999精品在线视频,手机成人午夜在线视频,久久不卡国产精品无码,中日无码在线观看,成人av手机在线观看,日韩精品亚洲一区中文字幕,亚洲av无码人妻,四虎国产在线观看 ?

Hydrodynamic cavitation as an efficient method for the formation of sub-100 nm O/W emulsions with high stability

2016-05-26 09:28:51ZhiliangZhangGuangquanWangYongNieJianbingJi
Chinese Journal of Chemical Engineering 2016年10期

Zhiliang Zhang*,Guangquan Wang,Yong Nie,Jianbing Ji

Zhejiang Provincal Key Laboratory of Biofuel,College of Chemical Engineering,Zhejiang University of Technology,Hangzhou 310014,China

1.Introduction

Emulsion is a dispersion consisting of at least two immiscible liquids,with one of the liquids being dispersed as small,spherical droplets in the other[1].Nowadays,a growing interest has been attracted on utilization of emulsions in food[1,2],cosmetic[3],pharmaceutical[4],and chemical industries[5].The properties of emulsions depend on their droplet size and size distribution[6–8].Preparation of emulsions with small droplet size and high stability is attractive for both theoretical and practical point of view[6].

Generally,two approaches are employed for the formation of emulsions:high-energy approaches and low-energy approaches[1].The high-energy approaches include high-pressure homogenization[9,10],colloid mills[11],and sonication[5,12,13].Emulsions produced by these techniques had high stability[14,15].However,high-energy approaches are usually associated with high-energy input,making them unfavorable for industrial applications[6,16].Viewing the drawbacks of the high-energy approaches,several novel methods with low-energy consumption have been investigated for the formation of emulsions,such as membrane emulsification[17]and microchannel emulsification[18].The membrane emulsification gains the advantage on controlling droplet size distribution by membrane pore and is suitable for shear-or temperature-sensitive materials,such as starch and proteins[17].The major limiting factor of this practice is the low dispersed phase flux [17,19].The microchannel emulsification,usually implemented by a tube-in-tube microchannel reactor,has a great potential for the high throughput emulsification of emulsions[18].Nevertheless,the formed emulsions are larger than 10 μm and exhibit a poor controlling of the droplet size.

Hydrodynamic cavitation, a newly developed process intensification technique,has recently demonstrated a great potential for formation of emulsions[20–22].Hydrodynamic cavitation is generated when a moving liquid passes through constriction geometries(e.g.orifice and venture)[23].It has a good prospect in industrial application for its easy scale-up and low energy consumption[24–26].However,emulsions prepared by hydrodynamic cavitation are in the order of hundreds of nanometers rather than sub-100 nmsofar.In this work,we applied hydrodynamic cavitation as an efficient method for the formation of sub-100 nm O/W emulsions with high stability.Re fined soybean oil was used as a typical oil phase to prepare O/Wemulsions.The effects of process parameters(i.e.the inlet pressure,the number of cavitation passes and the surfactant concentration)on the droplet size of emulsions and its stability were investigated in detail.

2.Experimental

Re fined soybean oil(TESCO,Hangzhou,China),heptane and castor oil(Aladdin,Shanghai,China)were tested as oil phase.Deionized water was water phase.Sodium dodecyl sulfate(SDS,Aladdin,Shanghai,China)was selected as stabilizer.

Fig.1.The schematic diagram of the hydrodynamic cavitation emulsification process.

The schematic diagram of the process was shown in Fig.1.The hydrodynamic cavitation was generated by a valve with the diameter of 3 mm.By controlling the valve opening,the inlet pressure could be controlled.In a typical experiment,200 ml of oil was mixed with 2 L of water(1.25 wt%SDS)in a tank.The mixture was pumped into the valve by a pump(120 psi).O/W emulsion was formed after the mixture passed through the valve.

The droplet size distribution and zeta potential of the emulsions were measured using a dynamic light scattering instrument(Zetasizer-nano ZS90,Malvern).Samples were diluted appropriately before the droplet size measurements using deionized water.All samples were analyzed in triplicate. The Z-average diameter was reported as the average droplet size [12,13]. The polydispersity index(PDI),which reflected the quality of distribution of the droplet size in an emulsion,was recorded in the measurement.Zeta potential value is an index of the stability of emulsions.When the absolute value was larger than 30 mV,the system was considered to be stable.

3.Results and Discussion

The hydrodynamic cavitation emulsification process was exemplified using re fined soybean oil as oil phase.In this case,the experiment was carried out at the inlet pressure of 100 psi(1 MPa=145 psi).SDS was dissolved in water at the concentration of 1.25 wt%.As shown in Fig.2,milk like emulsion was formed.The average droplet size of the emulsion was 100 nm,which was much smaller than the reported droplet size(>10 μm)[18],demonstrating a successful hydrodynamic cavitation emulsification.

