the Nusselt number are determined according to the following equations: 117

T

C

E

R

R

O

95 96

ð3Þ

Thermal conductivity is also calculated using the following equation [26]: 114

nanocomposite with an average diameter of 80 nm (with spherical shape). The mixed hybrid nanofluids at a constant concentration 0.2 vol.% and using different concentrations of Sodium Dodecyl Sulfate (SDS) anionic and nonionic Poly Vinyl Pyrrolidone (PVP) surfactants in the range of 0.1–0.4 wt.% are provided by intense mixing via an ultrasonic device. There are numerous ways to prepare nanoparticles, one of which is Sol–gel. One of the advantages of this method is to prepare nanocomposites with high purity. Initially a homogenous suspension including solvent and precursor is solved and then the homogenous solution is turned into Sol by hydrolysis. After provoking the particles in Sol by HCl and NaOH, they join together and form a wet gel. Then after separating the solution and drying it, the nanoparticles are formed. Fig. 2 shows the TEM (transmission electron microscopy) images of dispersed nanoparticles in distilled water. The specifications of the employed nanoparticles and surfactants used in this study are

C

93 94

110





Nuð expÞ ¼



hð expÞ  d knf

ð5Þ

119 120

ð6Þ 122

where (Tw − Tb)M is a logarithmic temperature difference. 3. Results and discussion

123

3.1. Heat transfer rate in the presence of ionic surfactant

124

The trend of variation of hybrid nanofluid Nusselt number at different concentrations of anionic surfactant (SDS) is shown in Fig. 3. Comparing with the case of distilled water, the Nusselt number increases as anionic surfactant concentration is increased. As shown, an increase in the Reynolds number leads to an increase in heat transfer

125

N

91 92

108

U

89 90

ð1Þ 107 ð2Þ

ðρ  C P Þnf ¼ ð1− φÞ  ðρ  C P Þ f þ φ  ρ  C p P :

 ð expÞ ¼ m  cp  T b1 − T b2 h A  ðT w − T b ÞM

87 88

103

2.2. Determination of experimental Nusselt number

F

T1:2 T1:3 T1:4 T1:5 T1:6 T1:7 T1:8 T1:9 T1:10 T1:11 T1:12

O

Nomenclature

86

t1:1 t1:2

Table 1 Geometrical characteristics of the Helical Coil (mm).

T1:1

Fig. 1. The experimental set-up employed in the present study.

Please cite this article as: F. Hormozi, et al., An experimental investigation on the effects of surfactants on the thermal performance of hybrid nanofluids in helical coil heat exchangers, Int. Commun. Heat Mass Transf. (2016), http://dx.doi.org/10.1016/j.icheatmasstransfer.2016.09.022

126 127 128 129

3

F

F. Hormozi et al. / International Communications in Heat and Mass Transfer xxx (2016) xxx–xxx

P

R O

O

Fig. 3. Variation of Nusselt number for hybrid nanofluid by using different concentrations of anionic surfactant (SDS).

t2:1 t2:2

Table 2 Thermophysical characterization of nanopowders.

C

138 139

E

136 137

R

134 135

R

132 133

T

140 141

rate at given concentrations of anionic surfactant. In addition, improvement of the stability of hybrid nanofluid by using an anionic surfactant (at all concentrations) has a positive effect on the Nusselt number enhancement at different agitation intensities. The maximum nanoparticle stability is obtained at the SDS concentration of 0.1 wt.% where the maximum Nusselt number is obtained. The variations of the Nusselt number enhancement ratio (ratio of hybrid nanofluid Nusselt number with anionic surfactant to hybrid nanofluid Nusselt number without anionic surfactant) are presented in Fig. 4. It is shown that by adding anionic surfactant to hybrid nanofluid, the stability of nanoparticles in base fluid is improved such that the rate of heat transfer is increased. It should be noted that at anionic surfactant concentrations higher

Particle/base fluid

Average diameter (nm)

Purity (%)

Actual density (kg/m3)

CP (J/kg·K)

k (W/m·K)

t2:5 t2:6 t2:7

Al2O3 Ag nanocomposite

55 25 80

99 99 99

3690 9320 3830.75

780 233 766

30.5 429 41

N C O

t2:3 t2:4

Table 3 Properties of the employed surfactants.

U

t3:1 t3:2 t3:3

Surfactant

t3:4 t3:5

Sodium Dodecyl Sulfate (SDS) Poly Vinyl Pyrrolidone (PVP)

t4:1 t4:2 t4:3 t4:4 t4:5 t4:6 t4:7 t4:8

E

130 131

D

Fig. 2. TEM image of hybrid nanoparticles.

The molecular formula

Molecular weight

Density (g/cm3)

NaC12H25SO4 (C6H9NO)n

288.372 N105

1.01 1.2

Fig. 4. Variation of Nusselt number enhancement ratio for hybrid nanofluid by using different concentrations of anionic surfactant (SDS).

than 0.1 wt.%, the stability of nanoparticles is gradually decreased and thus a lower Nusselt number enhancement ratio is obtained [17,21]. According to Figs. 5 and 6, nanoparticles carry positive charge in a neutral aqueous environment. When a low concentration Sodium Dodecyl Sulfate (0.1 wt.%) is added to the hybrid nanofluid, the sodium cations of material (hydrophilic group) approach the base fluid and its sulfate anions (hydrophobic groups) that are made from a long dodecyl carbon chain (C12H25) are attracted on the surface of nanoparticles. Therefore, the nanoparticle surface has taken negative charge. Anionic groups are pulled into the inner layer and lead to strengthen the negative charge on the surface of nanoparticles. Moreover, it causes an increase in the thickness of electric double layer (EDL) and thus an increase in the absolute amount of zeta potential of the surface of nanoparticles such that a repulsive force between nanoparticles is created and the stability of nanoparticles in the base fluid is increased. As concentration of Sodium Dodecyl Sulfate increases, the concentration of sodium cations increases (positive charge) such that the cationic group enters into the inner layer. Thus, the net negative charge of the

Table 4 Uncertainty of measurement instruments. Parameter Fluid flow rate Steam temperature sensors Wall temperature sensors Inlet/outlet temperature sensors Pressure transmitters

Instrument ®

Flownetix 100series™ PT-100 Ω thermo resistance K-type Omega Thermocouples PT-100 Ω thermo resistance Keller, Series 35X-Bullet type

uncertainty ±1% of reading 0.1 K 0.1 K 0.1 K ±1% of reading

Fig. 5. (a) Chemical structure of SDS surfactant (NaC 12 H 25 SO 4 ), (b) schematic representation of surfactant micelle encapsulation over a nanoparticle.

Please cite this article as: F. Hormozi, et al., An experimental investigation on the effects of surfactants on the thermal performance of hybrid nanofluids in helical coil heat exchangers, Int. Commun. Heat Mass Transf. (2016), http://dx.doi.org/10.1016/j.icheatmasstransfer.2016.09.022

142 143 144 145 146 147 148 149 150 151 152 153 154 155 156 157 158 159

4

F. Hormozi et al. / International Communications in Heat and Mass Transfer xxx (2016) xxx–xxx

R O

O

F

Fig. 8. Variation of Nusselt number enhancement ratio for hybrid nanofluid by using different concentrations of nonionic surfactant (PVP).

3.2. Heat transfer rate in the presence of nonionic surfactant

171

According to Fig. 7 an increase in the concentration of nonionic surfactant (PVP) for the case of hybrid nanofluid leads to an increase in the stability of nanoparticles such that the Nusselt number of hybrid nanofluid at a given Reynolds number is improved. According to Fig. 8, the maximum increase in the rate of heat transfer occurs at the PVP concentration of 0.4 wt.%. As shown in Fig. 9, PVP doesn't have the potential of ionization in the base fluid. However its hydrophilic group which includes oxygen atoms can make hydrogen bond with water. At a low PVP concentration (i.e. 0.1 wt.%) in hybrid nanofluid, the molecules of PVP cannot cover the whole surface of nanoparticles such that nonionic surfactant molecule on nanoparticles can be connected to other nanoparticles from its side chain and it probably makes some of the nanoparticles agglomerate and cluster. As shown in Fig. 8, the more increase in the concentration of PVP nonionic surfactant, the more

178 179 180 181 182 183 184

Fig. 10. Variation of Nusselt number enhancement ratio for hybrid nanofluid by using different concentrations of SDS or PVP.