Fig.2.Droplet size distribution of O/W emulsion formed by hydrodynamic cavitation emulsification(inlet pressure:100 psi;SDS concentration:1.25 wt%;number of cavitation passes:1).Insert is the image of emulsion.

The inlet pressure is one of the most important parameters which affect the cavitating condition inside the cavitating device[25].To investigate the effect of inlet pressure,a series of emulsions were prepared by varying the inlet pressure from 20 to 150 psi.As shown in Fig.3,there was an obvious decrease in droplet size when the inlet pressure increased from 20 psi to 120 psi.Emulsion with an average size of 27 nm was formed at120psi.Zeta potential measurement showed negatively charged emulsion(34.0±0.7 mV),which implies a stable system[27,28].However,a further increase of inlet pressure to 150 psi,shows no Significant decrease in the drop size.It is worthy of noting that the polydispersity indexes of the emulsions were lower than 0.1 when the inlet pressure was larger than 120 psi(Table 1),demonstrating good monodispersity of emulsions.

Fig.3.Effect of inlet pressure on droplet size(SDS concentration:1.25 wt%;number of cavitation passes:6).

Table 1 Droplet size distributions of emulsions prepared under different inlet pressures(SDS concentration:1.25 wt%;number of cavitation passes:6)

The decreasing of droplet size with the increasing inlet pressure can be attributed to the following reasons.Increasing in the inlet pressure results in an reinforcement of the collapse intensity of cavity,due to which the magnitude of pressure pulse generated was enhanced,favoring the mass transfer between the two immiscible phases(i.e.oil and water)[29].Similar effects have been reported by Braeutigam[24]and Ghayal[30].The emulsion size did not change appreciably after 150 psi,possibly due to the elimination of mass transfer resistance under higher operating pressure[29].

Premix quality is an important factor influencing the quality of an emulsion[9].Passing emulsion through the cavitating device for more than one pass can improve the premix.As shown in Fig.4,the droplet size decreased with the increase of cavitation passes.With one cavitation pass,the average emulsion size was about 140 nm.Increasing the cavitation pass to 6,the emulsion size dramatically decreased to 27nm.This would be expected because the increase of cavitation passes allowed the increase of the energy input for emulsification.

Fig.4.Effect of number of cavitation passes on droplet size(inlet pressure:120 psi;SDS concentration:1.25 wt%).

Surfactants influence the emulsion formation,which help to control the emulsion size by reducing the interfacial tension and reducing agglomeration by affecting interfacial mobility[31].SDSwas used as stabilizer in this study,which acts as a protecting colloid during the emulsion formation, resulting in stabilized emulsion droplets. As shown in Fig. 5,there was a decrease in the droplet size with the increase of SDS concentrations.At low concentrations below 0.75 wt%, formation of relatively large oil drops was obtained. Increasing the concentration to 1.25%,the average droplet size decreased to 27 nm. Such results were similar to the results of the previous publication, and the reason could be attributed to the decrease of the interfacial tension and interfacial mobility[18].

Fig.5.Effect of SDS concentration on droplet size(inlet pressure:120 psi;number of cavitation passes:6).

The primary limitation for developing emulsions practical applications is the relatively low stability[6].The stability of emulsions is highly dependent on the structure but also the method used to prepare them[6,16].The droplet size distributions of the emulsions formed by highenergy approaches can remain unchanged over months[14,15].But the major disadvantage is the high energy cost[16].To assess the stability of emulsions prepared by the hydrodynamic cavitation emulsification method,the droplet size was recorded as a function of storage time at room temperature.

As summarized in Fig.6,the average droplet size of the emulsion has not obviously changed over 8 months,exhibiting a very good physical stability.The stability of the emulsion could essentially satisfy the stability requirements in most practical applications. More importantly, the hydrodynamic cavitation emulsification method can be generalized to fabricate a large variety of O/Wemulsions, such as heptane/water emulsion(68 nm), castor oil/water emulsion (19 nm), as shown in Fig. 7.Consequently, hydrodynamic cavitation emulsification is an efficient method for the formation of high-stability O/W emulsions.

Fig.6.Droplet size as a function of time for the emulsion stored at room temperature.

Fig.7.Droplet size distributions of heptane/water emulsion and castor oil/water emulsion.Inserts are the images of the emulsions.

4.Conclusions

In summary,we have demonstrated the hydrodynamic cavitation as an efficient method for the formation of sub-100 nm O/W emulsions with high stability.The effects of inlet cavitation pressure,number of cavitation passes and surfactant concentration on droplet size of the O/W emulsions were investigated.With the increase of inlet pressure,number of cavitation passes and surfactant concentration,the average droplet sizes of the O/W emulsions were decreased.At the inlet pressure of 120 psi,emulsion with the average size of 27 nm was formed after 6 cavitation passes.The formed O/W emulsion exhibited a very good physical stability during 8 months.The hydrodynamic cavitation emulsification has great potential for the formation of emulsions because it offers the benefit of lower energy consumption and easy to scale up.