R

E

C

Fig. 7. Variation of Nusselt number for hybrid nanofluid by using different concentrations of nonionic surfactant (PVP).

R

176 177

O

174 175

C

172 173

Fig. 9. a: Chemical structure of SDS surfactant (NaC12H25SO4). b: Chemical structure of PVP surfactant(C6H9NO)n.

complete coverage of surfactant molecules around nanoparticles. This leads to a better repulsive force and a better stability of the nanoparticles. With an increase in the concentration of PVP up to 0.4 wt.%, the surface of nanoparticles is significantly covered with surfactant. Thus with an increase in the thickness of the electric double layer, the net charge of surface of nanoparticles and consequently absolute value of the Zeta potential of surface of nanoparticles are increased. Increasing the thickness of the electrical double layer creates a repulsive force between the nanoparticles resulting in further dispersion and the stability of the nanoparticles in the base fluid and thus improving the heat transfer. The greatest increase in Nusselt number enhancement ratio is about 6.425% at the PVP concentration of 0.4 wt.% and Re of 5100 [22,32] as shown in Fig. 8. The Nusselt number enhancement ratio for hybrid nanofluid in the presence of SDS anionic and PVP nonionic surfactants are compared in Fig. 10 at different species concentrations. At lower Reynolds number,

N

167 168

U

165 166

D

170

163 164

T

169

nanoparticles and the zeta potential of surface of nanoparticles are decreased and the stability of nanoparticles is reduced. This decrease in stability results in an increase in agglomeration and settling rate of nanoparticles which in turn reduces the thermal performance. Therefore the stability or instability of nanoparticles has a considerable role in the enhancement of thermal performance of hybrid nanofluid. The maximum heat transfer rate is obtained at 0.1 wt.% concentration of SDS anionic surfactant at all agitation intensities and the maximum Nusselt number enhancement ratio is about 6.283% at the Reynolds number (Re) of 5100 as shown in Fig. 4 [32–34].

161 162

E

160

P

Fig. 6. Type of colloidal stabilization (electrostatic stabilization).

Please cite this article as: F. Hormozi, et al., An experimental investigation on the effects of surfactants on the thermal performance of hybrid nanofluids in helical coil heat exchangers, Int. Commun. Heat Mass Transf. (2016), http://dx.doi.org/10.1016/j.icheatmasstransfer.2016.09.022

185 186 187 188 189 190 191 192 193 194 195 196 197 198 199 200

F. Hormozi et al. / International Communications in Heat and Mass Transfer xxx (2016) xxx–xxx

212 213 214 215 216 217 218 219 220 221 222 223 224 225 226 227 228 229

3.3. Pressure drop in the helical coil

231 232

According to Fig. 11 an increase in Reynolds number and the concentration of SDS or PVP surfactants at a fixed concentration of hybrid nanofluid leads to a slight increase in helical coil pressure drop. This can be attributed to the increase of nanofluid viscosity due to an increase in the surfactant concentrations. Also an excessive increase of surfactant concentrations for the case of SDS speeds up the agglomeration process and settling of nanoparticles in the coil such that a higher pressure drop is experienced. In Fig. 12, pressure drop enhancement ratio of hybrid nanofluid with respect to distilled pure water at different SDS or PVP concentrations are presented. The greatest pressure drop is related to the hybrid nanofluid with SDS anionic surfactant at the concentration of 0.4 wt.% at the Reynolds number 5100. Using helical coil instead of straight pipe produces a more increase in pressure drop of hybrid nanofluid. [17,40]. The pressure drop enhancement ratio for 0.1 wt.% SDS (=1.03) is lower than that of the 0.4 wt.% PVP in the hybrid nanofluid (=1.07) indicating a 60% decrease in frictional loss when the

240 241 242 243 244 245 246

C

E

R

R

238 239

N C O

237

249

3.4. Thermal performance of hybrid nanofluid in the helical coil

Thermal performance ratio of the helical coil to the straight tube for 250 the hybrid nanofluid with surfactant is defined as follows [41]: 251 NuC;nfS NuS; f η¼ 0:1666 : ΔP C;nfS ΔP S; f

ð7Þ

According to Fig. 13, the thermal performance ratio for all cases is greater than one. The helical coil exhibits better heat transfer performance than a straight tube because of centrifugal force and secondary flow. Also by using the optimum concentrations of surfactants in the employed hybrid nanofluid, the suspension stability and the heat transfer rate are enhanced. According to Fig. 15 the maximum increase in the thermal performance ratio belongs to 0.1 wt.% concentration of SDS anionic surfactant which is equal to 1.1636. Thus the hybrid Alumina–Silver nanofluid (with concentration of 0.2 vol.%) with 0.1 wt.% SDS anionic surfactant show the best thermal performance in the employed helical coil heat exchanger.

Fig. 11. The hybrid nanofluid pressure drop in the presence of SDS and PVP surfactants.

253 254 255 256 257 258 Q4 259 260 261 262 263

4. Conclusion

264

In the present study, the effects of surfactants on the thermal performance of the hybrid nanofluid (prepared by using Alumina–Silver nanocomposite with 0.2 vol.% concentration) have been studied experimentally in a helical coil. The Sodium Dodecyl Sulfate (SDS) anionic surfactant and Poly Vinyl Pyrrolidone (PVP) nonionic surfactant in the concentration range of 0.1–0.4 wt.% are employed. The maximum heat

265 266

U

235 236

hybrid nanofluid in the presence of 0.1 wt.% SDS in helical coil is 247 employed. 248

T

230

233 234

Fig. 12. The hybrid nanofluid pressure drop enhancement ratio in the presence of SDS and PVP surfactants.

F

210 211

O

208 209

R O

207

P

205 206

D

203 204

thermal conductivity is the main influencing factor in controlling the rate of heat transfer. With increasing Reynolds number, the effect of thermal conductivity on the heat transfer becomes less considerable. [35,36]. On the other hand, the importance of other mechanisms including Brownian movement of nanoparticles, migration of the nanoparticles and reduction of thickness of boundary layer becomes more tangible in the increase in heat transfer rate [37–39]. In addition, at higher rate of Reynolds number, the effects of dispersion and turbulent movement lead to increase in fluid fluctuations and heat transfer rate. Moreover, it can be concluded that by increasing the concentration of both surfactants (anionic and nonionic) in hybrid nanofluid, the stability is increased and consequently the thermal performance of nanofluid is improved. As shown, the greatest increase in stability and the heat transfer rate is related to 0.4 wt.% of PVP nonionic surfactant in hybrid nanofluid in the helical coil. The results show that hybrid nanofluid with 0.1 wt.% of SDS anionic surfactant nearly has the same thermal performance as 0.4 wt.% of PVP nonionic surfactant. However, by increasing the concentration of SDS anionic surfactant from 0.1 wt.% to 0.4 wt.%, the stability of nanoparticles and the rate of heat transfer are gradually decreased. It is interesting to note that the PVP nonionic surfactant shows an opposite behavior. By increasing the concentration of PVP nonionic surfactant from 0.1 wt.% to 0.4 wt.%, the stability of nanoparticles and the rate of heat transfer are gradually increased according to the aforementioned discussion. As shown in Fig. 10, the maximum Nusselt number enhancement ratio of 1.063 (6.3% increase in heat transfer rate) can be obtained by using SDS anionic surfactant at a concentration as low as 0.1 wt.%. This concentration is 75% lower than the required concentration of 0.4 wt.% of PVP nonionic surfactant for the same duty.