[1]D.J.Mcclements,Edible nanoemulsions:Fabrication,properties,and functional performance,Soft Matter 7(6)(2011)2297–2316.

[2]C.Qian,D.J.Mcclements,Formation of nanoemulsions stabilized by model foodgrade emulsifiers using high-pressure homogenization:Factors affecting particle size,Food Hydrocolloids 25(5)(2011)1000–1008.

[3]P.Glampedaki,V.Dutschk,Stability studies of cosmetic emulsions prepared from natural products such as wine,grape seed oil and mastic resin,Colloids Surf.A Physicochem.Eng.Asp.460(0)(2014)306–311.

[4]N.Kiss,G.Brenn,H.Pucher,et al.,Formation of O/W emulsions by static mixers for pharmaceutical applications,Chem.Eng.Sci.66(21)(2011)5084–5094.

[5]S.M.T.Gharibzahedi,S.H.Razavi,S.M.Mousavi,Ultrasound-assisted formation of the canthaxanthin emulsions stabilized by arabic and xanthan gums,Carbohydr.Polym.96(1)(2013)21–30.

[6]L.Yu,C.Li,J.Xu,et al.,Highly stable concentrated nanoemulsions by the phase inversion composition method at elevated temperature,Langmuir 28(41)(2012)14547–14552.

[7]C.Solans,P.Izquierdo,J.Nolla,et al.,Nano-emulsions,Curr.Opin.Colloid Interface 10(3–4)(2005)102–110.

[8]A.Khalil,F.Puel,Y.Chevalier,et al.,Study of droplet size distribution during an emulsification process using in situ video probe coupled with an automatic image analysis,Chem.Eng.J.165(3)(2010)946–957.

[9]J.Floury,A.Desrumaux,J.Lardières,Effect of high-pressure homogenization on droplet size distributions and rheological properties of model oil-in-water emulsions,Innovative Food Sci.Emerg.Technol.1(2)(2000)127–134.

[10]S.Lee,T.Lefèvre,M.Subirade,et al.,Effects of ultra-high pressure homogenization on the properties and structure of interfacial protein layer in whey proteinstabilized emulsion,Food Chem.113(1)(2009)191–195.

[11]J.M.Perrier-Cornet,P.Marie,P.Gervais,Comparison of emulsification efficiency of protein-stabilized oil-in-water emulsions using jet,high pressure and colloid mill homogenization,J.Food Eng.66(2)(2005)211–217.

[12]K.A.Ramisetty,A.B.Pandit,P.R.Gogate,Ultrasound assisted preparation of emulsion of coconut oil in water:Understanding the effect of operating parameters and comparison of reactor designs,Chem.Eng.Process.Process Intensif.88(0)(2015)70–77.

[13]S.Y.Tang,P.Shridharan,M.Sivakumar,Impact of process parameters in the generation of novel aspirin nanoemulsions—Comparative studies between ultrasound cavitation and micro fluidizer,Ultrason.Sonochem.20(1)(2013)485–497.

[14]T.J.Wooster,M.Golding,P.Sanguansri,Impact of oil type on nanoemulsion formation and Ostwald ripening stability,Langmuir 24(22)(2008)12758–12765.

[15]J.N.Wilking,C.B.Chang,M.M.Fryd,et al.,Shear-induced disruption of dense nanoemulsion gels,Langmuir 27(9)(2011)5204–5210.

[16]M.M.Fryd,T.G.Mason,Advanced nanoemulsions,Annu.Rev.Phys.Chem.63(2012)493–518.

[17]S.M.Joscelyne,G.Tr?g?rdh,Membrane emulsification — A literature review,J.Membr.Sci.169(1)(2000)107–117.

[18]T.Li,Y.Zhou,J.Wang,et al.,High-throughput emulsification in a microporous tubein-tube microchannel device:O/W emulsion formation,Chem.Eng.J.228(0)(2013)155–161.

[19]D.M.Lloyd,I.T.Norton,F.Spyropoulos,Processing effects during rotating membrane emulsification,J.Membr.Sci.466(0)(2014)8–17.

[20]S.Y.Tang,M.Sivakumar,A novel and facile liquid whistle hydrodynamic cavitation reactor to produce submicron multiple emulsions,AICHE J.59(1)(2013)155–167.

[21]S.Parthasarathy,Y.T.Siah,S.Manickam,Generation and optimization of palm oilbased oil-in-water(O/W)submicron-emulsions and encapsulation of curcumin using a liquid whistle hydrodynamic cavitation reactor(LWHCR),Ind.Eng.Chem.Res.52(34)(2013)11829–11837.