E

201 202

5

Fig. 13. The variation of thermal performance of the helical coil with respect to the straight tube for the hybrid nanofluid in the presence of SDS or PVP.

Please cite this article as: F. Hormozi, et al., An experimental investigation on the effects of surfactants on the thermal performance of hybrid nanofluids in helical coil heat exchangers, Int. Commun. Heat Mass Transf. (2016), http://dx.doi.org/10.1016/j.icheatmasstransfer.2016.09.022

267 268 269 270

278 279 280 281 282 283 284 285

[27–31]

289

References

290 291 292 293 294 295 296 Q3 297 298 299 300 301 302 303 304 305 306 307 308 309 310 311 312 313 314 315 316 317 318 319 320 321 322 323 324 325 326 327 328 329

[1] V. Kubair, N.R. Kuloor, Heat transfer to Newtonian fluids in coiled pipes in laminar flow, Int. J. Heat Mass Transf. 9 (1966) 63–75. [2] M. Fakoor-Pakdaman, M.A. Akhavan-Behabadi, P. Razi, An experimental investigation on thermo-physical properties and overall performance of MWCNT/heat transfer oil nanofluid flow inside vertical helically coiled tubes, Exp. Thermal Fluid Sci. 40 (2012) 103–111. [3] R.A. Seban, E.F. Mclaughlint, Heat transfer in tube coil with laminar and turbulent flow, Heat Mass Transf. 6 (1962) 387–395. [4] R.L. Manlapaz, S.W. Churchill, Fully developed laminar convection from a helical coil, Chem. Eng. 9 (1980) 185–200. [5] S.U.S. Choi, Enhancing thermal conductivity of fluids with nanoparticle, ASME FED 231 (1995) 99–105. [6] M. Tajik Jamal-Abad, A.H. Zamzamian, M. Dehghan, Experimental studies on the heat transfer and pressure drop characteristics of Cu–water and Al–water nanofluids in a spiral coil, Exp. Thermal Fluid Sci. 47 (2013) 206–212. [7] S. Zeinali Heris, S.G. Etemad, M. Nasr Esfahany, Experimental investigation of oxide nanofluid laminar flow convective heat transfer, Int. Commun. Heat Mass Transf. 33 (2006) 529–535. [8] S. Zeinali Heris, M. Nasr Esfahany, S.G. Etemad, Experimental investigation of convective heat transfer of Al2O3/water nanofluid in circular tube, Int. J. Heat Fluid Flow 28 (2) (2007) 203–210. [9] J.A. Eastman, S.U.S. Choi, S. Li, W. Yu, L.J. Thompson, Anomalously increased effective thermal conductivities of ethylene glycol-based nanofluids containing copper nanoparticles, Appl. Phys. Lett. 78 (2001) 718–720. [10] M.A. Akhavan-Behabadi, M. Fakoor Pakdaman, M. Ghazvini, Experimental investigation on the convective heat transfer of nanofluid flow inside vertical helically coiled tubes under uniform wall temperature condition, Int. Commun. Heat Mass Transf. 39 (2012) 556–564. [11] S. Suresh, K.P. Venkitaraj, P. Selvakumar, Comparative study on thermal performance of helical screw tape inserts in laminar flow using Al2O3/water and CuO/water nanofluids, Superlattice. Microst. 49 (2011) 608–622. [12] S. Suresh, K.P. Venkitaraj, P. Selvakumar, M. Chandrasekar, Effect of Al2O3–Cu/water hybrid nanofluid in heat transfer, Exp. Thermal Fluid Sci. 38 (2012) 54–60. [13] M. Baghbanzadeh, A. Rashidi, A.H. Soleimanisalim, D. Rashtchian, Investigating the rheological properties of nanofluids of water/hybrid nanostructure of spherical silica/MWCNT, Thermochim. Acta 578 (2014) 53–58. [14] M.A. Baghbanzadeh, A. Rashidi, D. Rashtchian, R. Lotfi, A. Amrollahi, Synthesis of spherical silica/multiwall carbon nanotubes hybrid nanostructures and investigation of thermal conductivity of related nanofluids, Thermochim. Acta 549 (2012) 87–94.

U

N

C

O

R

R

E

C

T

288

F

277

O

Uncited references

275 276

R O

287 Q2

273 274

[15] L. Syam Sundar, M.K. Singh, A.C.M. Sousa, Enhanced heat transfer and friction factor of MWCNT–Fe3O4/water hybrid nanofluids, Int. Commun. Heat Mass Transf. 52 (2014) 73–83. [16] D. Madhesh, R. Parameshwaran, S. Kalaiselvam, Experimental investigation on convective heat transfer and rheological characteristics of Cu–TiO2 hybrid nanofluids, Exp. Thermal Fluid Sci. 52 (2014) 104–115. [17] C. Choi, H.S. Yoo, J.M. Oh, Preparation and heat transfer properties of nanoparticlein-transformer oil dispersions as advanced energy-efficient coolants, Curr. Appl. Phys. 8 (2008) 710–712. [18] L. Yang, K. Du, X.S. Zhang, B. Cheng, Preparation and stability of Al 2 O 3 nano-particle suspension of ammonia water solution, Appl. Therm. Eng. 31 (2011) 3643–3647. [19] K. Wusiman, H. Jeong, K. Tulugan, H. Afrianto, H. Chung, Thermal performance of multi-walled carbon nanotubes (MWCNTs) in aqueous suspensions with surfactants SDBS and SDS, Int. Commun. Heat Mass Transf. 41 (2013) 28–33. [20] L. Chen, H. Xie, Properties of carbon nanotube nanofluids stabilized by cationic gemini surfactant, Thermochim. Acta 506 (2010) 62–66. [21] L. Chen, H. Xie, Surfactant-free nanofluids containing double- and single-walled carbon nanotubes functionalized by a wet-mechanochemical reaction, Thermochim. Acta 497 (2010) 67–71. [22] X. Li, D. Zhu, X. Wang, Evaluation on dispersion behavior of the aqueous copper nano-suspensions, J. Colloid Interface Sci. 310 (2007) 456–463. [23] B.C. Pak, Y. Cho, Hydrodynamic and heat transfer study of dispersed fluids with submicron metallic oxide particle, Exp. Heat Transf. 11 (1998) 151–170. [24] Y. Xuan, W. Roetzel, Conceptions for heat transfer correlation of nanofluids, Int. J. Heat Mass Transf. 43 (2000) 3701–3707. [25] B. H.C, The viscosity of concentrated suspensions and solution, J. Chem. Phys. 20 (1952) 571. [26] F.J. Wasp, Solid–Liquid Slurry Pipeline Transportation, Trans. Tech, Berlin, 1977. [27] F.P. Incropera, D.P. De Witt, Fundamentals of Heat and Mass Transfer, fourth ed. John Wiley, New York, 1996. [28] R.A. Seban, E.F. Mclaughlint, Heat transfer in tube coil with laminar and turbulent flow, Heat Mass Transf. 6 (1962) 387–395. [29] M. Van Dyke, Extended Stokes series: laminar flow through a loosely coiled pipes, J. Fluid Mech. 86 (1978) 129–145. [30] V. Kubair, C.B.S. Varrier, Pressure drop for liquid flow in helical coils, Trans. Indian Inst. Chem. Eng. 14 (1961) 93. [31] H.D. Young, Statistical Treatment of Experimental Data, McGraw-Hill, New York, 1962. [32] W. Yu, H. Xie, A review on nanofluids: preparation, stability mechanisms, and applications, J. Nanomater. 1-17 (2012). [33] D. Zhu, X. Li, N. Wang, X. Wang, J. Gao, H. Li, Dispersion behavior and thermal conductivity characteristics of Al2O3–H2O nanofluids, Curr. Appl. Phys. 9 (2009) 131–139. [34] V. Karthik, S. Ghosh, S.K. Pabi, Effects of bulk stoichiometry and surface state of NiAl nano-dispersoid on the stability and heat transfer characteristics of water based nanofluid, Exp. Thermal Fluid Sci. 48 (2013) 156–162. [35] D. Wen, Y. Ding, Experimental investigation into convective heat transfer of nanofluid at the entrance region under laminar flow conditions, Int. J. Heat Mass Transf. 47 (24) (2004) 5181–5188. [36] H. Chen, W. Yang, Y. He, Y. Ding, L. Zhang, C. Tan, A.A. Lapkin, D.V. Bavykin, Heat transfer behaviour of aqueous suspensions of titanate nanofluid, Powder Technol. 183 (2008) 63–72. [37] A.A. Abbasian Arani, J. Amani, Experimental investigation of diameter effect on heat transfer performance and pressure drop of TiO2-water nanofluid, Exp. Thermal Fluid Sci. 44 (2013) 520–533. [38] M. Chandrasekar, S. Suresh, A. Chandra Bose, Experimental studies on heat transfer and friction factor characteristics of Al2 O 3 /water nanofluid in a circular pipe under laminar flow with wire coil inserts, Exp. Thermal Fluid Sci. 34 (2010) 122–130. [39] S. Suresh, M. Chandrasekar, S. Chandra Sekhar, Experimental studies on heat transfer and friction factor characteristics of CuO/water nanofluid under turbulent flow in a helically dimpled tube, Exp. Thermal Fluid Sci. 35 (2011) 542–549. [40] M. Drzazga, A. Gierczycki, G. Dzido, M. Lemanowicz, Influence of nonionic surfactant addition on drag reduction of water based nanofluid in a small diameter pipe, Chin. J. Chem. Eng. 21 (2013) 104–108. [41] H. Usui, Y. Sano, K. Iwashita, A. Isozaki, Enhancement of heat transfer by a combination of internally grooved rough tube and twisted tape, Int. Chem. Eng. 26 (1) (1996) 97–104.