[22]K.A.Ramisetty,A.B.Pandit,P.R.Gogate,Novel approach of producing oil in water emulsion using hydrodynamic cavitation reactor,Ind.Eng.Chem.Res.53(42)(2014)16508–16515.

[23]K.S.Suslick,M.M.Mdleleni,J.T.Ries,Chemistry induced by hydrodynamic cavitation,J.Am.Chem.Soc.119(39)(1997)9303–9304.

[24]K.P.Senthil,K.M.Siva,A.B.Pandit,Experimental quantification of chemical effects of hydrodynamic cavitation,Chem.Eng.Sci.55(9)(2000)1633–1639.

[25]V.K.Saharan,A.B.Pandit,P.S.Satish Kumar,et al.,Hydrodynamic cavitation as an advanced oxidation technique for the degradation of acid red 88 dye,Ind.Eng.Chem.Res.51(4)(2012)1981–1989.

[26]J.S.Raut,S.D.Stoyanov,C.Duggal,et al.,Hydrodynamic cavitation:A bottom-up approach to liquid aeration,Soft Matter 8(17)(2012)4562–4566.

[27]D.Li,M.B.Mueller,S.Gilje,et al.,Processable aqueous dispersions of graphene nanosheets,Nat.Nanotechnol.3(2)(2008)101–105.

[28]D.H.Everett,Basic principles of colloid science[M],Royal Society of Chemistry,1988.

[29]D.Ghayal,A.B.Pandit,V.K.Rathod,Optimization of biodiesel production in a hydrodynamic cavitation reactor using used frying oil,Ultrason.Sonochem.20(1)(2013)322–328.

[30]P.Braeutigam,M.Franke,Z.L.Wu,et al.,Role of different parameters in the optimization of hydrodynamic cavitation,Chem.Eng.Technol.33(6)(2010)932–940.

[31]X.Bernat,E.Piacentini,F.Bazzarelli,et al.,Ferrous ion effects on the stability and properties of oil-in-water emulsions formulated by membrane emulsification,Ind.Eng.Chem.Res.49(8)(2010)3818–3829.

主站蜘蛛池模板: 欧美在线视频不卡| 亚洲天堂日韩在线| 亚洲福利视频网址| 五月婷婷丁香综合| 九九这里只有精品视频| 好紧太爽了视频免费无码| 日韩在线影院| 婷婷色在线视频| 日本不卡在线播放| 国外欧美一区另类中文字幕| 呦视频在线一区二区三区| 国产亚洲男人的天堂在线观看 | 奇米影视狠狠精品7777| 亚洲欧美日韩中文字幕在线一区| 亚洲无码在线午夜电影| 亚洲天堂啪啪| aa级毛片毛片免费观看久| 91尤物国产尤物福利在线| 国产男女免费完整版视频| 青青青亚洲精品国产| 久久国产精品国产自线拍| 国产欧美视频在线| 亚洲码一区二区三区| 九九九九热精品视频| 青青草综合网| 欲色天天综合网| 亚洲人成影视在线观看| 狠狠色综合网| 中文字幕亚洲综久久2021| 国产91视频免费| 美女免费黄网站| 国产91精选在线观看| 国产美女一级毛片| 日韩中文精品亚洲第三区| 欧美性天天| 欧美人与牲动交a欧美精品 | 黄色国产在线| 亚洲精品视频免费| 最近最新中文字幕在线第一页| 一级毛片基地| 天天视频在线91频| 亚洲男人天堂网址| 波多野结衣二区| 亚洲欧洲日本在线| 国产探花在线视频| 五月天久久综合国产一区二区| 欧美激情视频二区| 欧美激情视频在线观看一区| 国产自在线播放| 国产凹凸一区在线观看视频| 午夜精品区| lhav亚洲精品| 日本日韩欧美| 91精品国产一区自在线拍| 日本91在线| 亚洲综合久久成人AV| 色综合中文| 日本尹人综合香蕉在线观看 | 亚洲日本www| 日韩欧美中文亚洲高清在线| 香蕉蕉亚亚洲aav综合| 99久久精品免费看国产电影| 国内a级毛片| 色噜噜在线观看| 色吊丝av中文字幕| 欧美在线一级片| 激情视频综合网| 色噜噜中文网| 72种姿势欧美久久久大黄蕉| 国产在线拍偷自揄观看视频网站| 国产小视频a在线观看| 亚洲综合狠狠| 久久天天躁夜夜躁狠狠| 国产在线91在线电影| 亚洲欧美自拍视频| 囯产av无码片毛片一级| 久久精品这里只有国产中文精品| 亚洲欧洲美色一区二区三区| 午夜精品一区二区蜜桃| 在线观看视频一区二区| 国产午夜无码专区喷水| 萌白酱国产一区二区|