P

286

transfer rate is obtained at 0.1 wt.% concentration of SDS anionic surfactant at all agitation intensities and the maximum Nusselt number enhancement ratio is about 6.283% at the Reynolds number of 5100. This concentration is 75% lower than the required concentration of 0.4 wt.% of PVP nonionic surfactant for the same duty. The pressure drop enhancement ratio for 0.1 wt.% SDS (= 1.03) is lower than that of the 0.4 wt.% PVP in the hybrid nanofluid (= 1.07) indicating a 60% decrease in frictional loss when the hybrid nanofluid in the presence of 0.1 wt.% SDS in helical coil is employed. The maximum increase in the thermal performance ratio (about 1.1636) can be achieved by using 0.1 wt.% concentration of SDS anionic surfactant. Thus the maximum thermal performance in the presence of hybrid Alumina– Silver nanofluid and SDS anionic surfactant is 16% higher than that of the pure distilled water. The proposed approach can be used as an energy saving technique for design of new compact heat exchangers and economizers.

D

271 272

F. Hormozi et al. / International Communications in Heat and Mass Transfer xxx (2016) xxx–xxx

E

6

Please cite this article as: F. Hormozi, et al., An experimental investigation on the effects of surfactants on the thermal performance of hybrid nanofluids in helical coil heat exchangers, Int. Commun. Heat Mass Transf. (2016), http://dx.doi.org/10.1016/j.icheatmasstransfer.2016.09.022

330 331 332 333 334 335 336 337 338 339 340 341 342 343 344 345 346 347 348 349 350 351 352 353 354 355 356 357 358 359 360 361 362 363 364 365 366 367 368 369 370 371 372 373 374 375 376 377 378 379 380 381 382 383 384 385 386 387 388 389 390 391 392 393 394 395 396 397 398